def draw_force_field(x_list, y_list, width, height):
from pprint import pprint
'''docstring for draw_force_field'''
log.info("draw_force_field is working..." )
X = []
Y = []
for row in range(0,height):
one_row_x = []
one_row_y = []
for col in range(0, width):
i = row * width + col
one_row_x.append(x_list[i])
one_row_y.append(y_list[i])
X.append(one_row_x)
Y.append(one_row_y)
#X.insert(0, one_row_x)
#Y.insert(0, one_row_y)
Q = plt.quiver( X, Y)
plt.quiverkey(Q, 0.5, 0.92, 2, r'')
#l,r,b,t = plt.axis()
#dx, dy = r-l, t-b
##axis([l-0.05*dx, r+0.05*dx, b-0.05*dy, t+0.05*dy])
#plt.xticks(range(0,width +3))
#plt.yticks(range(0,height + 3))
plt.title('Attraction Force field')
plt.savefig("pixel.jpg")
plt.show()
return 0
def plot_meancontquiv(turbine="turbine2", save=False):
mean_u = load_vel_map(turbine=turbine, component="u")
mean_v = load_vel_map(turbine=turbine, component="v")
mean_w = load_vel_map(turbine=turbine, component="w")
y_R = np.round(np.asarray(mean_u.columns.values, dtype=float), decimals=4)
z_R = np.asarray(mean_u.index.values, dtype=float)
plt.figure(figsize=(7.5, 4.1))
# Add contours of mean velocity
cs = plt.contourf(y_R, z_R, mean_u / U, 20, cmap=plt.cm.coolwarm)
cb = plt.colorbar(cs, orientation="vertical")
cb.set_label(r"$U/U_{\infty}$")
# Make quiver plot of v and w velocities
Q = plt.quiver(y_R, z_R, mean_v / U, mean_w / U, angles="xy", width=0.0022, edgecolor="none", scale=3.0)
plt.xlabel(r"$y/R$")
plt.ylabel(r"$z/R$")
plt.quiverkey(
Q, 0.65, 0.045, 0.1, r"$0.1 U_\infty$", labelpos="E", coordinates="figure", fontproperties={"size": "small"}
)
ax = plt.axes()
ax.set_aspect(1)
# Plot circle to represent turbine frontal area
circ = plt.Circle((0, 0), radius=1, facecolor="none", edgecolor="gray", linewidth=3.0)
ax.add_patch(circ)
plt.tight_layout()
if save:
plt.savefig("figures/" + turbine + "-meancontquiv.pdf")
def main():
plot_utils.apply_plot_params(width_cm=20, height_cm=20, font_size=10)
high_hles_years = [1993, 1995, 1998]
low_hles_years = [1997, 2001, 2006]
data_path = "/BIG1/skynet1_rech1/diro/sample_obsdata/eraint/eraint_uvslp_years_198111_201102_NDJmean_ts.nc"
with xr.open_dataset(data_path) as ds:
print(ds)
u = get_composit_for_name(ds, "u10", high_years_list=high_hles_years, low_years_list=low_hles_years)
v = get_composit_for_name(ds, "v10", high_years_list=high_hles_years, low_years_list=low_hles_years)
msl = get_composit_for_name(ds, "msl", high_years_list=high_hles_years, low_years_list=low_hles_years)
lons = ds["longitude"].values
lats = ds["latitude"].values
print(lats)
print(msl.shape)
print(lons.shape, lats.shape)
lons2d, lats2d = np.meshgrid(lons, lats)
fig = plt.figure()
map = Basemap(llcrnrlon=-130, llcrnrlat=22, urcrnrlon=-28,
urcrnrlat=65, projection='lcc', lat_1=33, lat_2=45,
lon_0=-95, resolution='i', area_thresh=10000)
clevs = np.arange(-11.5, 12, 1)
cmap = cm.get_cmap("bwr", len(clevs) - 1)
bn = BoundaryNorm(clevs, len(clevs) - 1)
x, y = map(lons2d, lats2d)
im = map.contourf(x, y, msl / 100, levels=clevs, norm=bn, cmap=cmap) # convert to mb (i.e hpa)
map.colorbar(im)
stride = 2
ux, vy = map.rotate_vector(u, v, lons2d, lats2d)
qk = map.quiver(x[::stride, ::stride], y[::stride, ::stride], ux[::stride, ::stride], vy[::stride, ::stride],
scale=10, width=0.01, units="inches")
plt.quiverkey(qk, 0.5, -0.1, 2, "2 m/s", coordinates="axes")
map.drawcoastlines(linewidth=0.5)
map.drawcountries()
map.drawstates()
#plt.show()
fig.savefig("hles_wind_compoosits.png", bbox_inches="tight", dpi=300)
def add_std_vector_to_12months_cycle_figure(plt, fig, CF, parameter): std_length = parameter[0] scale = parameter[1] qkeyx = parameter[2] qkeyy = parameter[3] plt.quiverkey(CF, qkeyx, qkeyy, std_length, str(std_length)) return plt
def PLOT_E(v1,v2,v3,v4,scale,title="",flag_out=0,name_out="output.png",flag_show=0):
if not len(v1) == len (v2):
print("v1 and v2 have different length")
return
if not len(v1) == len (v3):
print("v1 and v3 have different length")
return
if not len(v1) == len (v4):
print("v1 and v4 have different length")
return
E1 = []
E2 = []
for i in range(len(v1)):
E=math.hypot(v3[i],v4[i])
T=math.atan2(v4[i],v3[i])
E1.append( E*math.cos(0.5*T))
E2.append( E*math.sin(0.5*T))
plt.title(title)
A=plt.quiver(v1,v2,E1,E2,scale=(float)(scale),width=0.005,headwidth=0,pivot='middle')
plt.quiverkey(A,0.95,0.95,0.1,"0.1")
plt.axis('scaled')
if flag_out == 1:
plt.savefig(name_out)
if flag_show == 1:
plt.show()
plt.close()
def plot_meancontquiv():
data = calcwake(t1=0.4)
y_R = data["y/R"]
z_R = data["z/R"]
u = data["meanu"]
v = data["meanv"]
w = data["meanw"]
plt.figure(figsize=(7, 9))
# Add contours of mean velocity
cs = plt.contourf(y_R, z_R, u/U, 20, cmap=plt.cm.coolwarm)
cb = plt.colorbar(cs, shrink=1, extend="both",
orientation="horizontal", pad=0.1)
#ticks=np.round(np.linspace(0.44, 1.12, 10), decimals=2))
cb.set_label(r"$U/U_{\infty}$")
# Make quiver plot of v and w velocities
Q = plt.quiver(y_R, z_R, v/U, w/U, angles="xy", width=0.0022,
edgecolor="none", scale=3.0)
plt.xlabel(r"$y/R$")
plt.ylabel(r"$z/R$")
plt.quiverkey(Q, 0.8, 0.21, 0.1, r"$0.1 U_\infty$",
labelpos="E",
coordinates="figure",
fontproperties={"size": "small"})
ax = plt.axes()
ax.set_aspect(1)
# Plot circle to represent turbine frontal area
circ = plt.Circle((0, 0), radius=1, facecolor="none", edgecolor="gray",
linewidth=3.0)
ax.add_patch(circ)
plt.tight_layout()
def whiskerplot(cat,col,fig):
if col == 'psf':
key = r'e_{PSF}'
if col == 'e':
key = r'e'
if col == 'dpsf':
key = r'\Delta e_{PSF}'
scale=0.02
y,x,mw,e1,e2,e=field.field.whisker_calc(cat,col=col)
pos0=0.5*np.arctan2(e2/mw,e1/mw)
e/=mw
for i in range(len(x)):
y[i,:,:],x[i,:,:]=field.field_methods.ccd_to_field(i,y[i,:,:]-2048,x[i,:,:]-1024)
print 'y,x',y[i,:,:],x[i,:,:]
plt.figure(fig)
print np.shape(x),np.shape(y),np.shape(np.sin(pos0)*e),np.shape(np.cos(pos0)*e)
Q = plt.quiver(np.ravel(y),np.ravel(x),np.ravel(np.sin(pos0)*e),np.ravel(np.cos(pos0)*e),units='width',pivot='middle',headwidth=0,width=.0005)
plt.quiverkey(Q,0.2,0.2,scale,str(scale)+' '+key,labelpos='E',coordinates='figure',fontproperties={'weight': 'bold'})
plt.savefig('plots/y1/whisker_'+col+'.pdf', dpi=500, bbox_inches='tight')
plt.close(fig)
return
def plot_grid(EIC_grid,sat_track,sat_krig,title):
'''
This function plots a scatter map of the EICS grid and its horizontal components, and the krigged value for the
satellite.
:param EIC_grid: The EICS grid
:param satPos: The position of the satellite
:param ptz_u: The krigged u component of the satellite
:param ptz_v: The krigged v component of the satllite
:param title: Timestamp of the satellite
:return: The figure
'''
# Define the size of the figure in inches
plt.figure(figsize=(18,18))
# The horizontal components of the Ionospheric current from the EICS grid
u = EIC_grid[:,2]
v = EIC_grid[:,3]
'''
The m variable defines the basemap of area that is going to be displayed.
1) width and height is the area in pixels of the area to be displayed.
2) resolution is the resolution of the boundary dataset being used 'c' for crude and 'l' for low
3) projection is type of projection of the basemape, in this case it is a Lambert Azimuthal Equal Area projection
4) lat_ts is the latitude of true scale,
5) lat_0 and lon_0 is the latitude and longitude of the central point of the basemap
'''
m = Basemap(width=8000000, height=8000000, resolution='l', projection='lcc',\
lat_0=60,lon_0=-100.)
m.drawcoastlines() #draw the coastlines on the basemap
# draw parallels and meridians and label them
m.drawparallels(np.arange(-80.,81.,20.),labels=[1,0,0,0],fontsize=10)
m.drawmeridians(np.arange(-180.,181.,20.),labels=[0,0,0,1],fontsize=10)
# Project the inputted grid into x,y values defined of the projected basemap parameters
x,y =m(EIC_grid[:,1],EIC_grid[:,0])
satx,saty = m(sat_track[::10,7],sat_track[::10,6])
satkrigx,satkrigy = m(sat_krig[1],sat_krig[0])
'''
Plot the inputted grid as a quiver plot on the basemap,
1) x,y are the projected latitude and longitude coordinates of the grid
2) u and v are the horizontal components of the current
3) the EICS grid values are plotted in blue color where as the satellite krigged values are in red
'''
eic = m.quiver(x,y,u,v,width = 0.004, scale=10000,color='#0000FF')
satkrig = m.quiver(satkrigx,satkrigy,sat_krig[2],sat_krig[3],color='#FF0000',width=0.004, scale = 10000)
satpos = m.scatter(satx,saty,s=100,marker='.',c='#009933',edgecolors='none',label='Satellite Track')
sat_halo = m.scatter(satkrigx,satkrigy,s=400,facecolors='none',edgecolors='#66FF66',linewidth='5')
plt.title(title)
plt.legend([satpos],['Satellite Track'],loc='upper right',scatterpoints=1)
plt.quiverkey(satkrig,0.891,0.948,520,u'\u00B1' +'520 mA/m',labelpos='E')
plt.savefig('EICS_20110311_002400.png',bbox_inches='tight',pad_inches=0.2)
def water_quiver1(current_data):
u = water_u1(current_data)
v = water_v1(current_data)
plt.hold(True)
Q = plt.quiver(current_data.x[::2, ::2], current_data.y[::2, ::2], u[::2, ::2], v[::2, ::2])
max_speed = np.max(np.sqrt(u ** 2 + v ** 2))
label = r"%s m/s" % str(np.ceil(0.5 * max_speed))
plt.quiverkey(Q, 0.15, 0.95, 0.5 * max_speed, label, labelpos="W")
plt.hold(False)
def animate(n): # the function of the animation
ax.cla()
plt.title('Drifter: {0} {1}'.format(drifter_ID,point['time'][n].strftime("%F %H:%M")))
draw_basemap(ax, points)
ax.plot(drifter_points['lon'],drifter_points['lat'],'bo-',markersize=6,label='Drifter')
ax.annotate(an2,xy=(dr_points['lon'][-1],dr_points['lat'][-1]),xytext=(dr_points['lon'][-1]+0.01*track_days,
dr_points['lat'][-1]+0.01*track_days),fontsize=6,arrowprops=dict(arrowstyle="fancy"))
ax.plot(model_points['lon'][:n+1],model_points['lat'][:n+1],'ro-',markersize=6,label=MODEL)
#M = np.hypot(U[n], V[n])
Q = ax.quiver(X,Y,U[n],V[n],color='black',pivot='tail',units='xy')
plt.quiverkey(Q, 0.5, 0.92, 1, r'$1 \frac{m}{s}$', labelpos='E',fontproperties={'weight': 'bold','size':18})
def plotResPosArrow2D(ccdSet, iexp, matchVec, sourceVec, outputDir):
import matplotlib.pyplot as plt
_xm = []
_ym = []
_dxm = []
_dym = []
for m in matchVec:
if (m.good == True and m.iexp == iexp):
_xm.append(m.u)
_ym.append(m.v)
_dxm.append((m.xi_fit - m.xi)*3600)
_dym.append((m.eta_fit - m.eta)*3600)
_xs = []
_ys = []
_dxs = []
_dys = []
if (len(sourceVec) != 0):
for s in sourceVec:
if (s.good == True and s.iexp == iexp):
_xs.append(s.u)
_ys.append(s.v)
_dxs.append((s.xi_fit - s.xi)*3600)
_dys.append((s.eta_fit - s.eta)*3600)
xm = numpy.array(_xm)
ym = numpy.array(_ym)
dxm = numpy.array(_dxm)
dym = numpy.array(_dym)
xs = numpy.array(_xs)
ys = numpy.array(_ys)
dxs = numpy.array(_dxs)
dys = numpy.array(_dys)
plt.clf()
plt.rc("text", usetex=USETEX)
plt.rc('xtick', labelsize=10)
plt.rc('ytick', labelsize=10)
plotCcd(ccdSet)
q = plt.quiver(xm, ym, dxm, dym, units="inches", angles="xy", scale=1, color="green", label="external")
if len(xm) != 0 and len(ym) != 0:
xPos = round(xm.min() + (xm.max() - xm.min())*0.002, -2)
yPos = round(ym.max() + (ym.max() - ym.min())*0.025, -2)
plt.quiverkey(q, xPos, yPos, 0.1, "0.1 arcsec", coordinates="data", color="blue", labelcolor="blue",
labelpos='E', fontproperties={'size': 10})
plt.quiver(xs, ys, dxs, dys, units="inches", angles="xy", scale=1, color="red", label="internal")
plt.axes().set_aspect("equal")
plt.legend(fontsize=8)
plt.title("LSST: %d" % (iexp))
plt.savefig(os.path.join(outputDir, "ResPosArrow2D_%d.png" % (iexp)), format="png")
def plot_whisker(x,y,e1,e2,name='',label='',scale=.01,key='',chip=False):
plt.figure()
Q = plt.quiver(x,y,e1,e2,units='width',pivot='middle',headwidth=0,width=.0005)
if chip:
plt.quiverkey(Q,0.2,0.125,scale,str(scale)+' '+key,labelpos='E',coordinates='figure',fontproperties={'weight': 'bold'})
plt.xlim((-250,4250))
plt.ylim((-200,2100))
else:
plt.quiverkey(Q,0.2,0.2,scale,str(scale)+' '+key,labelpos='E',coordinates='figure',fontproperties={'weight': 'bold'})
plt.savefig('plots/footprint/whisker_'+name+'_'+label+'.png', dpi=500,bbox_inches='tight')
plt.close()
return
def plot_flow(binpath, pngpath, title, value):
data = np.fromfile(binpath, dtype=float)
# reading additional info
NX = int(data[0])
NY = int(data[1])
data = data[2:]
# hack
a = NX
NX = NY
NY = a
U = data[0:len(data):2]
V = data[1:len(data):2]
# get max and min vector
UV = np.vstack((U, V))
UV_max = np.amax(UV, axis=1)
UV_min = np.amin(UV, axis=1)
# get sqrt(x^x + y^y)
UV_max = np.square(UV_max)
UV_max = np.sum(UV_max)
UV_max = np.sqrt(UV_max)
UV_min = np.square(UV_min)
UV_min = np.sum(UV_min)
UV_min = np.sqrt(UV_min)
UV_average = (UV_max + UV_min) / 2
U = U.reshape(NX, NY)
V = V.reshape(NX, NY)
# create figure
plt.figure(figsize=(6 * NY / NX, 6))
# title
plt.title(title)
Q = plt.quiver(U, V, color='r', pivot='mid', units='xy')
plt.quiverkey(Q, 0.5, 0.95, UV_average, '{0:.3e} {1}'.format(UV_average, value), labelpos='W')
l,r,b,t = plt.axis()
l,r,b,t = 0.0, NY, 0.0, NX
dx, dy = r-l, t-b
plt.axis([l-0.05*dx, r+0.05*dx, b-0.05*dy, t+0.05*dy])
plt.savefig(pngpath, dpi=150)
plt.close()
return 0
def quick_static(gflist,datapath,run_name,run_num,c):
'''
Make quick quiver plot of static fields
IN:
gflist: Tod ecide which stations to plot
datapath: Where are the data files
'''
import matplotlib.pyplot as plt
from numpy import genfromtxt,where,zeros,meshgrid,linspace
GF=genfromtxt(gflist,usecols=3)
sta=genfromtxt(gflist,usecols=0,dtype='S')
lon=genfromtxt(gflist,usecols=1,dtype='f')
lat=genfromtxt(gflist,usecols=2,dtype='f')
#Read coseismcis
i=where(GF!=0)[0]
lon=lon[i]
lat=lat[i]
n=zeros(len(i))
e=zeros(len(i))
u=zeros(len(i))
#Get data
if run_name!='' or run_num!='':
run_name=run_name+'.'
run_num=run_num+'.'
for k in range(len(i)):
neu=genfromtxt(datapath+run_name+run_num+sta[i[k]]+'.static.neu')
n[k]=neu[0]#/((neu[0]**2+neu[1]**2)**0.5)
e[k]=neu[1]#/((neu[0]**2+neu[1]**2)**0.5)
u[k]=neu[2]#/(2*abs(neu[2]))
#Plot
plt.figure()
xi = linspace(min(lon), max(lon), 500)
yi = linspace(min(lat), max(lat), 500)
X, Y = meshgrid(xi, yi)
#c=Colormap('bwr')
#plt.contourf(X,Y,Z,100)
#plt.colorbar()
Q=plt.quiver(lon,lat,e,n,width=0.001,color=c)
plt.scatter(lon,lat,color='b')
plt.grid()
plt.title(datapath+run_name+run_num)
plt.show()
qscale_en=1
plt.quiverkey(Q,X=0.1,Y=0.9,U=qscale_en,label=str(qscale_en)+'m')
def overdraw_vec_with_axis(plt, datax, datay, xgrid, ygrid, std_length=0.1, scale=1, intvl=3, qkeyx=0.8, qkeyy=0.8, lw = 2):
import matplotlib.pyplot as plt
if datax.shape!=datay.shape:
raise Exception('datax and datay don\'t have same shape!')
if datax.shape[0] != ygrid.size:
raise Exception('data size x does not match ygrid size!')
if datay.shape[1] != xgrid.size:
raise Exception('data size y does not match xgrid size!')
X, Y=np.meshgrid(xgrid, ygrid)
Q=plt.quiver(X[::intvl, ::intvl], Y[::intvl, ::intvl], datax[::intvl, ::intvl], datay[::intvl, ::intvl], angles='xy', scale=scale, lw = lw)
plt.quiverkey(Q, qkeyx, qkeyy, std_length, str(std_length))
return plt
def plotmap(self, domain = [0., 360., -90., 90.], res='c', stepp=2, scale=20):
latitudes = self.windspeed.latitudes.data
longitudes = self.windspeed.longitudes.data
m = bm(projection='cyl',llcrnrlat=latitudes.min(),urcrnrlat=latitudes.max(),\
llcrnrlon=longitudes.min(),urcrnrlon=longitudes.max(),\
lat_ts=0, resolution=res)
lons, lats = np.meshgrid(longitudes, latitudes)
cmap = palettable.colorbrewer.sequential.Oranges_9.mpl_colormap
f, ax = plt.subplots(figsize=(10,6))
m.ax = ax
x, y = m(lons, lats)
im = m.pcolormesh(lons, lats, self.windspeed.data, cmap=cmap)
cb = m.colorbar(im)
cb.set_label('wind speed (m/s)', fontsize=14)
Q = m.quiver(x[::stepp,::stepp], y[::stepp,::stepp], \
self.uanoms.data[::stepp,::stepp], self.vanoms.data[::stepp,::stepp], \
pivot='middle', scale=scale)
l,b,w,h = ax.get_position().bounds
qk = plt.quiverkey(Q, l+w-0.1, b-0.03, 5, "5 m/s", labelpos='E', fontproperties={'size':14}, coordinates='figure')
m.drawcoastlines()
return f
def my_plot(u,v,t,daystr,levels):
#boston light swim
ax= [-71.10, -70.10, 41.70, 42.70] # region to plot
vel_arrow = 0.2 # velocity arrow scale
subsample = 8 # subsampling of velocity vectors
# find velocity points in bounding box
ind = np.argwhere((lonc >= ax[0]) & (lonc <= ax[1]) & (latc >= ax[2]) & (latc <= ax[3]))
np.random.shuffle(ind)
Nvec = int(len(ind) / subsample)
idv = ind[:Nvec]
# tricontourf plot of water depth with vectors on top
plt.figure(figsize=(20,10))
plt.subplot(111,aspect=(1.0/np.cos(lat[:].mean()*np.pi/180.0)))
#tricontourf(tri, t,levels=levels,shading='faceted',cmap=plt.cm.gist_earth)
plt.tricontourf(tri, t,levels=levels,shading='faceted')
plt.axis(ax)
plt.gca().patch.set_facecolor('0.5')
cbar=plt.colorbar()
cbar.set_label('Forecast Surface Temperature (C)', rotation=-90)
plt.tricontour(tri, t,levels=[0])
Q = plt.quiver(lonc[idv],latc[idv],u[idv],v[idv],scale=10)
maxstr='%3.1f m/s' % vel_arrow
qk = plt.quiverkey(Q,0.92,0.08,vel_arrow,maxstr,labelpos='W')
plt.title('NECOFS Surface Velocity, Layer %d, %s UTC' % (ilayer, daystr))
plt.plot(lon_track,lat_track,'m-o')
plt.plot(lon_buoy,lat_buoy,'y-o')
def velocidadlimpio(self):
#sino no llega al 2, asi funciona
v = np.arange(-3, 3,1)
[x,y] = np.meshgrid(v,v)
z=np.multiply(x,np.exp( -np.power(x,2) - np.power(y,2) ))
#Matplotlib t invierte el orden de las matrices a diferenciade matlab
[py,px] = np.gradient(z,1,1)
print 'x '+str(x)
print 'y '+str(y)
print 'z '+str(z)
print 'px '+str(px)
print 'py '+str(py)
#q = plt.quiver(X, Y, u, v, angles='xy', scale=40, color=['r'])
#p = plt.quiverkey(q,1,16.5,50,"50 m/s",coordinates='data',color='r')
#primero los rangos, despues los valores q contiene
q = plt.quiver(x,y, px, py)
p = plt.quiverkey(q,1,16.5,50,"50 m/s",coordinates='data',color='r')
plt.title('Velocidad')
plt.show()
print 'Fourth plot loaded...'
def plot_meancontquiv(t1_fraction=0.5, cb_orientation="vertical", save=False):
"""Plot contours of normalized mean streamwise velocity and vectors of
cross-stream and vertical mean velocity.
"""
data = load_probe_data(t1_fraction=t1_fraction)
y_R = data["y_R"]
z_H = data["z_H"]
mean_u = data["mean_u"]
mean_v = data["mean_v"]
mean_w = data["mean_w"]
scale = 7.5/10.0
plt.figure(figsize=(10*scale, 3*scale))
# Add contours of mean velocity
cs = plt.contourf(y_R, z_H, mean_u, 20, cmap=plt.cm.coolwarm)
if cb_orientation == "horizontal":
cb = plt.colorbar(cs, shrink=1, extend="both",
orientation="horizontal", pad=0.14)
elif cb_orientation == "vertical":
cb = plt.colorbar(cs, shrink=0.88, extend="both",
orientation="vertical", pad=0.02)
cb.set_label(r"$U/U_{\infty}$")
# Make quiver plot of v and w velocities
Q = plt.quiver(y_R, z_H, mean_v, mean_w, width=0.0022,
edgecolor="none", scale=3)
plt.xlabel(r"$y/R$")
plt.ylabel(r"$z/H$")
plt.ylim(-0.15, 0.85)
plt.xlim(-1.68/R, 1.68/R)
if cb_orientation == "horizontal":
plt.quiverkey(Q, 0.65, 0.26, 0.1, r"$0.1 U_\infty$",
labelpos="E",
coordinates="figure",
fontproperties={"size": "small"})
elif cb_orientation == "vertical":
plt.quiverkey(Q, 0.65, 0.09, 0.1, r"$0.1 U_\infty$",
labelpos="E",
coordinates="figure",
fontproperties={"size": "small"})
plot_turb_lines()
ax = plt.axes()
ax.set_aspect(H/R)
plt.yticks([0, 0.13, 0.25, 0.38, 0.5, 0.63, 0.75])
plt.grid(True)
plt.tight_layout()
if save:
plt.savefig("figures/meancontquiv.pdf")
plt.savefig("figures/meancontquiv.png", dpi=300)
def plot_meancontquiv(save=False, show=False, savetype=".pdf",
cb_orientation="vertical"):
"""Plot mean contours/quivers of velocity."""
mean_u = load_vel_map("u")
mean_v = load_vel_map("v")
mean_w = load_vel_map("w")
y_R = np.round(np.asarray(mean_u.columns.values, dtype=float), decimals=4)
z_H = np.asarray(mean_u.index.values, dtype=float)
plt.figure(figsize=(7.5, 4.8))
# Add contours of mean velocity
cs = plt.contourf(y_R, z_H, mean_u,
np.arange(0.15, 1.25, 0.05), cmap=plt.cm.coolwarm)
if cb_orientation == "horizontal":
cb = plt.colorbar(cs, shrink=1, extend="both",
orientation="horizontal", pad=0.14)
elif cb_orientation == "vertical":
cb = plt.colorbar(cs, shrink=1, extend="both",
orientation="vertical", pad=0.02)
cb.set_label(r"$U/U_{\infty}$")
plt.hold(True)
# Make quiver plot of v and w velocities
Q = plt.quiver(y_R, z_H, mean_v, mean_w, width=0.0022,
edgecolor="none", scale=3.0)
plt.xlabel(r"$y/R$")
plt.ylabel(r"$z/H$")
# plt.ylim(-0.2, 0.78)
# plt.xlim(-3.2, 3.2)
if cb_orientation == "horizontal":
plt.quiverkey(Q, 0.65, 0.26, 0.1, r"$0.1 U_\infty$",
labelpos="E",
coordinates="figure",
fontproperties={"size": "small"})
elif cb_orientation == "vertical":
plt.quiverkey(Q, 0.65, 0.055, 0.1, r"$0.1 U_\infty$",
labelpos="E",
coordinates="figure",
fontproperties={"size": "small"})
plot_turb_lines()
plot_exp_lines()
ax = plt.axes()
ax.set_aspect(2.0)
plt.yticks(np.around(np.arange(-1.125, 1.126, 0.125), decimals=2))
plt.tight_layout()
if show:
plt.show()
if save:
plt.savefig("figures/meancontquiv"+savetype)
def Vector(plt, X, Y, data, parameter, label_flg = 0): # std_length,scaleの目安として、 # 流速の場合、1, 10.0 # 風応力の場合、0.1, 1.0 std_length = parameter[0] scale = parameter[1] intvl = parameter[2] qkeyx = parameter[3] qkeyy = parameter[4] data[np.where(abs(data)==np.inf)]=np.nan datax = data[0, :, :] datay = data[1, :, :] Q=plt.quiver(X[::intvl,::intvl],Y[::intvl,::intvl],datax[::intvl,::intvl],datay[::intvl,::intvl],angles='xy',scale=scale) if label_flg == 0: plt.quiverkey(Q, qkeyx, qkeyy, std_length, str(std_length)) return plt, Q
def DrawUV(self, m, micapsfile, clipborder, patch):
if m is plt:
if self.stream:
plot = m.streamplot(self.X, self.Y, self.U, self.V,
density=self.density,
linewidth=self.linewidth,
color=self.color,
cmap=self.cmap
)
if self.barbs:
barbs = m.barbs(self.X, self.Y, self.U, self.V,
length=self.length, barb_increments=dict(half=2, full=4, flag=20),
sizes=dict(emptybarb=0))
pass
else:
# transform vectors to projection grid.
uproj, vproj, xx, yy = \
m.transform_vector(self.U, self.V, self.x, self.y, self.barbsgrid[0], self.barbsgrid[1],
returnxy=True, masked=True)
if isinstance(self.color, np.ndarray):
self.color = self.colorlist
if self.stream:
# plot = m.streamplot(xx, yy, uproj, vproj # , latlon=True
# # density=self.density,
# # linewidth=self.linewidth,
# # color=self.color
# # cmap=self.cmap
# )
# now plot.
Q = m.quiver(xx, yy, uproj, vproj, color=self.color, scale=self.scale)
# make quiver key.
speed = micapsfile.uv.markscalelength
qk = plt.quiverkey(Q, 0.1, 0.1, speed, '%.0f m/s' % speed, labelpos='W')
if self.barbs:
barbs = m.barbs(xx, yy, uproj, vproj, length=self.length,
barb_increments=dict(half=2, full=4, flag=20),
sizes=dict(emptybarb=0),
barbcolor='k', flagcolor='r',
linewidth=0.5)
if clipborder.path is not None and clipborder.using:
from matplotlib.patches import FancyArrowPatch
from matplotlib.collections import PolyCollection
from matplotlib.lines import Line2D
for artist in plt.gca().get_children():
if self.wholeclip:
# from matplotlib.patches import Polygon
if not isinstance(artist, Line2D):
artist.set_clip_path(patch)
else:
from matplotlib.collections import LineCollection
if isinstance(artist, FancyArrowPatch) or isinstance(artist, PolyCollection) or \
isinstance(artist, LineCollection):
artist.set_clip_path(patch)
def _show_currentloop_field():
'''http://www.netdenizen.com/emagnettest/offaxis/?offaxisloop
'''
from numpy import sqrt
r = numpy.linspace(0.0, 3.0, 51)
z = numpy.linspace(-1.0, 1.0, 51)
R, Z = numpy.meshgrid(r, z)
a = 1.0
V = 230 * sqrt(2.0)
rho = 1.535356e-08
II = V/rho
mu0 = pi * 4e-7
alpha = R / a
beta = Z / a
gamma = Z / R
Q = (1+alpha)**2 + beta**2
k = sqrt(4*alpha / Q)
from scipy.special import ellipk
from scipy.special import ellipe
Kk = ellipk(k**2)
Ek = ellipe(k**2)
B0 = mu0*II / (2*a)
V = B0 / (pi*sqrt(Q)) \
* (Ek * (1.0 - alpha**2 - beta**2)/(Q - 4*alpha) + Kk)
U = B0 * gamma / (pi*sqrt(Q)) \
* (Ek * (1.0 + alpha**2 + beta**2)/(Q - 4*alpha) - Kk)
Q = plt.quiver(R, Z, U, V)
plt.quiverkey(
Q, 0.7, 0.92, 1e4, '$1e4$',
labelpos='W',
fontproperties={'weight': 'bold'},
color='r'
)
plt.show()
return
def quiver_3d(x,y,vx,vy,vz, ax=None, sep=1):
import matplotlib.pyplot as plt
if ax==None:
ax = plt.figure().add_subplot(111)
Q = ax.quiver(vy[::sep,::sep], vx[::sep,::sep], \
vz[::sep,::sep], pivot='mid')
qk = plt.quiverkey(Q, 0.9, 0.95, 5, r'$5 \frac{m}{s}$',
labelpos='E',
coordinates='figure',
fontproperties={'weight': 'bold'})
return ax
def plotVectorField(X,Y):
plt.figure()
Q = plt.quiver(X,Y)
qk = plt.quiverkey(Q, 0.5, 0.92, 2, r'$2 \frac{m}{s}$', labelpos='W',
fontproperties={'weight': 'bold'})
l,r,b,t = plt.axis()
dx, dy = r-l, t-b
plt.axis([l-0.05*dx, r+0.05*dx, b-0.05*dy, t+0.05*dy])
plt.title('Minimal arguments, no kwargs')
plt.show()
def add_quiver(self, vname, t, k, cff, step, scale):
"""
ベクトルの ax を返す関数
2015-11-08 作成
"""
X, Y = self.get_xy('quiver', step)
if 'u_eastward' in self.nc.variables.keys():
u = self.nc.variables['u_eastward'][t,k-1,::step,::step]
v = self.nc.variables['v_northward'][t,k-1,::step,::step]
else:
u = self.nc.variables['u'][t,k-1,::step,::step]
v = self.nc.variables['v'][t,k-1,::step,::step]
ax = plt.gca()
print X.shape, Y.shape, u.shape, v.shape
if 'u_eastward' in self.nc.variables.keys():
Q = ax.quiver(X, Y, u, v, units='width', angles='xy', scale=scale)
else:
Q = ax.quiver(X[:-1,:], Y[:-1,:], u[:-1,:], v, units='width', angles='xy', scale=scale)
plt.quiverkey(Q, 0.9, 0.1, 1.0/scale, '1 m/s')
return Q
def plot_meancontquiv():
data = calcwake(t1=3.0)
y_R = data["y/R"]
z_H = data["z/H"]
u = data["meanu"]
v = data["meanv"]
w = data["meanw"]
xvorticity = data["xvorticity"]
plt.figure(figsize=(7, 6.8))
# Add contours of mean velocity
cs = plt.contourf(y_R, z_H, u, 20, cmap=plt.cm.coolwarm)
cb = plt.colorbar(cs, shrink=1, extend='both',
orientation='horizontal', pad=0.12)
#ticks=np.round(np.linspace(0.44, 1.12, 10), decimals=2))
cb.set_label(r'$U/U_{\infty}$')
plt.hold(True)
# Make quiver plot of v and w velocities
Q = plt.quiver(y_R, z_H, v, w, angles='xy', width=0.0022,
edgecolor="none", scale=3.0)
plt.xlabel(r'$y/R$')
plt.ylabel(r'$z/H$')
#plt.ylim(-0.2, 0.78)
#plt.xlim(-3.2, 3.2)
plt.xlim(-3.66, 3.66)
plt.ylim(-1.22, 1.22)
plt.quiverkey(Q, 0.8, 0.22, 0.1, r'$0.1 U_\infty$',
labelpos='E',
coordinates='figure',
fontproperties={'size': 'small'})
plt.hlines(0.5, -1, 1, linestyles='solid', colors='gray',
linewidth=3)
plt.hlines(-0.5, -1, 1, linestyles='solid', colors='gray',
linewidth=3)
plt.vlines(-1, -0.5, 0.5, linestyles='solid', colors='gray',
linewidth=3)
plt.vlines(1, -0.5, 0.5, linestyles='solid', colors='gray',
linewidth=3)
ax = plt.axes()
ax.set_aspect(2.0)
def reload_and_postprocess(int_u = None):
# Creates a pretty picture =)
if int_u is None:
f = open('data/disk_compression/int_u_disk.pkl', 'rb')
int_u = cPickle.load(f)
x_pts = 20
y_pts = 22
x = np.linspace(-0.95, 0.95, x_pts)
y = np.linspace(-0.95, 0.95, y_pts)
X, Y = np.meshgrid(x, y)
fig = plt.figure()
ax = fig.add_subplot(1, 1, 1)
quiver_plot = plt.quiver(X, Y, int_u[0, :, :], int_u[1, :, :])
plt.quiverkey(quiver_plot, 0.60, 0.95, 0.05, r'0.05', labelpos='W')
plt.xlabel('X')
plt.ylabel('Y')
plt.ylim([-1.1, 1.2])
plt.xlim([-1.1, 1.1])
circ = plt.Circle((0, 0), radius = 1.0, color = 'g', fill = False)
ax.add_patch(circ)
plt.title(r'Displacement vectors for a disk compressed in plane strain')
plt.show()
def single_ax(ax, title, df):
states = df.index
num_sts = len(states)
y = np.linspace(0, num_sts-1, num_sts)
if case == 'vec':
assert len(df.columns) == 1
x = [0]
x_num_sts = 1
else:
assert len(df.columns) == num_sts
x = y
x_num_sts = num_sts
xx, yy = np.meshgrid(x, y)
# print(xx)
# print(yy)
ax.set_xlim(-1, x_num_sts)
ax.set_xticks(np.arange(0, x_num_sts))
ax.xaxis.tick_top()
ax.set_ylim(-1, num_sts)
ax.set_yticks(np.arange(0, num_sts))
ax.invert_yaxis()
ax.set_aspect('equal', adjustable='box')
ax.set_title(title, y=1.2)
for st, nom in enumerate(states):
ax.annotate(nom, xy=(x_num_sts+.25, st),
annotation_clip=False)
max_mag = np.max(np.absolute(df.values))
q = ax.quiver(xx, yy, df.values.real,
df.values.imag, scale=max_mag, units='x')
plt.quiverkey(q, 0, -2, max_mag,
'= {:.2e}'.format(max_mag), labelpos='E', coordinates='data')
def PlotCurrentField(self,t,**kwargs):
''' PlotNewRiskmapFig - Produces a pretty picture from the RiskMapArray which is
useful for providing a context within which to plot simulation results. Requires
'matplotlib<http://matplotlib.sourceforge.net>' pyplot functionality
Args: t
* t (int) : time index for the current data file that was loaded last.
'''
if kwargs.has_key('max_depth'):
max_depth = kwargs['max_depth']
else:
max_depth = self.MaxDepth
if kwargs.has_key('min_depth'):
min_depth = kwargs['min_depth']
else:
min_depth = self.MinDepth
if kwargs.has_key('arrow_color'):
arrow_color = kwargs['arrow_color']
else:
arrow_color = 'k'
d0,d1 = FindLowAndHighIndices(min_depth,self.depth)
d1,d2 = FindLowAndHighIndices(max_depth,self.depth)
print 'Averaging depths between indices %d and %d.'%(d0,d2)
import matplotlib.pyplot as plt
mapResX, mapResY = 20, 20
width,height = self.Width, self.Height
#import pdb; pdb.set_trace()
u2,v2 = self.u[:,d0:d2,:,:],self.v[:,d0:d2,:,:]
u2ma,v2ma = np.ma.masked_array(u2,np.isnan(u2)),np.ma.masked_array(v2,np.isnan(v2))
u_mean, v_mean = u2ma.mean(axis=1).filled(np.nan),v2ma.mean(axis=1).filled(np.nan)
#u_mean, v_mean = self.u.mean(axis=1),self.v.mean(axis=1)
X,Y = np.linspace(0, width-0.5, mapResX), np.linspace(0, height-0.5, mapResY)
aX,aY = np.meshgrid(X,Y)
U,V = np.zeros((mapResX,mapResY)),np.zeros((mapResX,mapResY))
for j in range(0,mapResY):
for i in range(0,mapResX):
myLat,myLon = self.GetLatLonfromXY(X[i],Y[j])
if self.GetRisk(myLat, myLon, False )<0.9:
U[j,i], V[j,i] = BilinearInterpolate(myLat,myLon,self.lat,self.lon,u_mean[int(t)]), \
BilinearInterpolate(myLat,myLon,self.lat,self.lon,v_mean[int(t)])
q = plt.quiver(aX,aY,U,V,scale=self.gVel*10,color=arrow_color)
p = plt.quiverkey(q,1,height-0.5,self.gVel,"%.3f m/s"%(self.gVel),coordinates='data',color='k')
def plot_image(self,
wavelength0,
overplot=False,
inclination=None,
cmap=None,
ax=None,
axes_units='AU',
polarization=False,
polfrac=False,
psf_fwhm=None,
vmin=None,
vmax=None,
dynamic_range=1e6,
colorbar=False):
""" Show one image from an MCFOST model
Parameters
----------
wavelength : string
note this is a string!! in microns. TBD make it take strings or floats
inclination : float
Which inclination to plot, in the case where there are multiple images?
If not specified, defaults to the median inclination of whichever RT mode
inclinations were computed.
overplot : bool
Should we overplot on current axes (True) or display a new figure? Default is False
cmap : matplotlib Colormap instance
Color map to use for display.
ax : matplotlib Axes instance
Axis to display into.
vmin, vmax : scalars
Min and max values for image display. Always shows in log stretch
dynamic_range : float
default vmin is vmax/dynamic range. Default dynamic range is 1e6.
axes_units : str
Units to label the axes in. May be 'AU', 'arcsec', 'deg', or 'pixels'
psf_fwhm : float or None
convolve with PSF of this FWHM? Default is None for no convolution
colorbar : bool
Also draw a colorbar
To Do:
* Add convolution with PSFs
* Add coronagraphic occulters
"""
wavelength = self._standardize_wavelength(wavelength0)
if inclination is None:
inclination = self.parameters.inclinations[len(
self.parameters.inclinations) / 2]
if not overplot:
if ax is None: plt.clf()
else: plt.cla()
if ax is None: ax = plt.gca()
# Read in the data and select the image of
imHDU = self.images[wavelength]
inclin_index = utils.find_closest(self.parameters.inclinations,
inclination)
image = imHDU.data[0, 0, inclin_index, :, :]
# Set up color mapping
if cmap is None:
from copy import deepcopy
#cmap = plt.cm.gist_heat
cmap = deepcopy(plt.cm.gist_gray)
cmap.set_over('white')
cmap.set_under('black')
cmap.set_bad('black')
if vmax is None: vmax = image.max()
if vmin is None: vmin = vmax / dynamic_range
norm = matplotlib.colors.LogNorm(vmin=vmin, vmax=vmax, clip=True)
# calculate the display extent of the image
# check if the image header has CDELT keywords, if so use those in preference to
# the plate scale specified in the parameter file.
# This will gracefully handle the case of the user overriding the default pixel
# scale on the command line to MCFOST.
cd1 = imHDU.header['CDELT1']
cd2 = imHDU.header['CDELT2']
pixelscale = np.asarray([cd1, cd2]) # in degrees
if axes_units.lower() == 'deg':
pass
elif axes_units.lower() == 'arcsec':
pixelscale *= 3600
elif axes_units.lower() == 'au':
pixelscale *= 3600 * self.parameters.distance
elif axes_units.lower() == 'pixels' or axes_units.lower() == 'pixel':
pixelscale = np.ones(2)
else:
raise ValueError("Unknown unit for axes_units: " + axes_units)
halfsize = (np.asarray(image.shape)) / 2 * pixelscale
extent = [-halfsize[0], halfsize[0], -halfsize[1], halfsize[1]]
# Optional: convolve with PSF
if psf_fwhm is not None:
raise NotImplementedError("This code not yet implemented")
import optics
#psf = optics.airy_2d(aperture=10.0, wavelength=1.6e-6, pixelscale=0.020, shape=(99,99))
psf = pyfits.getdata(
'/Users/mperrin/Dropbox/AAS2013/models_pds144n/manual/keck_psf_tmp4.fits'
)
from astropy.nddata import convolve
convolved = convolve(image, psf, normalize_kernel=True)
image = convolved
if polfrac:
ax = plt.subplot(121)
# Display the image!
ax = utils.imshow_with_mouseover(ax,
image,
norm=norm,
cmap=cmap,
extent=extent,
origin='lower')
ax.set_xlabel("Offset [{unit}]".format(unit=axes_units))
ax.set_ylabel("Offset [{unit}]".format(unit=axes_units))
ax.set_title("Image for " + wavelength + " $\mu$m")
if polarization == True:
# overplot polarization vectors
# don't show every pixel's vectors:
showevery = 5
imQ = imHDU.data[
1, 0,
inclin_index, :, :] * -1 #MCFOST sign convention requires flip for +Q = up
imU = imHDU.data[
2, 0, inclin_index, :, :] * -1 #MCFOST sign convention, ditto
imQn = imQ / image
imUn = imU / image
polfrac_ar = np.sqrt(imQn**2 + imUn**2)
theta = 0.5 * np.arctan2(imUn, imQn) + np.pi / 2
vecX = polfrac_ar * np.cos(theta) * -1
vecY = polfrac_ar * np.sin(theta)
Y, X = np.indices(image.shape)
Q = plt.quiver(X[::showevery, ::showevery],
Y[::showevery, ::showevery],
vecX[::showevery, ::showevery],
vecY[::showevery, ::showevery],
headwidth=0,
headlength=0,
headaxislength=0.0,
pivot='middle',
color='white')
plt.quiverkey(Q,
0.85,
0.95,
0.5,
"50% pol.",
coordinates='axes',
labelcolor='white',
labelpos='E',
fontproperties={'size': 'small'}) #, width=0.003)
# ax = plt.subplot(152)
# ax.imshow(imQn, vmin=-1, vmax=1, cmap=matplotlib.cm.RdBu)
# ax.set_title('Q')
# ax = plt.subplot(153)
# ax.imshow(imUn, vmin=-1, vmax=1, cmap=matplotlib.cm.RdBu)
# ax.set_title('U')
# ax = plt.subplot(154)
# ax.imshow(vecX, vmin=-1, vmax=1, cmap=matplotlib.cm.RdBu)
# ax.set_title('vecX')
# ax = plt.subplot(155)
# ax.imshow(vecY, vmin=-1, vmax=1, cmap=matplotlib.cm.RdBu)
# ax.set_title('vecY')
# ax.colorbar()
#plt.colorbar()
if polfrac:
# Display a 2nd panel showing the polarization fraction
ax2 = plt.subplot(122)
cmap2 = plt.cm.gist_heat
cmap2 = plt.cm.jet
cmap2.set_over('red')
cmap2.set_under('black')
cmap2.set_bad('black')
ax2 = utils.imshow_with_mouseover(ax2,
polfrac_ar,
vmin=0,
vmax=1,
cmap=cmap2)
ax2.set_title("Polarization fraction")
cax = plt.axes([0.92, 0.25, 0.02, 0.5])
plt.colorbar(ax2.images[0], cax=cax, orientation='vertical')
if colorbar == True:
cb = plt.colorbar(mappable=ax.images[0])
cb.set_label("Intensity [$W/m^2/pixel$]")
pivot='mid',
color='blue',
#cmap = plt.cm.seismic
)
# Main tweaks
# Radius limits
ax1.set_ylim(0, 4)
# Radius Ticks
ax1.set_yticks(np.linspace(0, 4, 5))
# Radius tick position in degrees
ax1.set_rlabel_position(135)
# Angle ticks
ax1.set_xticks(np.linspace(0, 2.0 * np.pi, 17)[:-1])
# Additional tweaks
plt.grid(True)
plt.quiverkey(Quiver,
1.01,
1.01,
3,
label='3 m/s',
labelcolor='blue',
labelpos='N',
coordinates='axes')
# plt.colorbar(Quiver)
# plt.legend() - no label option, hence no legend
plt.title('Polar Quiver Plots')
plt.show()
def plot2dxy_vector(ufilename, vfilename, ttest=True, lvl=850):
f, ax = plt.subplots(1, figsize=(16, 10))
#llon = 130; rlon = 230; blat = -25; tlat = 25
llon = 130
rlon = 230
blat = -55
tlat = 30
#draw map
m = Basemap(ax=ax,
llcrnrlon=85 + (llon - 180),
llcrnrlat=18.5 + blat,
urcrnrlon=85 + (rlon - 180),
urcrnrlat=18.5 + tlat,
resolution='c',
projection='merc',
lat_0=18.5,
lon_0=85)
m.drawcoastlines()
parallels = np.arange(-90, 90, 15.)
m.drawparallels(parallels, labels=[1, 0, 0, 0])
meridians = np.arange(0., 360., 15.)
m.drawmeridians(meridians, labels=[0, 0, 0, 1])
#quiver on top
if ttest:
u_da_raw = xr.open_dataarray(ufilename + '.nc')
v_da_raw = xr.open_dataarray(vfilename + '.nc')
u_da_sig = xr.open_dataarray(ufilename + '_ttest.nc')
v_da_sig = xr.open_dataarray(vfilename + '_ttest.nc')
Uraw = u_da_raw.values
Vraw = v_da_raw.values
Usig = u_da_sig.values
Vsig = v_da_sig.values
Usig[np.where(Vsig != 0.0)] = Uraw[np.where(Vsig != 0.0)]
Vsig[np.where(Usig != 0.0)] = Vraw[np.where(Usig != 0.0)]
u_da = u_da_raw
v_da = v_da_raw
u_da.values = Usig
v_da.values = Vsig
else:
u_da = xr.open_dataarray(ufilename + '.nc')
v_da = xr.open_dataarray(vfilename + '.nc')
u_comp = u_da.sel({
'lv_ISBL0': lvl
}, method='nearest').sel({
'g4_lat_1': slice(tlat, blat),
'g4_lon_2': slice(llon, rlon)
})
v_comp = v_da.sel({
'lv_ISBL0': lvl
}, method='nearest').sel({
'g4_lat_1': slice(tlat, blat),
'g4_lon_2': slice(llon, rlon)
})
x = u_comp.coords['g4_lon_2'].values - 180 + 85
y = u_comp.coords['g4_lat_1'].values + 18.5
x, dummy = m(x, x)
dummy, y = m(y, y)
U = u_comp.values
V = v_comp.values
#Q = m.quiver(x, y, U, V)
Q = m.quiver(x[::3],
y[::3],
U[::3, ::3],
V[::3, ::3],
pivot='mid',
units='inches',
scale=75,
scale_units='width',
headwidth=5,
headlength=2,
headaxislength=5)
qk = plt.quiverkey(Q,
0.9,
0.9,
2,
'2 m/s',
labelpos='E',
coordinates='figure')
#bounding box and center
x, y = m([75, 95, 95, 75, 75], [10, 10, 27, 27, 10])
m.plot(x, y, 'r-', lw=2.5)
x, y = m([85], [18.5])
m.plot(x, y, 'ro', ms=5)
if ttest:
ax.set_title('{}: {} mb, ttest'.format(ufilename, lvl))
else:
ax.set_title('{}: {} mb'.format(ufilename, lvl))
plt.tight_layout(pad=4)
def plot(self,
timedata=None,
udata=None,
vdata=None,
ylabel=None,
**kwargs):
if kwargs['rotate'] != 0.0:
print "rotating vectors"
angle_offset_rad = np.deg2rad(kwargs['rotate'])
udata = udata * np.cos(angle_offset_rad) + vdata * np.sin(
angle_offset_rad)
vdata = -1 * udata * np.sin(angle_offset_rad) + vdata * np.cos(
angle_offset_rad)
magnitude = np.sqrt(udata**2 + vdata**2)
fig = plt.figure(1)
ax2 = plt.subplot2grid((2, 1), (0, 0), colspan=1, rowspan=1)
ax1 = plt.subplot2grid((2, 1), (1, 0), colspan=1, rowspan=1)
# Plot u and v components
# Plot quiver
ax1.set_ylim(-1 * np.nanmax(magnitude), np.nanmax(magnitude))
fill1 = ax1.fill_between(timedata, magnitude, 0, color='k', alpha=0.1)
# Fake 'box' to be able to insert a legend for 'Magnitude'
p = ax1.add_patch(plt.Rectangle((1, 1), 1, 1, fc='k', alpha=0.1))
leg1 = ax1.legend([p], ["Current magnitude [cm/s]"], loc='lower right')
leg1._drawFrame = False
# 1D Quiver plot
q = ax1.quiver(timedata,
0,
udata,
vdata,
color='r',
units='y',
scale_units='y',
scale=1,
headlength=1,
headaxislength=1,
width=0.04,
alpha=.95)
qk = plt.quiverkey(q,
0.2,
0.05,
25,
r'$25 \frac{cm}{s}$',
labelpos='W',
fontproperties={'weight': 'bold'})
# Plot u and v components
ax1.set_xticklabels(ax1.get_xticklabels(), visible=True)
ax2.set_xticklabels(ax2.get_xticklabels(), visible=True)
ax1.axes.get_xaxis().set_visible(True)
ax1.set_xlim(timedata.min() - 0.5, timedata.max() + 0.5)
ax1.set_ylabel("Velocity (cm/s)")
ax2.plot(kwargs['timedata2'],
kwargs['data2'][:, 0, 0, 0],
'k-',
linewidth=1)
ax2.set_xlim(timedata.min() - 0.5, timedata.max() + 0.5)
ax2.set_xlabel("Date (UTC)")
ax2.set_ylabel("Salinity (PSU)")
ax2.xaxis.set_major_locator(MonthLocator())
ax2.xaxis.set_minor_locator(
MonthLocator(bymonth=range(1, 13), bymonthday=15))
ax2.xaxis.set_major_formatter(ticker.NullFormatter())
ax2.xaxis.set_minor_formatter(ticker.NullFormatter())
ax1.xaxis.set_major_locator(MonthLocator())
ax1.xaxis.set_minor_locator(
MonthLocator(bymonth=range(1, 13), bymonthday=15))
ax1.xaxis.set_major_formatter(ticker.NullFormatter())
ax1.xaxis.set_minor_formatter(DateFormatter('%b %y'))
ax2.spines['bottom'].set_visible(False)
ax1.spines['top'].set_visible(False)
ax1.xaxis.set_ticks_position('top')
ax2.xaxis.set_ticks_position('bottom')
ax2.yaxis.set_ticks_position('both')
ax1.tick_params(axis='both', which='minor', labelsize=self.labelsize)
ax2.tick_params(axis='both', which='minor', labelsize=self.labelsize)
return plt, fig
var, lons_cyclic = addcyclic(var, lons)
var, lons_cyclic = shiftgrid(180., var, lons_cyclic, start=False)
u, lons_cyclic = addcyclic(u, lons)
u, lons_cyclic = shiftgrid(180., u, lons_cyclic, start=False)
v, lons_cyclic = addcyclic(v, lons)
v, lons_cyclic = shiftgrid(180., v, lons_cyclic, start=False)
lon2d, lat2d = np.meshgrid(lons_cyclic, lats)
x, y = m(lon2d, lat2d)
cs = m.contourf(x, y, var[:, :], values, extend='both')
#cs1 = m.contour(x,y,var[:,:],
# values,linewidths=0.2,colors='k',
# linestyles='-')
cs2 = m.quiver(x, y, u, v, scale=150, color='k')
qk = plt.quiverkey(cs2, 1, 0.03, 10, r'10 m/s', labelpos='W')
cmap = ncm.cmap('testcmap')
cs.set_cmap(cmap)
cbar = m.colorbar(cs, location='right', pad='10%', drawedges=True)
cbar.set_ticks(barlim)
cbar.set_ticklabels(map(str, barlim))
cbar.ax.tick_params(axis='x', size=.1)
cbar.set_label(r'\textbf{925mb wind anomalies [m/s]}')
fig.suptitle(r'\textbf{JAS 2007}')
plt.savefig(directoryfigure + 'testwind.png', dpi=300)
'Completed: Script done!'
def main(dataDir,
visit,
title="",
outputTxtFileName=None,
showFwhm=False,
minFwhm=None,
maxFwhm=None,
correctDistortion=False,
showEllipticity=False,
ellipticityDirection=False,
showNdataFwhm=False,
showNdataEll=False,
minNdata=None,
maxNdata=None,
gridPoints=30,
verbose=False):
butler = dafPersist.ButlerFactory(mapper=hscSim.HscSimMapper(
root=dataDir)).create()
camera = butler.get("camera")
if not (showFwhm or showEllipticity or showNdataFwhm or showNdataEll
or outputTxtFileName):
showFwhm = True
#
# Get a dict of cameraGeom::Ccd indexed by serial number
#
ccds = {}
for raft in camera:
for ccd in raft:
ccd.setTrimmed(True)
ccds[ccd.getId().getSerial()] = ccd
#
# Read all the tableSeeingMap files, converting their (x, y) to focal plane coordinates
#
xArr = []
yArr = []
ellArr = []
fwhmArr = []
paArr = []
aArr = []
bArr = []
e1Arr = []
e2Arr = []
elle1e2Arr = []
for tab in butler.subset("tableSeeingMap", visit=visit):
# we could use tab.datasetExists() but it prints a rude message
fileName = butler.get("tableSeeingMap_filename", **tab.dataId)[0]
if not os.path.exists(fileName):
continue
with open(fileName) as fd:
ccd = None
for line in fd.readlines():
if re.search(r"^\s*#", line):
continue
fields = [float(_) for _ in line.split()]
if ccd is None:
ccd = ccds[int(fields[0])]
x, y, fwhm, ell, pa, a, b = fields[1:8]
x, y = ccd.getPositionFromPixel(geom.PointD(x, y)).getMm()
xArr.append(x)
yArr.append(y)
ellArr.append(ell)
fwhmArr.append(fwhm)
paArr.append(pa)
aArr.append(a)
bArr.append(b)
if len(fields) == 11:
e1 = fields[8]
e2 = fields[9]
elle1e2 = fields[10]
else:
e1 = -9999.
e2 = -9999.
elle1e2 = -9999.
e1Arr.append(e1)
e2Arr.append(e2)
elle1e2Arr.append(elle1e2)
xArr = np.array(xArr)
yArr = np.array(yArr)
ellArr = np.array(ellArr)
fwhmArr = np.array(fwhmArr) * 0.168 # arcseconds
paArr = np.radians(np.array(paArr))
aArr = np.array(aArr)
bArr = np.array(bArr)
e1Arr = np.array(e1Arr)
e2Arr = np.array(e2Arr)
elle1e2Arr = np.array(elle1e2Arr)
if correctDistortion:
import lsst.afw.geom.ellipses as afwEllipses
dist = camera.getDistortion()
for i in range(len(aArr)):
axes = afwEllipses.Axes(aArr[i], bArr[i], paArr[i])
if False: # testing only!
axes = afwEllipses.Axes(1.0, 1.0, np.arctan2(yArr[i], xArr[i]))
quad = afwGeom.Quadrupole(axes)
quad = quad.transform(
dist.computeQuadrupoleTransform(geom.PointD(xArr[i], yArr[i]),
False))
axes = afwEllipses.Axes(quad)
aArr[i], bArr[i], paArr[i] = axes.getA(), axes.getB(
), axes.getTheta()
ellArr = 1 - bArr / aArr
if len(xArr) == 0:
gridPoints = 0
xs, ys = [], []
else:
N = gridPoints * 1j
extent = [min(xArr), max(xArr), min(yArr), max(yArr)]
xs, ys = np.mgrid[extent[0]:extent[1]:N, extent[2]:extent[3]:N]
title = [
title,
]
title.append("\n#")
if outputTxtFileName:
f = open(outputTxtFileName, 'w')
f.write("# %s visit %s\n" % (" ".join(title), visit))
for x, y, ell, fwhm, pa, a, b, e1, e2, elle1e2 \
in zip(xArr, yArr, ellArr, fwhmArr, paArr, aArr, bArr, e1Arr, e2Arr, elle1e2Arr):
f.write('%f %f %f %f %f %f %f %f %f %f\n' %
(x, y, ell, fwhm, pa, a, b, e1, e2, elle1e2))
if showFwhm:
title.append("FWHM (arcsec)")
if len(xs) > 0:
fwhmResampled = griddata(xArr, yArr, fwhmArr, xs, ys)
plt.imshow(fwhmResampled.T,
extent=extent,
vmin=minFwhm,
vmax=maxFwhm,
origin='lower')
plt.colorbar()
if outputTxtFileName:
ndataGrids = getNumDataGrids(xArr, yArr, fwhmArr, xs, ys)
f = open(outputTxtFileName + '-fwhm-grid.txt', 'w')
f.write("# %s visit %s\n" % (" ".join(title), visit))
for xline, yline, fwhmline, ndataline \
in zip(xs.tolist(), ys.tolist(), fwhmResampled.tolist(), ndataGrids):
for xx, yy, fwhm, ndata in zip(xline, yline, fwhmline,
ndataline):
if fwhm is None:
fwhm = -9999
f.write('%f %f %f %d\n' % (xx, yy, fwhm, ndata))
elif showEllipticity:
title.append("Ellipticity")
scale = 4
if ellipticityDirection: # we don't care about the magnitude
ellArr = 0.1
u = -ellArr * np.cos(paArr)
v = -ellArr * np.sin(paArr)
if gridPoints > 0:
u = griddata(xArr, yArr, u, xs, ys)
v = griddata(xArr, yArr, v, xs, ys)
x, y = xs, ys
else:
x, y = xArr, yArr
Q = plt.quiver(
x,
y,
u,
v,
scale=scale,
pivot="middle",
headwidth=0,
headlength=0,
headaxislength=0,
)
keyLen = 0.10
if not ellipticityDirection: # we care about the magnitude
plt.quiverkey(Q, 0.20, 0.95, keyLen, "e=%g" % keyLen, labelpos='W')
if outputTxtFileName:
ndataGrids = getNumDataGrids(xArr, yArr, ellArr, xs, ys)
f = open(outputTxtFileName + '-ell-grid.txt', 'w')
f.write("# %s visit %s\n" % (" ".join(title), visit))
# f.write('# %f %f %f %f %f %f %f\n' % (x, y, ell, fwhm, pa, a, b))
for xline, yline, uline, vline, ndataline \
in zip(x.tolist(), y.tolist(), u.tolist(), v.tolist(), ndataGrids):
for xx, yy, uu, vv, ndata in zip(xline, yline, uline, vline,
ndataline):
if uu is None:
uu = -9999
if vv is None:
vv = -9999
f.write('%f %f %f %f %d\n' % (xx, yy, uu, vv, ndata))
elif showNdataFwhm:
title.append("N per fwhm grid")
if len(xs) > 0:
ndataGrids = getNumDataGrids(xArr, yArr, fwhmArr, xs, ys)
plt.imshow(ndataGrids,
interpolation='nearest',
extent=extent,
vmin=minNdata,
vmax=maxNdata,
origin='lower')
plt.colorbar()
else:
pass
elif showNdataEll:
title.append("N per ell grid")
if len(xs) > 0:
ndataGrids = getNumDataGrids(xArr, yArr, ellArr, xs, ys)
plt.imshow(ndataGrids,
interpolation='nearest',
extent=extent,
vmin=minNdata,
vmax=maxNdata,
origin='lower')
plt.colorbar()
else:
pass
# plt.plot(xArr, yArr, "r.")
# plt.plot(xs, ys, "b.")
plt.axes().set_aspect('equal')
plt.axis([-20000, 20000, -20000, 20000])
def frameInfoFrom(filepath):
with fits.open(filepath) as hdul:
h = hdul[0].header
'object=ABELL2163 filter=HSC-I exptime=360.0 alt=62.11143274 azm=202.32265181 '
'hst=(23:40:08.363-23:40:48.546)'
return 'object=%s filter=%s exptime=%.1f azm=%.2f hst=%s' % \
(h['OBJECT'], h['FILTER01'], h['EXPTIME'], h['AZIMUTH'], h['HST'])
title.insert(
0,
frameInfoFrom(
butler.get('raw_filename', {
'visit': visit,
'ccd': 0
})[0]))
title.append(r'$\langle$FWHM$\rangle %4.2f$"' % np.median(fwhmArr))
plt.title("%s visit=%s" % (" ".join(title), visit), fontsize=9)
return plt
def geoplot(data=None, lon=None, lat=None, **kw):
'''Show 2D data in a lon-lat plane.
Parameters
-----------
data: array of shape (n_lat, n_lon), or [u_array, v_array]-like for (u,v)
data or None(default) when only plotting the basemap.
lon: n_lon length vector or None(default).
lat: n_lat length vector or None(default).
kw: dict parameters related to basemap or plot functions.
Basemap related parameters:
----------------------------
basemap_kw: dict parameter in the initialization of a Basemap.
proj or projection: map projection name (default='moll')
popular projections: 'ortho', 'np'(='nplaea'), 'sp'(='splaea')
and other projections given from basemap.
lon_0: map center longitude (None as default).
lat_0: map center latitude (None as default).
lonlatcorner: (llcrnrlon, urcrnrlon, llcrnrlat, urcrnrlat).
boundinglat: latitude at the map out boundary (None as default).
basemap_round or round: True(default) or False.
fill_continents: bool value (False as default).
continents_kw: dict parameter used in the Basemap.fillcontinents method.
continents_color: color of continents ('0.33' as default).
lake_color: color of lakes ('none' as default).
ocean_color: color of ocean (None as default).
coastlines_kw: dict parameter used in the Basemap.drawcoastlines method.
coastlines_color: color of coast lines ('0.33' as default).
gridOn: bool value (True as default).
gridLabelOn: bool value (False as default).
parallels_kw: dict parameters used in the Basemap.drawparallels method.
parallels: parallels to be drawn (None as default).
parallels_color: color of parallels ('0.5' as default).
parallels_labels:[0,0,0,0] or [1,0,0,0].
meridians_kw: dict parameters used in the Basemap.drawmeridians method.
meridians: meridians to be drawn (None as default).
meridians_color: color of meridians (parallels_color as default).
meridians_labels: [0,0,0,0] or [0,0,0,1].
lonlatbox: None or (lon_start, lon_end, lat_start, lat_end).
lonlatbox_kw: dict parameters in the plot of lon-lat box.
lonlatbox_color:
General plot parameters:
-------------------------
ax: axis object, default is plt.gca()
plot_type: a string of plot type from ('pcolor', 'pcolormesh', 'imshow', 'contourf', 'contour', 'quiver', 'scatter') or None(default).
cmap: pyplot colormap.
clim: a tuple of colormap limit.
levels: sequence, int or None (default=None)
plot_kw: dict parameters used in the plot functions.
Pcolor/Pcolormesh related parameters:
-------------------------------
rasterized: bool (default is True).
Imshow related parameters
---------------------------
origin: 'lower' or 'upper'.
extent: horizontal range.
interpolation: 'nearest' (default) or 'bilinear' or 'cubic'.
Contourf related parameters:
-------------------------------
extend: 'both'(default).
Contour related parameters:
----------------------------
label_contour: False(default) or True.
Whether to label contours or not.
colors: contour color (default is 'gray').
Quiver plot related parameters:
--------------------------------
stride: stride along lon and lat.
stride_lon: stride along lon.
stride_lat: stride along lat.
quiver_scale: quiver scale.
quiver_color: quiver color.
sparse_polar_grids: bool, default is True.
quiver_kw: dict parameters used in the plt.quiver function.
hide_qkey: bool value, whether to show the quiverkey plot.
qkey_X: X parameter in the plt.quiverkey function (default is 0.85).
qkey_Y: Y parameter in the plt.quiverkey function (default is 1.02).
qkey_U: U parameter in the plt.quiverkey function (default is 2).
qkey_label: label parameter in the plt.quiverkey function.
qkey_labelpos: labelpos parameter in the plt.quiverkey function.
qkey_kw: dict parameters used in the plt.quiverkey function.
Scatter related parameters:
------------------------------
scatter_data: None(default) or (lonvec, latvec).
Hatch plot related parameters:
----------------------------------
hatches: ['///'] is default.
Colorbar related parameters:
-------------------------------
hide_cbar: bool value, whether to show the colorbar.
cbar_type: 'vertical'(shorten as 'v') or 'horizontal' (shorten as 'h').
cbar_extend: extend parameter in the plt.colorbar function.
'neither' as default here.
cbar_size: default '2.5%' for vertical colorbar,
'5%' for horizontal colorbar.
cbar_pad: default 0.1 for vertical colorbar,
0.4 for horizontal colorbar.
cbar_kw: dict parameters used in the plt.colorbar function.
units: str
long_name: str
Returns
--------
basemap object if only basemap is plotted.
plot object if data is shown.
'''
# target axis
ax = kw.pop('ax', None)
if ax is not None:
plt.sca(ax)
if isinstance(data, xr.DataArray):
data_array = data.copy()
data = data_array.values
if np.any(np.isnan(data)):
data = ma.masked_invalid(data)
if lon is None:
try:
lonname = [
s for s in data_array.dims
if s in ('lon', 'longitude', 'X')
][0]
except IndexError:
lonname = [s for s in data_array.dims if 'lon' in s][0]
lon = data_array[lonname]
if lat is None:
try:
latname = [
s for s in data_array.dims if s in ('lat', 'latitude', 'Y')
][0]
except IndexError:
latname = [s for s in data_array.dims if 'lat' in s][0]
lat = data_array[latname]
# guess data name
try:
data_name = data_array.attrs['long_name']
except KeyError:
try:
data_name = data_array.name
except AttributeError:
data_name = ''
# guess data units
try:
data_units = data_array.attrs['units']
except KeyError:
data_units = ''
# copy the original data
elif data is not None:
try:
data = data.copy()
except:
try:
# data has two components(u,v)
data = (data[0].copy(), data[1].copy())
except:
pass
if lon is not None:
lon = lon.copy()
if lat is not None:
lat = lat.copy()
# #### basemap parameters
# basemap kw parameter
basemap_kw = kw.pop('basemap_kw', {})
# projection
# proj = kw.pop('proj', 'cyl')
# proj = kw.pop('proj', 'moll')
proj = kw.pop('proj', 'hammer')
proj = kw.pop('projection',
proj) # projection overrides the proj parameter
# short names for nplaea and splaea projections
if proj in ('npolar', 'polar', 'np'):
proj = 'nplaea'
elif proj in ('spolar', 'sp'):
proj = 'splaea'
# lon_0
lon_0 = kw.pop('lon_0', None)
if lon_0 is None:
if lon is not None:
if np.isclose(np.abs(lon[-1] - lon[0]), 360):
lon_0 = (lon[0] + lon[-2]) / 2.0
else:
lon_0 = (lon[0] + lon[-1]) / 2.0
else:
# dummy = np.linspace(0, 360, data.shape[1]+1)[0:-1]
# lon_0 = ( dummy[0] + dummy[-1] )/2.0
lon_0 = 180
# elif proj in ('moll', 'cyl', 'hammer', 'robin'):
# lon_0 = 180
# elif proj in ('ortho','npstere', 'nplaea', 'npaeqd', 'spstere', 'splaea', 'spaeqd'):
# lon_0 = 0
else: # lon_0 is specified
if lon is not None and proj in ('moll', 'cyl', 'hammer'):
# correct the lon_0 so that it is at the edge of a grid box
lon_0_data = (lon[0] + lon[-1]) / 2.0
d_lon = lon[1] - lon[0]
d_lon_0 = lon_0 - lon_0_data
lon_0 = float(int(d_lon_0 / d_lon)) * d_lon + lon_0_data
# lat_0
lat_0 = kw.pop('lat_0', None)
if lat_0 is None:
if lat is not None:
lat_0 = (lat[0] + lat[-1]) / 2.0
elif proj in ('ortho', ):
lat_0 = 45
# lonlatcorner = (llcrnrlon, urcrnrlon, llcrnrlat, urcrnrlat)
lonlatcorner = kw.pop('lonlatcorner', None)
if lonlatcorner is not None:
llcrnrlon = lonlatcorner[0]
urcrnrlon = lonlatcorner[1]
llcrnrlat = lonlatcorner[2]
urcrnrlat = lonlatcorner[3]
else:
llcrnrlon = None
urcrnrlon = None
llcrnrlat = None
urcrnrlat = None
llcrnrlon = basemap_kw.pop('llcrnrlon', llcrnrlon)
urcrnrlon = basemap_kw.pop('urcrnrlon', urcrnrlon)
llcrnrlat = basemap_kw.pop('llcrnrlat', llcrnrlat)
urcrnrlat = basemap_kw.pop('urcrnrlat', urcrnrlat)
if llcrnrlon is None and urcrnrlon is None and llcrnrlat is None and urcrnrlat is None:
lonlatcorner = None
else:
lonlatcorner = (llcrnrlon, urcrnrlon, llcrnrlat, urcrnrlat)
# boundinglat
boundinglat = kw.pop('boundinglat', None)
if boundinglat is None:
if proj in ('npstere', 'nplaea', 'npaeqd'):
boundinglat = 30
elif proj in ('spstere', 'splaea', 'spaeqd'):
boundinglat = -30
# basemap round: True or False
if proj in ('npstere', 'nplaea', 'npaeqd', 'spstere', 'splaea', 'spaeqd'):
basemap_round = kw.pop('basemap_round', True)
else:
basemap_round = kw.pop('basemap_round', False)
basemap_round = kw.pop('round', basemap_round)
# base map
proj = basemap_kw.pop('projection', proj)
lon_0 = basemap_kw.pop('lon_0', lon_0)
lat_0 = basemap_kw.pop('lat_0', lat_0)
boundinglat = basemap_kw.pop('boundinglat', boundinglat)
basemap_round = basemap_kw.pop('round', basemap_round)
m = Basemap(projection=proj,
lon_0=lon_0,
lat_0=lat_0,
boundinglat=boundinglat,
round=basemap_round,
llcrnrlon=llcrnrlon,
urcrnrlon=urcrnrlon,
llcrnrlat=llcrnrlat,
urcrnrlat=urcrnrlat,
**basemap_kw)
# fill continents or plot coast lines
fill_continents = kw.pop('fill_continents', False)
if fill_continents:
# use Basemap.fillcontinents method
continents_kw = kw.pop('continents_kw', {})
continents_color = kw.pop('continents_color', '0.33')
continents_color = continents_kw.pop('color', continents_color)
lake_color = kw.pop('lake_color', 'none')
lake_color = continents_kw.pop('lake_color', lake_color)
m.fillcontinents(color=continents_color,
lake_color=lake_color,
**continents_kw)
# else:
draw_coastlines = kw.pop('draw_coastlines', not fill_continents)
if draw_coastlines:
# use Basemap.drawcoastlines method
coastlines_kw = kw.pop('coastlines_kw', {})
coastlines_color = kw.pop('coastlines_color', '0.33')
coastlines_color = coastlines_kw.pop('color', coastlines_color)
coastlines_lw = kw.pop('coastlines_lw', 0.5)
coastlines_lw = coastlines_kw.pop('lw', coastlines_lw)
m.drawcoastlines(color=coastlines_color,
linewidth=coastlines_lw,
**coastlines_kw)
ocean_color = kw.pop('ocean_color', None)
if ocean_color is not None:
m.drawmapboundary(fill_color=ocean_color)
# parallels
gridOn = kw.pop('gridOn', True)
gridLabelOn = kw.pop('gridLabelOn', False)
parallels_kw = kw.pop('parallels_kw', {})
# parallels = kw.pop('parallels', np.arange(-90,91,30))
parallels = kw.pop('parallels', None)
parallels = parallels_kw.pop('parallels', parallels)
parallels_color = kw.pop('parallels_color', '0.5')
parallels_color = parallels_kw.pop('color', parallels_color)
parallels_lw = kw.pop('parallels_lw', 0.5)
parallels_lw = parallels_kw.pop('lw', parallels_lw)
parallels_labels = kw.pop('parallels_labels', None)
parallels_labels = parallels_kw.pop('labels', parallels_labels)
if parallels_labels is None:
if gridLabelOn:
parallels_labels = [1, 0, 0, 0]
else:
parallels_labels = [0, 0, 0, 0]
if parallels is not None:
m.drawparallels(parallels,
color=parallels_color,
labels=parallels_labels,
linewidth=parallels_lw,
**parallels_kw)
elif gridOn:
m.drawparallels(np.arange(-90, 91, 30),
color=parallels_color,
linewidth=parallels_lw,
labels=parallels_labels,
**parallels_kw)
# meridians
meridians_kw = kw.pop('meridians_kw', {})
# meridians = kw.pop('meridians', np.arange(-180, 360, 30))
meridians = kw.pop('meridians', None)
meridians = meridians_kw.pop('meridians', meridians)
meridians_color = kw.pop('meridians_color', parallels_color)
meridians_color = meridians_kw.pop('color', meridians_color)
meridians_lw = kw.pop('meridians_lw', parallels_lw)
meridians_lw = meridians_kw.pop('lw', meridians_lw)
meridians_labels = kw.pop('meridians_labels', None)
meridians_labels = meridians_kw.pop('labels', meridians_labels)
if meridians_labels is None:
if gridLabelOn:
if proj in ('npstere', 'nplaea', 'npaeqd', 'spstere', 'splaea',
'spaeqd'):
meridians_labels = [1, 1, 0, 0]
elif proj in ('cyl', ):
meridians_labels = [0, 0, 0, 1]
else:
meridians_labels = [0, 0, 0, 0]
print('Meridian are not labeled.')
else:
meridians_labels = [0, 0, 0, 0]
if meridians is not None:
m.drawmeridians(meridians,
color=meridians_color,
labels=meridians_labels,
linewidth=meridians_lw,
**meridians_kw)
elif gridOn:
m.drawmeridians(np.arange(0, 360, 30),
color=meridians_color,
labels=meridians_labels,
linewidth=meridians_lw,
**meridians_kw)
# lonlatbox
lonlatbox = kw.pop('lonlatbox', None)
if lonlatbox is not None:
lonlon = np.array([
np.linspace(lonlatbox[0], lonlatbox[1],
100), lonlatbox[1] * np.ones(100),
np.linspace(lonlatbox[1], lonlatbox[0], 100),
lonlatbox[0] * np.ones(100)
]).ravel()
latlat = np.array([
lonlatbox[2] * np.ones(100),
np.linspace(lonlatbox[2], lonlatbox[3], 100),
lonlatbox[3] * np.ones(100),
np.linspace(lonlatbox[3], lonlatbox[2], 100)
]).ravel()
lonlatbox_kw = kw.pop('lonlatbox_kw', {})
lonlatbox_color = kw.pop('lonlatbox_color', 'k')
lonlatbox_color = lonlatbox_kw.pop('color', lonlatbox_color)
m.plot(lonlon,
latlat,
latlon=True,
color=lonlatbox_color,
**lonlatbox_kw)
# scatter
scatter_data = kw.pop('scatter_data', None)
if scatter_data is not None:
# L = data.astype('bool')
# marker_color = kw.pop('marker_color', 'k')
# plot_obj = m.scatter(X[L], Y[L], color=marker_color, **kw)
lonvec, latvec = scatter_data
plot_obj = m.scatter(lonvec, latvec, **kw)
# #### stop here and return the map object if data is None
if data is None:
return m
# data prepare
input_data_have_two_components = isinstance(data, tuple) \
or isinstance(data, list)
if input_data_have_two_components:
# input data is (u,v) or [u, v] where u, v are ndarray and two components of a vector
assert len(
data) == 2, 'quiver data must contain only two componets u and v'
u = data[0].squeeze()
v = data[1].squeeze()
assert u.ndim == 2, 'u component data must be two dimensional'
assert v.ndim == 2, 'v component data must be two dimensional'
data = np.sqrt(u**2 + v**2) # calculate wind speed
else: # input data is a ndarray
data = data.squeeze()
assert data.ndim == 2, 'Input data must be two dimensional!'
# lon
if lon is None:
# lon = np.linspace(0, 360, data.shape[1]+1)[0:-1]
# lon_edge = np.hstack((
# lon[0]*2 - lon[1],
# lon,
# lon[-1]*2 - lon[-2]))
# lon_edge = ( lon_edge[:-1] + lon_edge[1:] )/2.0
lon_edge = np.linspace(lon_0 - 180, lon_0 + 180, data.shape[1] + 1)
lon = (lon_edge[:-1] + lon_edge[1:]) / 2.0
else: # lon is specified
if np.isclose(np.abs(lon[-1] - lon[0]), 360):
# first and last longitude point to the same location: remove the last longitude
lon = lon[:-1]
data = data[:, :-1]
if input_data_have_two_components:
u = u[:, :-1]
v = v[:, :-1]
if (not np.isclose(lon_0, (lon[0] + lon[-1]) / 2.0)
and proj in ('moll', 'cyl', 'hammer', 'robin')):
# lon_0 not at the center of lon, need to shift grid
lon_west_end = lon_0 - 180 + (
lon[1] - lon[0]) / 2.0 # longitude of west end
# make sure the longitude of west end within the lon
if lon_west_end < lon[0]:
lon_west_end += 360
elif lon_west_end > lon[-1]:
lon_west_end -= 360
data, lon_shift = shiftgrid(lon_west_end, data, lon, start=True)
if input_data_have_two_components:
u, lon_shift = shiftgrid(lon_west_end, u, lon, start=True)
v, lon_shift = shiftgrid(lon_west_end, v, lon, start=True)
lon = lon_shift
if lon[0] < -180:
lon += 360
elif lon[-1] >= 540:
lon -= 360
lon_hstack = np.hstack(
(2 * lon[0] - lon[1], lon, 2 * lon[-1] - lon[-2]))
lon_edge = (lon_hstack[:-1] + lon_hstack[1:]) / 2.0
# lat
if lat is None:
lat_edge = np.linspace(-90, 90, data.shape[0] + 1)
lat = (lat_edge[:-1] + lat_edge[1:]) / 2.0
else:
lat_hstack = np.hstack(
(2 * lat[0] - lat[1], lat, 2 * lat[-1] - lat[-2]))
lat_edge = (lat_hstack[:-1] + lat_hstack[1:]) / 2.0
lat_edge[lat_edge > 90] = 90
lat_edge[lat_edge < -90] = -90
Lon, Lat = np.meshgrid(lon, lat)
X, Y = m(Lon, Lat)
Lon_edge, Lat_edge = np.meshgrid(lon_edge, lat_edge)
X_edge, Y_edge = m(Lon_edge, Lat_edge)
# ###### plot parameters
# plot_type
plot_type = kw.pop('plot_type', None)
if plot_type is None:
if input_data_have_two_components:
plot_type = 'quiver'
# elif ( proj in ('cyl',)
# and lonlatcorner is None
# ):
# plot_type = 'imshow'
# print('plot_type **** imshow **** is used.')
elif proj in ('nplaea', 'splaea', 'ortho'):
# pcolormesh has a problem for these projections
plot_type = 'pcolor'
print('plot_type **** pcolor **** is used.')
else:
plot_type = 'pcolormesh'
print('plot_type **** pcolormesh **** is used.')
# cmap
cmap = kw.pop('cmap', None)
if cmap is None:
zz_max = data.max()
zz_min = data.min()
if zz_min >= 0:
try:
cmap = plt.get_cmap('viridis')
except:
cmap = plt.get_cmap('OrRd')
elif zz_max <= 0:
try:
cmap = plt.get_cmap('viridis')
except:
cmap = plt.get_cmap('Blues_r')
else:
cmap = plt.get_cmap('RdBu_r')
elif isinstance(cmap, str):
cmap = plt.get_cmap(cmap)
# clim parameters
clim = kw.pop('clim', None)
robust = kw.pop('robust', False)
if clim is None:
if isinstance(data, np.ma.core.MaskedArray):
data1d = data.compressed()
else:
data1d = data.ravel()
notNaNs = np.logical_not(np.isnan(data1d))
data1d = data1d[notNaNs]
if robust:
a = np.percentile(data1d, 2)
b = np.percentile(data1d, 98)
else:
a = data1d.min()
b = data1d.max()
if a * b < 0:
b = max(abs(a), abs(b))
a = -b
clim = a, b
# levels
levels = kw.pop('levels', None)
if levels is None:
if plot_type in ('contour', 'contourf', 'contourf+'):
a, b = clim
levels = np.linspace(a, b, 11)
elif isinstance(levels, int):
if plot_type in ('contour', 'contourf', 'contourf+'):
a, b = clim
levels = np.linspace(a, b, levels)
elif plot_type in ('pcolor', 'pcolormesh', 'imshow'):
cmap = plt.get_cmap(cmap.name, levels - 1)
else: # levels is a sequence
if plot_type in ('pcolor', 'pcolormesh', 'imshow'):
cmap = plt.get_cmap(cmap.name, len(levels) - 1)
clim = min(levels), max(levels)
# colorbar parameters
if plot_type in ('pcolor', 'pcolormesh', 'contourf', 'contourf+',
'imshow'):
cbar_type = kw.pop('cbar_type', 'vertical')
cbar_kw = kw.pop('cbar_kw', {})
cbar_extend = kw.pop('cbar_extend', 'neither')
cbar_extend = cbar_kw.pop('extend', cbar_extend)
hide_cbar = kw.pop('hide_cbar', False)
if cbar_type in ('v', 'vertical'):
cbar_size = kw.pop('cbar_size', '2.5%')
cbar_size = cbar_kw.pop('size', cbar_size)
cbar_pad = kw.pop('cbar_pad', 0.1)
cbar_pad = cbar_kw.pop('pad', cbar_pad)
cbar_position = 'right'
cbar_orientation = 'vertical'
elif cbar_type in ('h', 'horizontal'):
# cbar = hcolorbar(units=units)
cbar_size = kw.pop('cbar_size', '5%')
cbar_size = cbar_kw.pop('size', cbar_size)
cbar_pad = kw.pop('cbar_pad', 0.4)
cbar_pad = cbar_kw.pop('pad', cbar_pad)
cbar_position = 'bottom'
cbar_orientation = 'horizontal'
# units in colorbar
units = kw.pop('units', None)
if units is None:
try:
units = data_units # input data is a DataArray
except:
units = ''
# long_name in colorbar
long_name = kw.pop('long_name', None)
if long_name is None:
try:
long_name = data_name # if input data is a DataArray
if long_name is None:
long_name = ''
except:
long_name = ''
# ###### plot
# pcolor
if plot_type in ('pcolor', ):
rasterized = kw.pop('rasterized', True)
plot_obj = m.pcolor(X_edge,
Y_edge,
data,
cmap=cmap,
rasterized=rasterized,
**kw)
# pcolormesh
elif plot_type in ('pcolormesh', ):
rasterized = kw.pop('rasterized', True)
plot_obj = m.pcolormesh(X_edge,
Y_edge,
data,
cmap=cmap,
rasterized=rasterized,
**kw)
# imshow
elif plot_type in ('imshow', ):
if Y_edge[-1, 0] > Y_edge[0, 0]:
origin = kw.pop('origin', 'lower')
else:
origin = kw.pop('origin', 'upper')
extent = kw.pop(
'extent',
[X_edge[0, 0], X_edge[0, -1], Y_edge[0, 0], Y_edge[-1, 0]])
interpolation = kw.pop('interpolation', 'nearest')
plot_obj = m.imshow(data,
origin=origin,
cmap=cmap,
extent=extent,
interpolation=interpolation,
**kw)
# contourf
elif plot_type in ('contourf', ):
if proj in ('ortho','npstere', 'nplaea', 'npaeqd', 'spstere',
'splaea', 'spaeqd')\
and np.isclose(np.abs(lon_edge[-1]-lon_edge[0]), 360):
data, lon = addcyclic(data, lon)
Lon, Lat = np.meshgrid(lon, lat)
X, Y = m(Lon, Lat)
extend = kw.pop('extend', 'both')
plot_obj = m.contourf(X,
Y,
data,
extend=extend,
cmap=cmap,
levels=levels,
**kw)
# contour
elif plot_type in ('contour', ):
if proj in ('ortho','npstere', 'nplaea', 'npaeqd', 'spstere',
'splaea', 'spaeqd')\
and np.isclose(np.abs(lon_edge[-1]-lon_edge[0]), 360):
data, lon = addcyclic(data, lon)
Lon, Lat = np.meshgrid(lon, lat)
X, Y = m(Lon, Lat)
colors = kw.pop('colors', 'k')
if colors is not None:
cmap = None
alpha = kw.pop('alpha', 0.5)
plot_obj = m.contour(X,
Y,
data,
cmap=cmap,
colors=colors,
levels=levels,
alpha=alpha,
**kw)
label_contour = kw.pop('label_contour', False)
if label_contour:
plt.clabel(plot_obj, plot_obj.levels[::2], fmt='%.2G')
# contourf + contour
elif plot_type in ('contourf+', ):
if proj in ('ortho','npstere', 'nplaea', 'npaeqd', 'spstere',
'splaea', 'spaeqd')\
and np.isclose(np.abs(lon_edge[-1]-lon_edge[0]), 360):
data, lon = addcyclic(data, lon)
Lon, Lat = np.meshgrid(lon, lat)
X, Y = m(Lon, Lat)
extend = kw.pop('extend', 'both')
linewidths = kw.pop('linewidths', 1)
plot_obj = m.contourf(X,
Y,
data,
extend=extend,
cmap=cmap,
levels=levels,
**kw)
colors = kw.pop('colors', 'k')
if colors is not None:
cmap = None
alpha = kw.pop('alpha', 0.5)
m.contour(X,
Y,
data,
cmap=cmap,
colors=colors,
alpha=alpha,
levels=levels,
linewidths=linewidths,
**kw)
# quiverplot
elif plot_type in ('quiver', ):
nGrids = kw.pop('nGrids', 50)
nx = kw.pop('nx', nGrids)
ny = kw.pop('ny', nGrids)
stride = kw.pop('stride', 1)
stride_lon = kw.pop('stride_lon', stride)
stride_lat = kw.pop('stride_lat', stride)
print(stride, stride_lon, stride_lat)
if (stride != 1) or (stride_lon != 1) or (
stride_lat != 1
): # compatible with old api, with stride, stride_lon, stride_lat controling quiver grids. To be obsolete. Use nGrids, nx, ny instead
print('stride used')
lon_ = lon[::stride_lon] # subset of lon
lat_ = lat[::stride_lat]
u_ = u[::stride_lat, ::stride_lon]
v_ = v[::stride_lat, ::stride_lon]
# sparse polar area
sparse_polar_grids = kw.pop('sparse_polar_grids', True)
if sparse_polar_grids:
msk = np.empty(u_.shape) * np.nan
for i in range(lat_.size):
step = int(1. / np.cos(lat_[i] * np.pi / 180))
msk[i, 0::step] = 0
u_ += msk
v_ += msk
Lon_, Lat_ = np.meshgrid(lon_, lat_)
u_rot, v_rot, X_, Y_ = m.rotate_vector(u_,
v_,
Lon_,
Lat_,
returnxy=True)
else: # use nGrids, nx, ny to control the quiver grids
if lon.max() > 180:
u_, lon_ = shiftgrid(180., u, lon, start=False)
v_, lon_ = shiftgrid(180., v, lon, start=False)
else:
u_ = u
v_ = v
lon_ = lon
u_rot, v_rot, X_, Y_ = m.transform_vector(u_,
v_,
lon_,
lat,
nx,
ny,
returnxy=True)
quiver_color = kw.pop('quiver_color', 'g')
quiver_scale = kw.pop('quiver_scale', None)
hide_qkey = kw.pop('hide_qkey', False)
qkey_kw = kw.pop('qkey_kw', {})
qkey_X = kw.pop('qkey_X', 0.85)
qkey_X = qkey_kw.pop('X', qkey_X)
qkey_Y = kw.pop('qkey_Y', 1.02)
qkey_Y = qkey_kw.pop('Y', qkey_Y)
qkey_U = kw.pop('qkey_U', 2)
qkey_U = qkey_kw.pop('U', qkey_U)
qkey_label = kw.pop('qkey_label', '{:g} '.format(qkey_U) + units)
qkey_label = qkey_kw.pop('label', qkey_label)
qkey_labelpos = kw.pop('qkey_labelpos', 'W')
qkey_labelpos = qkey_kw.pop('labelpos', qkey_labelpos)
plot_obj = m.quiver(X_,
Y_,
u_rot,
v_rot,
color=quiver_color,
scale=quiver_scale,
**kw)
if not hide_qkey:
# quiverkey plot
plt.quiverkey(plot_obj,
qkey_X,
qkey_Y,
qkey_U,
label=qkey_label,
labelpos=qkey_labelpos,
**qkey_kw)
# hatch plot
elif plot_type in ('hatch', 'hatches'):
hatches = kw.pop('hatches', ['///'])
plot_obj = m.contourf(X,
Y,
data,
colors='none',
hatches=hatches,
extend='both',
**kw)
else:
print(
'Please choose a right plot_type from ("pcolor", "contourf", "contour")!'
)
# set clim
if plot_type in ('pcolor', 'pcolormesh', 'imshow'):
plt.clim(clim)
# plot colorbar
if plot_type in ('pcolor', 'pcolormesh', 'contourf', 'contourf+',
'imshow'):
ax_current = plt.gca()
divider = make_axes_locatable(ax_current)
cax = divider.append_axes(cbar_position, size=cbar_size, pad=cbar_pad)
cbar = plt.colorbar(plot_obj,
cax=cax,
extend=cbar_extend,
orientation=cbar_orientation,
**cbar_kw)
if cbar_type in ('v', 'vertical'):
# put the units on the top of the vertical colorbar
cbar.ax.xaxis.set_label_position('top')
cbar.ax.set_xlabel(units)
cbar.ax.set_ylabel(long_name)
elif cbar_type in ('h', 'horizontal'):
# cbar.ax.yaxis.set_label_position('right')
# cbar.ax.set_ylabel(units, rotation=0, ha='left', va='center')
if long_name == '' or units == '':
cbar.ax.set_xlabel('{}{}'.format(long_name, units))
else:
cbar.ax.set_xlabel('{} [{}]'.format(long_name, units))
# remove the colorbar to avoid repeated colorbars
if hide_cbar:
cbar.remove()
# set back the main axes as the current axes
plt.sca(ax_current)
return plot_obj
def draw_wind(m, lons, lats,
model, dsize, background,
location, lat, lon,
RUNDATE, VALIDDATE, fxx,
alpha, half_box, barb_thin,
level='10 m',
Fill=False,
Shade=False,
Barbs=False,
Quiver=False,
p95=False,
Convergence=False,
Vorticity=False):
"""
wind speed, wind barbs, wind quiver, Convergence, Divergence,
shade high wind area, wind speed 95th percentile exceedance
"""
LEVEL = level.replace(' ', '')
H_UV = get_hrrr_variable(RUNDATE, 'UVGRD:%s' % level,
model=model, fxx=fxx,
outDIR='/uufs/chpc.utah.edu/common/home/u0553130/temp/',
verbose=False, value_only=False)
if Fill:
m.pcolormesh(lons, lats, H_UV['SPEED'],
latlon=True,
cmap=cm_wind(),
vmin=0, vmax=60,
zorder=2,
alpha=alpha)
cb = plt.colorbar(orientation='horizontal', pad=pad, shrink=shrink, extend='max')
cb.set_label(r'%s Wind Speed (m s$\mathregular{^{-1}}$)' % level)
if Shade:
m.contourf(lons, lats, H_UV['SPEED'],
levels=[10, 15, 20, 25],
colors=('yellow', 'orange', 'red'),
alpha=alpha,
extend='max',
zorder=3,
latlon=True)
cb = plt.colorbar(orientation='horizontal', shrink=shrink, pad=pad)
cb.set_label(r'%s Wind Speed (ms$\mathregular{^{-1}}$)' % level)
if Barbs or Quiver:
if level == '10 m':
color = 'k'
elif level == '80 m':
color = 'darkred'
elif level == '500 mb':
color = 'navy'
else:
color='k'
# For small domain plots, trimming the edges significantly reduces barb plotting time
if barb_thin < 20:
subset = hrrr_subset(H_UV, half_box=half_box, lat=lat, lon=lon, verbose=False)
else:
subset = H_UV
# Need to rotate vectors for map projection
subset['UGRD'], subset['VGRD'] = m.rotate_vector(subset['UGRD'], subset['VGRD'], subset['lon'], subset['lat'])
thin = barb_thin
# Add to plot
if Barbs:
m.barbs(subset['lon'][::thin,::thin], subset['lat'][::thin,::thin],
subset['UGRD'][::thin,::thin], subset['VGRD'][::thin,::thin],
zorder=10, length=5.5, color=color,
barb_increments={'half':2.5, 'full':5,'flag':25},
latlon=True)
if Quiver:
Q = m.quiver(subset['lon'][::thin,::thin], subset['lat'][::thin,::thin],
subset['UGRD'][::thin,::thin], subset['VGRD'][::thin,::thin],
zorder=10,
units='inches',
scale=40, color=color,
latlon=True)
qk = plt.quiverkey(Q, .92, 0.07, 10, r'10 s$^{-1}$',
labelpos='S',
coordinates='axes',
color='magenta')
qk.text.set_backgroundcolor('w')
if p95:
DIR = '/uufs/chpc.utah.edu/common/home/horel-group8/blaylock/HRRR_OSG/hourly30/UVGRD_%s/' % level.replace(' ', '_')
FILE = 'OSG_HRRR_%s_m%02d_d%02d_h%02d_f00.h5' % (('UVGRD_%s' % level.replace(' ', '_'), VALIDDATE.month, VALIDDATE.day, VALIDDATE.hour))
with h5py.File(DIR+FILE, 'r') as f:
spd_p95 = f["p95"][:]
masked = H_UV['SPEED']-spd_p95
masked = np.ma.array(masked)
masked[masked < 0] = np.ma.masked
m.pcolormesh(lons, lats, masked,
vmax=10, vmin=0,
latlon=True,
zorder=9,
cmap='viridis',
alpha=alpha)
cb = plt.colorbar(orientation='horizontal', pad=pad, shrink=shrink)
cb.set_label(r'%s Wind Speed exceeding 95th Percentile (m s$\mathregular{^{-1}}$)' % level)
if Convergence or Vorticity:
dudx, dudy = np.gradient(H_UV['UGRD'], 3, 3)
dvdx, dvdy = np.gradient(H_UV['VGRD'], 3, 3)
if Vorticity:
vorticity = dvdx - dudy
# Mask values
vort = vorticity
vort = np.ma.array(vort)
vort[np.logical_and(vort < .05, vort > -.05) ] = np.ma.masked
m.pcolormesh(lons, lats, vort,
latlon=True, cmap='bwr',
zorder=8,
vmax=np.max(vort),
vmin=-np.max(vort))
cb = plt.colorbar(orientation='horizontal', pad=pad, shrink=shrink)
cb.set_label(r'%s Vorticity (s$\mathregular{^{-1}}$)' % level)
if Convergence:
convergence = dudx + dvdy
# Mask values
conv = convergence
conv = np.ma.array(conv)
conv[np.logical_and(conv < .05, conv > -.05) ] = np.ma.masked
m.pcolormesh(lons, lats, conv,
latlon=True, cmap='bwr',
zorder=8,
vmax=np.max(conv),
vmin=-np.max(conv))
cb = plt.colorbar(orientation='horizontal', pad=pad, shrink=shrink)
cb.set_label(r'%s Convergence (s$\mathregular{^{-1}}$)' % level)
v = np.ma.masked_where(np.abs(v) >= 999, v)
x = f.variables['lon'][:]
y = f.variables['lat'][:]
vel = np.sqrt(u * u + v * v, where=(np.ma.getmaskarray(u) == False))
f.close()
# -
# ## Using colormap
plt.figure()
q = plt.quiver(x, y, u, v, vel, cmap=plt.cm.get_cmap('hsv'), scale=1000)
q.set_clim(0, 50)
cb = plt.colorbar(q)
cb.set_label('Wind speed (m/s)')
plt.show()
# ## Using reference arrow
#
# Adding a reference arrow is done by using the [quiverkey](https://matplotlib.org/3.1.1/api/_as_gen/matplotlib.pyplot.quiverkey.html) function
plt.figure()
q = plt.quiver(x, y, u, v, scale=1000)
keys = plt.quiverkey(q,
-131,
21,
70,
'Wind speed\n(50 m/s)',
coordinates='data')
plt.show()
def main():
source_all = [
'f4\\W3Main', 'f5\\W3OH', 'f6\\L1448I', 'f7\\L1448N', 'f8\\L1448C',
'f9\\L1445', 'f10\\IRAS2A', 'f11\\SVS13', 'f12\\IRAS4A', 'f13\\IRAS4B',
'f14\\HH211', 'f15\\DGTau', 'f16\\L1551', 'f17\\L1527', 'f18\\CB26',
'f19\\OrionKL', 'f20\\MMS5', 'f20\\MMS6', 'f21\\FIR4', 'f23\\VLA1623',
'f24\\SerEmb17', 'f26\\SerEmb8', 'f27\\SerEmb6', 'f31\\B335',
'f32\\DR21OH', 'f33\\L1157', 'f34\\CB230'
]
for ii in range(len(source_all)):
try:
tapol, scuba, hertz, sharp, Idust, xx, yy = take_data(
source_all[ii])
Imax = max((Idust[0].data[0, 0, :, :]).flatten())
center = numpy.where(Idust[0].data[0, 0, :, :] == Imax)
f, (ax1, ax2) = plt.subplots(1, 2, figsize=(60, 20))
tap = range(len(tapol[0]))
for i in range(len(tapol[0])):
tap[i] = numpy.sqrt((tapol[0][i] - xx[center[0]])**2.0 +
(tapol[1][i] - yy[center[1]])**2.0)
ax1.scatter(tap, tapol[4], color='b', label='tapol')
if scuba != []:
scu = range(len(scuba[0]))
for i in range(len(scuba[0])):
scu[i] = numpy.sqrt((scuba[0][i] - xx[center[0]])**2.0 +
(scuba[1][i] - yy[center[1]])**2.0)
ax1.scatter(scu, scuba[3], color='r', label='scuba')
if hertz != []:
her = range(len(hertz[0]))
for j in range(len(hertz[0])):
her[j] = numpy.sqrt((hertz[0][j] - xx[center[0]])**2.0 +
(hertz[1][j] - yy[center[1]])**2.0)
ax1.scatter(her, hertz[3], color='y', label='hertz')
if sharp != []:
sha = range(len(sharp[0]))
for k in range(len(sharp[0])):
sha[k] = numpy.sqrt((sharp[0][k] - xx[center[0]])**2.0 +
(sharp[1][k] - yy[center[1]])**2.0)
ax1.scatter(sha, sharp[3], color='g', label='sharp')
ax1.legend()
xx_dust, yy_dust = a.sky_coor(Idust)
ax2.contourf(Idust[0].data[0, 0, :, ::-1],
extent=[
max(xx_dust),
min(xx_dust),
min(yy_dust),
max(yy_dust)
],
origin='lower',
aspect='auto')
# qv1 = ax2.quiver(-tapol[0],tapol[1],-tapol[4]*numpy.sin(tapol[6]*numpy.pi/180.0),tapol[4]*numpy.cos(tapol[6]*numpy.pi/180.0),headwidth=0,width=0.001,scale=100,color='w',pivot='middle')
qv1 = ax2.quiver(-tapol[0],
tapol[1],
-tapol[2] *
numpy.sin(tapol[6] * numpy.pi / 180.0),
tapol[2] * numpy.cos(tapol[6] * numpy.pi / 180.0),
headwidth=0,
width=0.001,
scale=100,
color='w',
pivot='middle')
plt.quiverkey(qv1, 0.2, 0.2, 4, '4% Tapol')
if scuba != []:
qv2 = ax2.quiver(
-scuba[0],
scuba[1],
-scuba[3] * numpy.sin(scuba[5] * numpy.pi / 180.0),
scuba[3] * numpy.cos(scuba[5] * numpy.pi / 180.0),
headwidth=0,
width=0.001,
color='r',
scale=100,
pivot='middle')
plt.quiverkey(qv2, 0.2, 0.15, 4, '4% Scuba')
if hertz != []:
qv3 = ax2.quiver(
-hertz[0],
hertz[1],
-hertz[3] * numpy.sin(hertz[5] * numpy.pi / 180.0),
hertz[3] * numpy.cos(hertz[5] * numpy.pi / 180.0),
headwidth=0,
width=0.001,
color='y',
scale=100,
pivot='middle')
plt.quiverkey(qv3, 0.2, 0.1, 4, '4% Hertz')
if sharp != []:
qv4 = ax2.quiver(
-sharp[0],
sharp[1],
-sharp[3] * numpy.sin(sharp[5] * numpy.pi / 180.0),
sharp[3] * numpy.cos(sharp[5] * numpy.pi / 180.0),
headwidth=0,
width=0.001,
color='g',
scale=100,
pivot='middle')
plt.quiverkey(qv4, 0.2, 0.05, 4, '4% Sharp')
if ii > 4:
plt.savefig(source_all[ii][4:] + '_vector.png')
plt.clf()
else:
plt.savefig(source_all[ii][3:] + '_vector.png')
plt.clf()
except:
print 'except', source_all[ii]
def trend_all():
srfc = cnst.ERA_MONTHLY_SRFC_SYNOP
pl = cnst.ERA_MONTHLY_PL_SYNOP
storm_mean = 'aggs/gridsat_WA_-65_monthly_count_-40base_15-21UTC_1000km2.nc'
storm_extreme = 'aggs/gridsat_WA_-70_monthly_count_5000km2.nc'
mcs = cnst.GRIDSAT + storm_extreme
fpath = cnst.network_data + 'figs/CLOVER/months/'
box = [5, 55, -36, 0] # [-18,40,0,25] #
da = xr.open_dataset(pl)
da = u_darrays.flip_lat(da)
da = da.sel(longitude=slice(box[0], box[1]),
latitude=slice(box[2], box[3]))
da2 = xr.open_dataset(srfc)
da2 = u_darrays.flip_lat(da2)
da2 = da2.sel(longitude=slice(box[0], box[1]),
latitude=slice(box[2], box[3]))
da3 = xr.open_dataset(mcs)
da3 = da3.sel(lon=slice(box[0], box[1]), lat=slice(box[2], box[3]))
lons = da.longitude
lats = da.latitude
press = da2['sp']
press = press[press['time.hour'] == 12]
press.values = press.values * 1000
low_press = 850
up_press = 550
q = da['q'].sel(level=slice(low_press - 100, low_press)).mean('level')
q = q[q['time.hour'] == 12]
t2d = da2['t2m'] #['t2m']
#t2d = da['t'].sel(level=slice(800, 850)).mean('level')
t2d = t2d[t2d['time.hour'] == 12]
u600 = da['u'].sel(level=slice(up_press - 100, up_press)).mean('level')
u600 = u600[u600['time.hour'] == 12]
v600 = da['v'].sel(level=slice(up_press - 100, up_press)).mean('level')
v600 = v600[v600['time.hour'] == 12]
ws600 = u_met.u_v_to_ws_wd(u600, v600)
u800 = da['u'].sel(level=slice(low_press - 100, low_press)).mean('level')
u800 = u800[u800['time.hour'] == 12]
v800 = da['v'].sel(level=slice(low_press - 100, low_press)).mean('level')
v800 = v800[v800['time.hour'] == 12]
shear_u = u600 - u800 #u600-
shear_v = v600 - v800 # v600-
ws_shear = u_met.u_v_to_ws_wd(shear_u.values, shear_v.values)
ws_600 = t2d.copy(deep=True)
ws_600.name = 'ws'
ws_600.values = ws600[0]
shear = t2d.copy(deep=True)
shear.name = 'shear'
shear.values = ws_shear[0]
u6 = u800
v6 = v800 # wind vectors
q.values = q.values * 1000
grid = t2d.salem.grid.regrid(factor=0.25)
t2 = t2d # grid.lookup_transform(t2d)
tir = grid.lookup_transform(da3['tir'])
grid = grid.to_dataset()
tir = xr.DataArray(tir,
coords=[da3['time'], grid['y'], grid['x']],
dims=['time', 'latitude', 'longitude'])
months = [
(11, 1), 1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12
] #, 2,3,10]#[(12,2)]#[1,2,3,4,5,6,7,8,9,10,11,12]# #,2,3,11,12]#[(12,2)]#[1,2,3,4,5,6,7,8,9,10,11,12]# #,2,3,11,12]
dicm = {}
dicmean = {}
for m in months:
method = 'mk'
if type(m) == int:
m = [m]
sig = True
t2trend, t2mean = calc_trend(t2,
m,
method=method,
sig=sig,
hour=12,
wilks=False) #hour=12,
t2_mean = t2mean.mean(axis=0)
tirtrend, tirmean = calc_trend(tir,
m,
method=method,
sig=sig,
wilks=False)
tirm_mean = tirmean.mean(axis=0)
qtrend, qmean = calc_trend(q,
m,
method=method,
sig=sig,
hour=12,
wilks=False) #hour=12,
q_mean = qmean.mean(axis=0)
sheartrend, shearmean = calc_trend(shear,
m,
method=method,
sig=sig,
hour=12,
wilks=False) #hour=12,
shear_mean = shearmean.mean(axis=0)
u6trend, u6mean = calc_trend(u6,
m,
method=method,
sig=sig,
hour=12,
wilks=False) #hour=12,
u6_mean = u6mean.mean(axis=0)
v6trend, v6mean = calc_trend(v6,
m,
method=method,
sig=sig,
hour=12,
wilks=False) #hour=12,
v6_mean = v6mean.mean(axis=0)
t2trend_unstacked = t2trend * 10. # warming over decade
qtrend_unstacked = qtrend * 10. # warming over decade
sheartrend_unstacked = sheartrend * 10. # warming over decade
u6trend_unstacked = u6trend * 10
v6trend_unstacked = v6trend * 10
tirtrend_unstacked = (
(tirtrend.values) * 10. / tirm_mean.values) * 100.
tirtrend_out = xr.DataArray(tirtrend_unstacked,
coords=[grid['y'], grid['x']],
dims=['latitude', 'longitude'])
tirmean_out = xr.DataArray(tirm_mean,
coords=[grid['y'], grid['x']],
dims=['latitude', 'longitude'])
dicm[m[0]] = tirtrend_out
dicmean[m[0]] = tirmean_out
t_da = t2trend_unstacked
q_da = qtrend_unstacked
s_da = sheartrend_unstacked
ti_da = tirtrend_unstacked
if len(m) == 1:
fp = fpath + 'trend_synop_-70C5000_trend_' + str(
m[0]).zfill(2) + '.png'
else:
fp = fpath + 'trend_synop_-70C5000_trend_' + str(
m[0]).zfill(2) + '-' + str(m[1]).zfill(2) + '.png'
map = t2d.salem.get_map()
f = plt.figure(figsize=(15, 8), dpi=300)
# transform their coordinates to the map reference system and plot the arrows
xx, yy = map.grid.transform(shear.longitude.values,
shear.latitude.values,
crs=shear.salem.grid.proj)
xx, yy = np.meshgrid(xx, yy)
#Quiver only every 7th grid point
u = u6trend_unstacked.values[1::2, 1::2]
v = v6trend_unstacked.values[1::2, 1::2]
#Quiver only every 7th grid pointtr
uu = u6_mean.values[1::2, 1::2]
vv = v6_mean.values[1::2, 1::2]
xx = xx[1::2, 1::2]
yy = yy[1::2, 1::2]
ax1 = f.add_subplot(221)
map.set_data(t_da.values, interp='linear') # interp='linear'
map.set_contour((t2_mean.values - 273.15).astype(np.float64),
interp='linear',
colors='k',
linewidths=0.5,
levels=[20, 23, 26, 29, 32, 35])
map.set_plot_params(levels=[
-0.5, -0.4, -0.3, -0.2, -0.1, -0.05, -0.02, 0.02, 0.05, 0.1, 0.2,
0.3, 0.4, 0.5
],
cmap='RdBu_r',
extend='both') # levels=np.arange(-0.5,0.51,0.1),
#map.set_contour((t2_mean.values).astype(np.float64), interp='linear', colors='k', linewidths=0.5, levels=np.linspace(800,925,8))
#map.set_plot_params(levels=[-0.5,-0.4,-0.3,-0.2,-0.1,-0.05,-0.02, 0.02,0.05,0.1,0.2,0.3,0.4,0.5], cmap='RdBu_r', extend='both') # levels=np.arange(-0.5,0.51,0.1),
dic = map.visualize(ax=ax1,
title='2m temperature trend | contours: mean T',
cbar_title='K decade-1')
qu = ax1.quiver(xx, yy, uu, vv, scale=40, width=0.002) # 80
qk = plt.quiverkey(qu,
0.4,
0.03,
4,
'4 m s$^{-1}$',
labelpos='E',
coordinates='figure')
contours = dic['contour'][0]
plt.clabel(contours, inline=True, fontsize=7, fmt='%1.1f')
ax2 = f.add_subplot(222)
map.set_data(q_da.values, interp='linear') # interp='linear'
map.set_contour((q_mean.values).astype(np.float64),
interp='linear',
colors='k',
levels=[6, 8, 10, 12, 14, 16],
linewidths=0.5)
map.set_plot_params(levels=[
-0.4, -0.3, -0.2, -0.1, -0.05, -0.02, 0.02, 0.05, 0.1, 0.2, 0.3,
0.4
],
cmap='RdBu',
extend='both') # levels=np.arange(-0.5,0.51,0.1),
dic = map.visualize(
ax=ax2,
title='800hPa Spec. humidity trend | contours: mean q',
cbar_title='g kg-1 decade-1')
contours = dic['contour'][0]
plt.clabel(contours, inline=True, fontsize=7, fmt='%1.1f')
ax3 = f.add_subplot(223)
map.set_data(s_da.values, interp='linear') # interp='linear'
map.set_contour(s_da.values,
interp='linear',
levels=np.arange(-7, 7, 8),
cmap='Blues')
map.set_plot_params(levels=[
-0.5, -0.4, -0.3, -0.2, -0.1, -0.05, -0.02, 0.02, 0.05, 0.1, 0.2,
0.3, 0.4, 0.5
],
cmap='RdBu_r',
extend='both') # levels=np.arange(-0.5,0.51,0.1)
map.visualize(
ax=ax3,
title='800-500hPa wind shear trend, mean 850hPa wind vector trends',
cbar_title='m s-1 decade-1')
qu = ax3.quiver(xx, yy, u, v, scale=40, width=0.002) # 80
qk = plt.quiverkey(qu,
0.4,
0.03,
4,
'4 m s$^{-1}$',
labelpos='E',
coordinates='figure')
ax4 = f.add_subplot(224)
map.set_contour((tirm_mean.values).astype(np.float64),
interp='linear',
levels=[0.1, 0.5, 1, 2.5],
colors='k',
linewidths=0.5)
ti_da[ti_da == 0] = np.nan
map.set_data(ti_da) #
coord = [18, 25, -28, -20]
geom = shpg.box(coord[0], coord[2], coord[1], coord[3])
#map.set_geometry(geom, zorder=99, color='darkorange', linewidth=3, linestyle='--', alpha=0.3)
map.set_plot_params(
cmap='viridis', extend='both', levels=np.arange(
10, 41,
10)) # levels=np.arange(20,101,20) #np.arange(20,101,20)
dic = map.visualize(ax=ax4,
title='-65C cloud cover change | >1000km2 -40C',
cbar_title='$\%$ decade-1')
contours = dic['contour'][0]
plt.clabel(contours, inline=True, fontsize=7, fmt='%1.1f')
plt.tight_layout()
plt.savefig(fp)
plt.close('all')
pkl.dump(
dicm,
open(
cnst.network_data + 'data/CLOVER/saves/storm_frac_synop12UTC_SA.p',
'wb'))
pkl.dump(
dicmean,
open(
cnst.network_data +
'data/CLOVER/saves/storm_frac_mean_synop12UTC_SA.p', 'wb'))
pijd0 = 1
X, Y = np.meshgrid(np.arange(0, 5.2, step), np.arange(0, 4, step))
# others = [[1, 1], [1, 2], [2.732, 1], [2.732, 2]]
# others = [[1, 1], [1+1.732/2, 1.5], [2.732, 1]]
others = [[2, 2], [3, 2]]
U = 0
V = 0
for robot in others:
pijx = X - robot[0]
pijy = Y - robot[1]
pij0 = (pijx**2 + pijy**2)**0.5 # the norm of pij
pij0 = np.where(pij0 < 1e-4, 1, pij0)
tauij0 = 2 * (pij0**4 - pijd0**4) / pij0**3
U += tauij0 * pijx / pij0
V += tauij0 * pijy / pij0
U, V = saturate(U * K3, V * K3, 0.7)
plt.figure()
plt.title('Vector field')
Q = plt.quiver(X, Y, U, V, units='width')
qk = plt.quiverkey(Q,
0.9,
0.9,
2,
r'$2 \frac{m}{s}$',
labelpos='E',
coordinates='figure')
plt.axes().set_aspect('equal', 'datalim')
def show_image(wavelength,
parfilename=None,
par=None,
dir="./",
overplot=False,
inclination=80,
cmap=None,
ax=None,
polarization=False,
polfrac=False,
psf_fwhm=None,
vmin=None,
vmax=None):
""" Show one image from an MCFOST model
Parameters
----------
wavelength : string
note this is a string!! in microns. TBD make it take strings or floats
inclination : float
Which inclination to plot, in the case where there are multiple images? For RT computations
with just one, then this parameter is essentially ignored
overplot : bool
Should we overplot on current axes (True) or display a new figure? Default is False
cmap : matplotlib Colormap instance
Color map to use for display.
ax : matplotlib Axes instance
Axis to display into.
vmin, vmax : scalars
Min and max values for image display. Always shows in log stretch
psf_fwhm : float or None
convolve with PSF of this FWHM? Default is None for no convolution
parfilename : string, optional
par : dict, optional
dir : string
"""
if not overplot:
if ax is None: plt.clf()
else: plt.cla()
if ax is None: ax = plt.gca()
if par is None:
par = paramfiles.Paramfile(parfilename, dir)
if cmap is None:
cmap = plt.cm.gist_heat
cmap = plt.cm.gist_gray
cmap.set_over('white')
cmap.set_under('black')
cmap.set_bad('black')
rt_im = fits.getdata(dir + os.sep + "data_" + wavelength + os.sep +
"RT.fits.gz")
inclin_index = _find_closest(par.im_inclinations, inclination)
#print "using image %s, inc=%f" % ( str(inclin_index), par['im:inclinations'][inclin_index] )
#ax = plt.subplot(151)
image = rt_im[0, 0, inclin_index, :, :]
if vmax is None:
#image.shape = image.shape[2:] # drop leading zero-length dimensions...
vmax = image.max()
if vmin is None:
vmin = vmax / 1e8
norm = matplotlib.colors.LogNorm(vmin=vmin, vmax=vmax, clip=True)
if psf_fwhm is not None:
raise NotImplementedError("This code not yet implemented")
import optics
#psf = optics.airy_2d(aperture=10.0, wavelength=1.6e-6, pixelscale=0.020, shape=(99,99))
psf = pyfits.getdata(
'/Users/mperrin/Dropbox/AAS2013/models_pds144n/manual/keck_psf_tmp4.fits'
)
from astropy.nddata import convolve
convolved = convolve(image, psf, normalize_kernel=True)
image = convolved
if polfrac:
ax = plt.subplot(121)
ax = utils.imshow_with_mouseover(ax, image, norm=norm, cmap=cmap)
ax.set_xlabel("Offset [pix]")
ax.set_ylabel("Offset [pix]")
ax.set_title(wavelength + " $\mu$m")
if polarization == True:
# dont' show every pixel's vectors:
showevery = 5
imQ = rt_im[
1, 0,
inclin_index, :, :] * -1 #MCFOST sign convention requires flip for +Q = up
imU = rt_im[2, 0, inclin_index, :, :] * -1 #MCFOST sign convention
imQn = imQ / image
imUn = imU / image
polfrac_ar = np.sqrt(imQn**2 + imUn**2)
theta = 0.5 * np.arctan2(imUn, imQn) + np.pi / 2
vecX = polfrac_ar * np.cos(theta) * -1
vecY = polfrac_ar * np.sin(theta)
Y, X = np.indices(image.shape)
Q = plt.quiver(X[::showevery, ::showevery],
Y[::showevery, ::showevery],
vecX[::showevery, ::showevery],
vecY[::showevery, ::showevery],
headwidth=0,
headlength=0,
headaxislength=0.0,
pivot='middle',
color='white')
plt.quiverkey(Q,
0.85,
0.95,
0.5,
"50% pol.",
coordinates='axes',
labelcolor='white',
labelpos='E',
fontproperties={'size': 'small'}) #, width=0.003)
# ax = plt.subplot(152)
# ax.imshow(imQn, vmin=-1, vmax=1, cmap=matplotlib.cm.RdBu)
# ax.set_title('Q')
# ax = plt.subplot(153)
# ax.imshow(imUn, vmin=-1, vmax=1, cmap=matplotlib.cm.RdBu)
# ax.set_title('U')
# ax = plt.subplot(154)
# ax.imshow(vecX, vmin=-1, vmax=1, cmap=matplotlib.cm.RdBu)
# ax.set_title('vecX')
# ax = plt.subplot(155)
# ax.imshow(vecY, vmin=-1, vmax=1, cmap=matplotlib.cm.RdBu)
# ax.set_title('vecY')
# ax.colorbar()
#plt.colorbar()
if polfrac:
ax2 = plt.subplot(122)
cmap2 = plt.cm.gist_heat
cmap2 = plt.cm.jet
cmap2.set_over('red')
cmap2.set_under('black')
cmap2.set_bad('black')
ax2 = imshow_with_mouseover(ax2,
polfrac_ar,
vmin=0,
vmax=1,
cmap=cmap2)
ax2.set_title("Polarization fraction")
cax = plt.axes([0.92, 0.25, 0.02, 0.5])
plt.colorbar(ax2.images[0], cax=cax, orientation='vertical')
bounds = np.linspace(np.min(anom_NDEFM_speed), np.max(anom_NDEFM_speed), 20)
bounds = np.around(bounds, decimals=2)
CF = map.contourf(x,
y,
anom_NDEFM_speed[:, :],
20,
norm=MidpointNormalize(midpoint=0),
cmap=plt.cm.RdYlBu_r) #plt.cm.rainbow
cb = plt.colorbar(CF,
orientation='horizontal',
pad=0.05,
shrink=0.8,
boundaries=bounds)
cb.set_label('m/s')
Q = map.quiver(x[::2, ::2],
y[::2, ::2],
anom_NDEFM_u[::2, ::2],
anom_NDEFM_v[::2, ::2],
scale=150)
plt.quiverkey(Q, 0.93, 0.05, 10, '10 m/s')
ax.set_title('$Wind$ $Field$ $-$ $Winter$ $Anomalies$', size='15')
#map.plot(P_TT_lon, P_TT_lat, marker='D', color='w')
#map.plot(P_PP_lon, P_PP_lat, marker='D', color='w')
#map.plot(P_PN_lon, P_PN_lat, marker='D', color='w')
map.plot(TT_lon, TT_lat, marker=None, color='k')
map.plot(PP_lon, PP_lat, marker=None, color='k')
map.plot(PN_lon, PN_lat, marker=None, color='k')
map.fillcontinents(color='white')
plt.show()
def main():
# Plot diagnostics, model and pressure levels etc. to plot on for looping through
plot_type='mean'
plot_diags=['temp', 'sp_hum']
plot_levels = [925, 850, 700, 500]
#plot_levels = [925]
#experiment_ids = ['djznq', 'djzns', 'dklyu', 'dkmbq', 'dklwu', 'dklzq' ]
experiment_ids = ['dkjxq']
#experiment_id = 'djzny'
p_levels = [1000, 950, 925, 850, 700, 500, 400, 300, 250, 200, 150, 100, 70, 50, 30, 20, 10]
###### Unrotate global model data ##############################
######### Regrid to global, and difference #######
############################################################################
## Load global wind and orography
fw_global = '/nfs/a90/eepdw/Mean_State_Plot_Data/pp_files/djzn/djzny/30201_mean.pp'
fo_global = '/nfs/a90/eepdw/Mean_State_Plot_Data/pp_files/djzn/djzny/33.pp'
u_global,v_global = iris.load(fw_global)
oro_global = iris.load_cube(fo_global)
# Unrotate global coordinates
cs_glob = u_global.coord_system('CoordSystem')
cs_glob_v = v_global.coord_system('CoordSystem')
cs_glob_oro = oro_global.coord_system('CoordSystem')
lat_g = u_global.coord('grid_latitude').points
lon_g = u_global.coord('grid_longitude').points
lat_g_oro = oro_global.coord('grid_latitude').points
lon_g_oro = oro_global.coord('grid_longitude').points
if cs_glob!=cs_glob_v:
print 'Global model u and v winds have different poles of rotation'
# Unrotate global winds
if isinstance(cs_glob, iris.coord_systems.RotatedGeogCS):
print ' Global Model - Winds - djzny - Unrotate pole %s' % cs_glob
lons_g, lats_g = np.meshgrid(lon_g, lat_g)
lons_g,lats_g = iris.analysis.cartography.unrotate_pole(lons_g,lats_g, cs_glob.grid_north_pole_longitude, cs_glob.grid_north_pole_latitude)
lon_g=lons_g[0]
lat_g=lats_g[:,0]
for i, coord in enumerate (u_global.coords()):
if coord.standard_name=='grid_latitude':
lat_dim_coord_uglobal = i
if coord.standard_name=='grid_longitude':
lon_dim_coord_uglobal = i
csur_glob=cs_glob.ellipsoid
u_global.remove_coord('grid_latitude')
u_global.remove_coord('grid_longitude')
u_global.add_dim_coord(iris.coords.DimCoord(points=lat_g, standard_name='grid_latitude', units='degrees', coord_system=csur_glob), lat_dim_coord_uglobal)
u_global.add_dim_coord(iris.coords.DimCoord(points=lon_g, standard_name='grid_longitude', units='degrees', coord_system=csur_glob), lon_dim_coord_uglobal)
#print u_global
v_global.remove_coord('grid_latitude')
v_global.remove_coord('grid_longitude')
v_global.add_dim_coord(iris.coords.DimCoord(points=lat_g, standard_name='grid_latitude', units='degrees', coord_system=csur_glob), lat_dim_coord_uglobal)
v_global.add_dim_coord(iris.coords.DimCoord(points=lon_g, standard_name='grid_longitude', units='degrees', coord_system=csur_glob), lon_dim_coord_uglobal)
#print v_global
# Unrotate global model
if isinstance(cs_glob_oro, iris.coord_systems.RotatedGeogCS):
print ' Global Model - Orography - djzny - Unrotate pole %s - Winds and other diagnostics may have different number of grid points' % cs_glob_oro
lons_go, lats_go = np.meshgrid(lon_g_oro, lat_g_oro)
lons_go,lats_go = iris.analysis.cartography.unrotate_pole(lons_go,lats_go, cs_glob_oro.grid_north_pole_longitude, cs_glob_oro.grid_north_pole_latitude)
lon_g_oro=lons_go[0]
lat_g_oro=lats_go[:,0]
for i, coord in enumerate (oro_global.coords()):
if coord.standard_name=='grid_latitude':
lat_dim_coord_og = i
if coord.standard_name=='grid_longitude':
lon_dim_coord_og = i
csur_glob_oro=cs_glob_oro.ellipsoid
oro_global.remove_coord('grid_latitude')
oro_global.remove_coord('grid_longitude')
oro_global.add_dim_coord(iris.coords.DimCoord(points=lat_g_oro, standard_name='grid_latitude', units='degrees', coord_system=csur_glob_oro), lat_dim_coord_og)
oro_global.add_dim_coord(iris.coords.DimCoord(points=lon_g_oro, standard_name='grid_longitude', units='degrees', coord_system=csur_glob_oro), lon_dim_coord_og)
###############################################################################
#################### Load global heights and temp/sp_hum #####################
f_glob_h = '/nfs/a90/eepdw/Mean_State_Plot_Data/Mean_Heights_Temps_etc/408_pressure_levels_interp_pressure_djzny_%s' % (plot_type)
######################################################################################
with h5py.File(f_glob_h, 'r') as i:
mh = i['%s' % plot_type]
mean_heights_global = mh[. . .]
######################################################################################
## Loop through experiment id's ######################################################
for pl in plot_diags:
plot_diag=pl
f_glob_d = '/nfs/a90/eepdw/Mean_State_Plot_Data/Mean_Heights_Temps_etc/%s_pressure_levels_interp_djzny_%s' % (plot_diag, plot_type)
with h5py.File(f_glob_d, 'r') as i:
mg = i['%s' % plot_type]
mean_var_global = mg[. . .]
for experiment_id in experiment_ids:
expmin1 = experiment_id[:-1]
###############################################################################
#################### Load global heights and temp/sp_hum #####################
fname_h = '/nfs/a90/eepdw/Mean_State_Plot_Data/Mean_Heights_Temps_etc/408_pressure_levels_interp_pressure_%s_%s' % (experiment_id, plot_type)
fname_d = '/nfs/a90/eepdw/Mean_State_Plot_Data/Mean_Heights_Temps_etc/%s_pressure_levels_interp_%s_%s' % (plot_diag, experiment_id, plot_type)
# print fname_h
# print fname_d
# Height data file
with h5py.File(fname_h, 'r') as i:
mh = i['%s' % plot_type]
mean_heights = mh[. . .]
# print mean_heights.shape
with h5py.File(fname_d, 'r') as i:
mh = i['%s' % plot_type]
mean_var = mh[. . .]
# print mean_var.shape
f_oro = '/nfs/a90/eepdw/Mean_State_Plot_Data/pp_files/%s/%s/409.pp' % (expmin1, experiment_id)
oro = iris.load_cube(f_oro)
#print oro
for i, coord in enumerate (oro.coords()):
if coord.standard_name=='grid_latitude':
lat_dim_coord_oro = i
if coord.standard_name=='grid_longitude':
lon_dim_coord_oro = i
fu = '/nfs/a90/eepdw/Mean_State_Plot_Data/pp_files/%s/%s/30201_mean.pp' % (expmin1, experiment_id)
u_wind,v_wind = iris.load(fu)
# Wind may have different number of grid points so need to do unrotate again for wind grid points
lat_w = u_wind.coord('grid_latitude').points
lon_w = u_wind.coord('grid_longitude').points
p_levs = u_wind.coord('pressure').points
lat = oro.coord('grid_latitude').points
lon = oro.coord('grid_longitude').points
cs_w = u_wind.coord_system('CoordSystem')
cs = oro.coord_system('CoordSystem')
if isinstance(cs_w, iris.coord_systems.RotatedGeogCS):
print ' Wind - %s - Unrotate pole %s' % (experiment_id, cs_w)
lons_w, lats_w = np.meshgrid(lon_w, lat_w)
lons_w,lats_w = iris.analysis.cartography.unrotate_pole(lons_w,lats_w, cs_w.grid_north_pole_longitude, cs_w.grid_north_pole_latitude)
lon_w=lons_w[0]
lat_w=lats_w[:,0]
csur_w=cs_w.ellipsoid
for i, coord in enumerate (u_wind.coords()):
if coord.standard_name=='grid_latitude':
lat_dim_coord_uwind = i
if coord.standard_name=='grid_longitude':
lon_dim_coord_uwind = i
u_wind.remove_coord('grid_latitude')
u_wind.remove_coord('grid_longitude')
u_wind.add_dim_coord(iris.coords.DimCoord(points=lat_w, standard_name='grid_latitude', units='degrees', coord_system=csur_w),lat_dim_coord_uwind )
u_wind.add_dim_coord(iris.coords.DimCoord(points=lon_w, standard_name='grid_longitude', units='degrees', coord_system=csur_w), lon_dim_coord_uwind)
v_wind.remove_coord('grid_latitude')
v_wind.remove_coord('grid_longitude')
v_wind.add_dim_coord(iris.coords.DimCoord(points=lat_w, standard_name='grid_latitude', units='degrees', coord_system=csur_w), lat_dim_coord_uwind)
v_wind.add_dim_coord(iris.coords.DimCoord(points=lon_w, standard_name='grid_longitude', units='degrees', coord_system=csur_w),lon_dim_coord_uwind )
if isinstance(cs, iris.coord_systems.RotatedGeogCS):
print ' 409.pp - %s - Unrotate pole %s' % (experiment_id, cs)
lons, lats = np.meshgrid(lon, lat)
lon_low= np.min(lons)
lon_high = np.max(lons)
lat_low = np.min(lats)
lat_high = np.max(lats)
lon_corners, lat_corners = np.meshgrid((lon_low, lon_high), (lat_low, lat_high))
lons,lats = iris.analysis.cartography.unrotate_pole(lons,lats, cs.grid_north_pole_longitude, cs.grid_north_pole_latitude)
lon_corner_u,lat_corner_u = iris.analysis.cartography.unrotate_pole(lon_corners, lat_corners, cs.grid_north_pole_longitude, cs.grid_north_pole_latitude)
#lon_highu,lat_highu = iris.analysis.cartography.unrotate_pole(lon_high, lat_high, cs.grid_north_pole_longitude, cs.grid_north_pole_latitude)
lon=lons[0]
lat=lats[:,0]
lon_low = lon_corner_u[0,0]
lon_high = lon_corner_u[0,1]
lat_low = lat_corner_u[0,0]
lat_high = lat_corner_u[1,0]
for i, coord in enumerate (oro.coords()):
if coord.standard_name=='grid_latitude':
lat_dim_coord_oro = i
if coord.standard_name=='grid_longitude':
lon_dim_coord_oro = i
csur=cs.ellipsoid
oro.remove_coord('grid_latitude')
oro.remove_coord('grid_longitude')
oro.add_dim_coord(iris.coords.DimCoord(points=lat, standard_name='grid_latitude', units='degrees', coord_system=csur), lat_dim_coord_oro)
oro.add_dim_coord(iris.coords.DimCoord(points=lon, standard_name='grid_longitude', units='degrees', coord_system=csur), lon_dim_coord_oro)
else:
lons, lats = np.meshgrid(lon, lat)
lons_w, lats_w = np.meshgrid(lon_w, lat_w)
lon_low= np.min(lons)
lon_high = np.max(lons)
lat_low = np.min(lats)
lat_high = np.max(lats)
############## Regrid and Difference #################################
# Regrid Height and Temp/Specific humidity to global grid
h_regrid = np.empty((len(lat_g_oro), len(lon_g_oro)))
v_regrid = np.empty((len(lat_g_oro), len(lon_g_oro)))
for p in plot_levels:
### Search for pressure level match
s = np.searchsorted(p_levels[::-1], p)
h_regrid = scipy.interpolate.griddata((lats.flatten(),lons.flatten()),mean_heights[:,:,-(s+1)].flatten() , (lats_go,lons_go),method='linear')
v_regrid = scipy.interpolate.griddata((lats.flatten(),lons.flatten()),mean_var[:,:,-(s+1)].flatten() , (lats_go,lons_go),method='linear')
# Difference heights
plt_h = np.where(np.isnan(h_regrid), np.nan, h_regrid - mean_heights_global[:,:,-(s+1)])
#Difference temperature/specific humidity
plt_v = np.where(np.isnan(v_regrid), np.nan, v_regrid - mean_var_global[:,:,-(s+1)])
# Set u,v for winds, linear interpolate to approx. 2 degree grid
sc = np.searchsorted(p_levs, p)
##### Does not work on iris1.0 as on Leeds computers. Does work on later versions
#u_interp = u_wind[sc,:,:]
#v_interp = v_wind[sc,:,:].
#sample_points = [('grid_latitude', np.arange(lat_low,lat_high,2)), ('grid_longitude', np.arange(lon_low,lon_high,2))]
#u = iris.analysis.interpolate.linear(u_interp, sample_points, extrapolation_mode='linear')
#v = iris.analysis.interpolate.linear(v_interp, sample_points).data
##### Does work on Iris 1.0
# 2 degree lats lon lists for wind regridding on plot
lat_wind_1deg = np.arange(lat_low,lat_high, 2)
lon_wind_1deg = np.arange(lon_low,lon_high, 2)
### Regrid winds to global, difference, and then regrid to 2 degree spacing
fl_la_lo = (lats_w.flatten(),lons_w.flatten())
# print u_wind[sc,:,:].data.flatten().shape
u_wind_rg_to_glob = scipy.interpolate.griddata(fl_la_lo, u_wind[sc,:,:].data.flatten(), (lats_g, lons_g), method='linear')
v_wind_rg_to_glob = scipy.interpolate.griddata(fl_la_lo, v_wind[sc,:,:].data.flatten(), (lats_g, lons_g), method='linear')
u_w=u_wind_rg_to_glob-u_global[sc,:,:].data
v_w=v_wind_rg_to_glob-v_global[sc,:,:].data
#u_interp = u_wind[sc,:,:].data
#v_interp = v_wind[sc,:,:].data
lons_wi, lats_wi = np.meshgrid(lon_wind_1deg, lat_wind_1deg)
fl_la_lo = (lats_g.flatten(),lons_g.flatten())
u = scipy.interpolate.griddata(fl_la_lo, u_w.flatten(), (lats_wi, lons_wi), method='linear')
v = scipy.interpolate.griddata(fl_la_lo, v_w.flatten(), (lats_wi, lons_wi), method='linear')
#######################################################################################
### Plotting #########################################################################
#m_title = 'Height of %s-hPa level (m)' % (p)
# Set pressure height contour min/max
if p == 925:
clev_min = -24.
clev_max = 24.
elif p == 850:
clev_min = -24.
clev_max = 24.
elif p == 700:
clev_min = -24.
clev_max = 24.
elif p == 500:
clev_min = -24.
clev_max = 24.
else:
print 'Contour min/max not set for this pressure level'
# Set potential temperature min/max
if p == 925:
clevpt_min = -10.
clevpt_max = 10.
elif p == 850:
clevpt_min = -3.
clevpt_max = 3.
elif p == 700:
clevpt_min = -3.
clevpt_max = 3.
elif p == 500:
clevpt_min = -3.
clevpt_max = 3.
else:
print 'Potential temperature min/max not set for this pressure level'
# Set specific humidity min/max
if p == 925:
clevsh_min = -0.0025
clevsh_max = 0.0025
elif p == 850:
clevsh_min = -0.0025
clevsh_max = 0.0025
elif p == 700:
clevsh_min = -0.0025
clevsh_max = 0.0025
elif p == 500:
clevsh_min = -0.0025
clevsh_max = 0.0025
else:
print 'Specific humidity min/max not set for this pressure level'
#clevs_col = np.arange(clev_min, clev_max)
clevs_lin = np.linspace(clev_min, clev_max, num=24)
m =\
Basemap(llcrnrlon=lon_low,llcrnrlat=lat_low,urcrnrlon=lon_high,urcrnrlat=lat_high, rsphere = 6371229)
#x, y = m(lons, lats)
x,y = m(lons_go,lats_go)
print x.shape
x_w,y_w = m(lons_wi, lats_wi)
fig=plt.figure(figsize=(8,8))
ax = fig.add_axes([0.05,0.05,0.9,0.85], axisbg='#262626')
m.drawcoastlines(color='#262626')
m.drawcountries(color='#262626')
m.drawcoastlines(linewidth=0.5)
#m.fillcontinents(color='#CCFF99')
m.drawparallels(np.arange(-80,81,10),labels=[1,1,0,0])
m.drawmeridians(np.arange(0,360,10),labels=[0,0,0,1])
cs_lin = m.contour(x,y, plt_h, clevs_lin,colors='#262626',linewidths=0.5)
cmap=plt.cm.RdBu_r
#cmap.set_bad('#262626', 1.)
#cmap.set_over('#262626')
#cmap.set_under('#262626')
if plot_diag=='temp':
plt_v = np.ma.masked_outside(plt_v, clevpt_max+20, clevpt_min-20)
cs_col = m.contourf(x,y, plt_v, np.linspace(clevpt_min, clevpt_max), cmap=cmap, extend='both')
cbar = m.colorbar(cs_col,location='bottom',pad="5%", format = '%d')
cbar.set_ticks(np.arange(clevpt_min,clevpt_max+2,2.))
cbar.set_ticklabels(np.arange(clevpt_min,clevpt_max+2,2.))
cbar.set_label('K')
plt.suptitle('Difference from global model (Model - global ) of Height, Potential Temperature and Wind Vectors at %s hPa'% (p), fontsize=10)
elif plot_diag=='sp_hum':
plt_v = np.ma.masked_outside(plt_v, clevsh_max+20, clevsh_min-20)
cs_col = m.contourf(x,y, plt_v, np.linspace(clevsh_min, clevsh_max), cmap=cmap, extend='both')
cbar = m.colorbar(cs_col,location='bottom',pad="5%", format = '%.3f')
cbar.set_label('kg/kg')
plt.suptitle('Difference from global model (Model - Global Model ) of Height, Specific Humidity and Wind Vectors at %s hPa'% (p), fontsize=10)
wind = m.quiver(x_w,y_w, u, v, scale=150,color='#262626' )
qk = plt.quiverkey(wind, 0.1, 0.1, 5, '5 m/s', labelpos='W')
plt.clabel(cs_lin, fontsize=10, fmt='%d', color='black')
#plt.title('%s\n%s' % (m_title, model_name_convert_title.main(experiment_id)), fontsize=10)
plt.title('\n'.join(wrap('%s' % (model_name_convert_title.main(experiment_id)), 80)), fontsize=10)
#plt.show()
if not os.path.exists('/nfs/a90/eepdw/Mean_State_Plot_Data/Figures/%s/%s' % (experiment_id, plot_diag)): os.makedirs('/nfs/a90/eepdw/Mean_State_Plot_Data/Figures/%s/%s' % (experiment_id, plot_diag))
plt.savefig('/nfs/a90/eepdw/Mean_State_Plot_Data/Figures/%s/%s/geop_height_difference_120LAM_%shPa_%s_%s.png' % (experiment_id, plot_diag, p, experiment_id, plot_diag), format='png', bbox_inches='tight')
def plot_timeseries(dat, met, float):
f, ax = plt.subplots(6, 1, sharex=True)
if float != '7782b':
met = met.sel(floatid=float)
met['tau'] = np.sqrt(met.tx**2 + met.ty**2)
met.tx.plot(ax=ax[0], label=r'$\tau_x$')
met.ty.plot(ax=ax[0], label=r'$\tau_y$')
met.tau.plot(ax=ax[0], label=r'$\tau$')
ax[0].legend()
ax[0].set_xlabel(None)
ax[0].set_ylabel(r'wind stress [Nm$-2$]')
met = met.resample(time='9h', skipna=True).mean()
quiveropts = dict(headlength=0,
headwidth=1,
scale_units='y',
scale=1,
color='k')
qv = ax[1].quiver(met.time.values, np.zeros(met.time.shape), met.tx, met.ty,met.tau,
**quiveropts)
plt.quiverkey(qv, 0.9, 0.8, 0.5, '0.5 Nm$^{-2}$', coordinates='axes')
ax[1].set_xlabel(None)
ax[1].set_ylabel(r'wind stress vectors')
ax[1].set_ylim(-1,1)
dat.mld.plot(ax=ax[2], label=r'mld (0.03kgm$^{-3}$ from $\rho_{10m}$)')
ax[2].legend()
ax[2].set_xlabel(None)
ax[2].set_ylabel('Mixed layer depth [m]')
dat.hke.plot(ax=ax[3],marker='.',lw=0, label='total hke')
dat.hke_lowpass.plot(ax=ax[3],marker='.',lw=0, label='lowpass hke')
dat.hke_resid.plot(ax=ax[3], label='resid hke')
dat.hke_ni.plot(ax=ax[3], label='ni hke')
ax[3].legend()
ax[3].set_xlabel(None)
ax[3].set_ylabel('HKE [m$^2$s$^2$]')
dat.dHKEdt_total.pipe(np.abs).pipe(np.log10).plot(ax=ax[4],
lw=0,
marker='.',
label='total dhke/dt')
dat.dHKEdt_lowpass.pipe(np.abs).pipe(np.log10).plot(ax=ax[4],
lw=0,
marker='.',
label='lowpass dhke/dt')
dat.dHKEdt_resid.pipe(np.abs).pipe(np.log10).plot(ax=ax[4],
marker='.',
label='resid dhke/dt')
dat.dHKEdt_ni.pipe(np.abs).pipe(np.log10).plot(ax=ax[4],
marker='.',
label='ni dhke/dt')
ax[4].legend()
ax[4].set_xlabel(None)
ax[4].set_ylabel(r'$\frac{\partial HKE}{\partial t}$ [m$^2$s$^3$]')
dat.eps.pipe(np.abs).pipe(np.log10).plot(ax=ax[5],
marker='.',
lw=0.1,
label=r'$log_{10}(\epsilon)$')
# ax[7].set_ylim(-8,0)
ax[5].legend()
ax[5].set_xlabel(None)
ax[5].set_ylabel(r'$\epsilon$ [m$^2$s$^3$]')
ax[-1].set_xlim(dat.mld.time.values.min(), dat.mld.time.values.max())
plt.tight_layout()
plt.subplots_adjust(hspace=0.1)
plt.savefig(f'figures/storms/nov152017/{float:s}.pdf')
plt.close()
def plot_uv(ds, grd, block=2):
# Radius of the Earth in metres
r = 6.371e6
# Degrees to radians conversion factor
deg2rad = np.pi / 180
# Side length of blocks to average vectors over (can't plot vector at every
# single point or the plot will be way too crowded)
lon = grd.lon_rho.values
lat = grd.lat_rho.values
u = ds.ubar.values
v = ds.vbar.values
angle = np.zeros(np.shape(lon))
u_rho, v_rho = rotate_vector_roms(u, v, angle)
speed = np.sqrt(np.square(u_rho) + np.square(v_rho))
#print('initialize and fill up the arrays')
numy = np.size(lon, 0) #530
numx = np.size(lon, 1) #630
x = np.arange(numx)
y = np.arange(numy)
xmesh, ymesh = np.meshgrid(x, y)
#print(numx,numy,x,y)
# Average x, y, u_circ, and v_circ over block x block intervals
# Calculate number of blocks
size0 = int(np.ceil(numy / float(block)))
size1 = int(np.ceil(numx / float(block)))
# Set up arrays for averaged fields
x_block = np.ma.empty([size0, size1])
y_block = np.ma.empty([size0, size1])
u_block = np.ma.empty([size0, size1])
v_block = np.ma.empty([size0, size1])
# Set up arrays containing boundary indices
posn0 = list(np.arange(0, numy, block))
posn0.append(numy)
posn1 = list(np.arange(0, numx, block))
posn1.append(numx)
#print(posn0,posn1)
# Double loop to average each block (can't find a more efficient way to do
# this)
for j in np.arange(size0):
for i in np.arange(size1):
start0 = posn0[j]
end0 = posn0[j + 1]
start1 = posn1[i]
end1 = posn1[i + 1]
x_block[j, i] = np.mean(xmesh[start0:end0, start1:end1])
y_block[j, i] = np.mean(ymesh[start0:end0, start1:end1])
u_block[j, i] = np.mean(u_rho[start0:end0, start1:end1])
v_block[j, i] = np.mean(v_rho[start0:end0, start1:end1])
# Make the plot
fig, ax0 = plt.subplots(1, figsize=(15, 10))
speedP = ax0.pcolormesh(xmesh,
ymesh,
speed * 100,
vmin=0,
vmax=10,
cmap=cmo.speed)
plt.colorbar(speedP, ax=ax0)
# Add vectors for each block
quiverP = ax0.quiver(x_block,
y_block,
u_block,
v_block,
pivot="mid",
color='black',
scale_units='xy',
scale=0.01)
plt.quiverkey(quiverP,
0.75,
0.99,
0.1,
r'$10 \frac{cm}{s}$',
labelpos='E',
coordinates='figure')
ax0.set_title('Mean barotropic velocity (cm/s)', fontsize=16)
ax0.set_aspect('equal')
ax0.axis('off')
print('test')
return fig
def plotear(lllat,
urlat,
lllon,
urlon,
dist_lat,
dist_lon,
Lon,
Lat,
mapa,
bar_min,
bar_max,
unds,
titulo,
path,
C_T='k',
wind=False,
mapa_u=None,
mapa_v=None):
# lllat (low-left-lat) : float con la latitud de la esquina inferior izquierda
# urlat (uper-right-lat) : float con la latitud de la esquina superior derecha
# lllon (low-left-lon) : float con la longitud de la esquina inferior izquierda en coordenas negativas este
# urlon (uper-right-lon) : float con la longitud de la esquina superior derecha en coordenas negativas este
# dist_lat : entero que indica cada cuanto dibujar las lineas de los paralelos
# dist_lon : entero que indica cada cuanto dibujar las lineas de los meridianos
# Lon : array de numpy con las longitudes del mapa a plotearse en coordenadas negativas este
# Lat : array de numpy con las longitudes del mapa a plotearse
# mapa : array de numpy 2D a plotearse con contourf
# bar_min : mínimo valor del mapa a plotearse
# bar_max : máximo valor del mapa a plotearse
# unds : string de las unidades de la variable que se va a plotear
# titulo : string del titulo que llevará el mapa
# path : 'string de la dirección y el nombre del archivo que contendrá la figura a generarse'
# wind : boolean que diga si se quiere pintar flechas de viento (corrientes), donde True es que sí se va a hacer
# mapa_u : array de numpay 2D con la componente en x de la velocidad y que será utilizado para pintar las flechas. Este tomara algun valor siempre y cuando wind=True
# mapa_v : array de numpay 2D con la componente en y de la velocidad y que será utilizado para pintar las flechas. Este tomara algun valor siempre y cuando wind=True
# return : gráfica o mapa
fig = plt.figure(figsize=(8, 8), edgecolor='W', facecolor='W')
ax = fig.add_axes([0.1, 0.1, 0.8, 0.8])
map = Basemap(projection='merc',
llcrnrlat=lllat,
urcrnrlat=urlat,
llcrnrlon=lllon,
urcrnrlon=urlon,
resolution='i')
map.drawcoastlines(linewidth=0.8)
map.drawcountries(linewidth=0.8)
map.drawparallels(np.arange(lllat, urlat, dist_lat), labels=[1, 0, 0, 1])
map.drawmeridians(np.arange(lllon, urlon, dist_lon), labels=[1, 0, 0, 1])
lons, lats = np.meshgrid(Lon, Lat)
x, y = map(lons, lats)
bounds = np.linspace(bar_min, bar_max, 20)
bounds = np.around(bounds, decimals=2)
if wind == False:
CF1 = map.contourf(x,
y,
mapa,
20,
norm=MidpointNormalize(midpoint=0),
cmap=plt.cm.viridis,
levels=bounds,
extend='max') #plt.cm.rainbow , plt.cm.RdYlBu_r
CF2 = map.contourf(x,
y,
mapa,
20,
norm=MidpointNormalize(midpoint=0),
cmap=plt.cm.viridis,
levels=bounds,
extend='min') #plt.cm.rainbow, plt.cm.RdYlBu_r
else:
CF1 = map.contourf(x,
y,
mapa,
20,
cmap=plt.cm.rainbow,
levels=bounds,
extend='max') #plt.cm.rainbow , plt.cm.RdYlBu_r
CF2 = map.contourf(x,
y,
mapa,
20,
cmap=plt.cm.rainbow,
levels=bounds,
extend='min') #plt.cm.rainbow, plt.cm.RdYlBu_r
cb1 = plt.colorbar(CF1,
orientation='horizontal',
pad=0.05,
shrink=0.8,
boundaries=bounds)
cb1.set_label(unds)
ax.set_title(titulo, size='15', color=C_T)
if wind == True:
Q = map.quiver(x[::2, ::2],
y[::2, ::2],
mapa_u[::2, ::2],
mapa_v[::2, ::2],
scale=20)
plt.quiverkey(Q, 0.93, 0.05, 2, '2 m/s')
#map.fillcontinents(color='white')
plt.savefig(path + '.png', bbox_inches='tight', dpi=300)
plt.close('all')
def corr_box():
srfc = cnst.ERA_MONTHLY_SRFC_SYNOP
pl = cnst.ERA_MONTHLY_PL_SYNOP
mcs = cnst.GRIDSAT + 'aggs/gridsat_WA_-65_monthly_count_-40base_15-21UTC_1000km2.nc' # -70count
fpath = cnst.network_data + 'figs/CLOVER/months/'
dicm = pkl.load(
open(
cnst.network_data + 'data/CLOVER/saves/storm_frac_synop12UTC_SA.p',
'rb'))
dicmean = pkl.load(
open(
cnst.network_data +
'data/CLOVER/saves/storm_frac_mean_synop12UTC_SA.p', 'rb'))
# mcsbox = cnst.GRIDSAT + 'aggs/SAboxWest_meanT-40_1000km2.nc' # box_13W-13E-4-8N_meanT-50_from5000km2.nc'
# mcs_temp = xr.open_dataset(mcsbox)
# mcs_temp = mcs_temp['tir']
box = [5, 55, -36, 0] #[-18,55,-35,35]#[-10,55,-35,0]
da = xr.open_dataset(pl)
da = u_darrays.flip_lat(da)
da = da.sel(longitude=slice(box[0], box[1]),
latitude=slice(box[2], box[3])) # latitude=slice(36, -37))
da2 = xr.open_dataset(srfc)
da2 = u_darrays.flip_lat(da2)
da2 = da2.sel(longitude=slice(box[0], box[1]),
latitude=slice(box[2], box[3])) # latitude=slice(36, -37))
da3 = xr.open_dataset(mcs)
da3 = da3.sel(lon=slice(box[0], box[1]), lat=slice(box[2], box[3]))
lons = da.longitude
lats = da.latitude
press = da2['sp']
press = press[press['time.hour'] == 12]
press.values = press.values * 1000
low_press = 850
up_press = 550
q = da['q'].sel(level=slice(low_press - 50, low_press)).mean('level')
q = q[q['time.hour'] == 12]
t2d = da2['t2m'] #['t2m']
#t2d = da['t'].sel(level=slice(800, 850)).mean('level')
t2d = t2d[t2d['time.hour'] == 12]
u600 = da['u'].sel(level=slice(up_press - 50, up_press)).mean('level')
u600 = u600[u600['time.hour'] == 12]
v600 = da['v'].sel(level=slice(up_press - 50, up_press)).mean('level')
v600 = v600[v600['time.hour'] == 12]
ws600 = u_met.u_v_to_ws_wd(u600, v600)
u800 = da['u'].sel(level=slice(low_press - 50, low_press)).mean('level')
u800 = u800[u800['time.hour'] == 12]
v800 = da['v'].sel(level=slice(low_press - 50, low_press)).mean('level')
v800 = v800[v800['time.hour'] == 12]
shear_u = u600 - u800 #u600-
shear_v = v600 - v800 # v600-
ws_shear = u_met.u_v_to_ws_wd(shear_u.values, shear_v.values)
ws_600 = t2d.copy(deep=True)
ws_600.name = 'ws'
ws_600.values = ws600[0]
shear = t2d.copy(deep=True)
shear.name = 'shear'
shear.values = ws_shear[0]
q.values = q.values * 1000
tir = da3['tir']
tir = t2d.salem.lookup_transform(tir)
def array_juggling(data, month, hour=None):
m = month
if hour is not None:
if len(month) > 1:
data = data[((data['time.month'] >= month[0])
| (data['time.month'] <= month[1]))
& (data['time.hour'] == hour) &
(data['time.year'] >= 1983) &
(data['time.year'] <= 2017)]
else:
data = data[(data['time.month'] == month[0])
& (data['time.hour'] == hour) &
(data['time.year'] >= 1983) &
(data['time.year'] <= 2017)]
else:
if len(month) > 1:
data = data[((data['time.month'] >= month[0])
| (data['time.month'] <= month[1]))
& (data['time.year'] >= 1983) &
(data['time.year'] <= 2017)]
else:
data = data[(data['time.month'] == month[0])
& (data['time.year'] >= 1983) &
(data['time.year'] <= 2017)]
data_years = data.groupby('time.year').mean(axis=0)
data_mean = data.mean(axis=0)
# diff = xr.DataArray(data_years.values[1::, :, :] - data_years.values[0:-1, :, :],
# coords=[data_years.year[1::], data.latitude, data.longitude], dims=['year','latitude', 'longitude'] )
diff = xr.DataArray(
data_years.values,
coords=[data_years.year, data.latitude, data.longitude],
dims=['year', 'latitude', 'longitude'])
# unstack back to lat lon coordinates
return diff, data_mean
def corr(a, b, bsingle=None, c_box=None):
ds = xr.Dataset()
ds['pval'] = a.copy(deep=True).sum('year') * np.nan
ds['r'] = a.copy(deep=True).sum('year') * np.nan
ds['slope'] = a.copy(deep=True).sum('year') * np.nan
corr_box = c_box
if bsingle:
bb = b
else:
bb = b.sel(latitude=slice(corr_box[2], corr_box[3]),
longitude=slice(
corr_box[0],
corr_box[1])).mean(dim=['latitude', 'longitude'])
for lat in a.latitude.values:
for lon in a.longitude.values:
aa = a.sel(latitude=lat, longitude=lon)
if bsingle:
r, p = stats.pearsonr(aa.values, bb)
pf = np.polyfit(aa.values, bb, 1)
else:
r, p = stats.pearsonr(aa.values, bb.values)
pf = np.polyfit(aa.values, bb.values, 1)
slope = pf[0]
if (np.nansum(aa.values == 0) >= 10):
p = np.nan
r = np.nan
ds['r'].loc[{'latitude': lat, 'longitude': lon}] = r
ds['pval'].loc[{'latitude': lat, 'longitude': lon}] = p
ds['slope'].loc[{'latitude': lat, 'longitude': lon}] = slope
return ds
box_dic = {
1: [16, 30, -25, -20],
2: [12, 28, -10, 3],
3: [16, 25, -23, -18],
4: [16, 25, -23, -18],
10: [14, 28, -15, -5],
11: [16, 30, -20, -10],
12: [16, 30, -22, -12],
(11, 1): [18, 30, -23, -18]
}
months = [(11, 1), 2, 3, 10]
for m in months:
c_box = box_dic[m]
if type(m) == int:
m = [m]
t2diff, t2year = array_juggling(t2d, m) #
qdiff, qyear = array_juggling(q, m) #, hour=12
shdiff, sheyear = array_juggling(shear, m) #, hour=12
vdiff, vyear = array_juggling(v800, m) # , hour=12
udiff, uyear = array_juggling(u800, m) # , hour=12
tirdiff, tiryear = array_juggling(tir, m) # average frequency change
#mcs_month = mcs_temp[mcs_temp['time.month'] == m] # meanT box average change
#tirdiff = mcs_month.values[1::]-mcs_month.values[0:-1]
bs = False
try:
qcorr = corr(qdiff, tirdiff, bsingle=bs, c_box=c_box)
except:
continue
shearcorr = corr(shdiff, tirdiff, bsingle=bs, c_box=c_box)
tcorr = corr(t2diff, tirdiff, bsingle=bs, c_box=c_box)
dicm[m[0]].values[dicm[m[0]].values == 0] = np.nan
print('plot')
if len(m) == 1:
fp = fpath + 'corr_mid_-70C_synop_-50base_linear_850T' + str(
m[0]).zfill(2) + '.png'
else:
fp = fpath + 'corr_mid_-70C_synop_-50base_linear_850T' + str(
m[0]).zfill(2) + '-' + str(m[1]).zfill(2) + '.png'
map = shear.salem.get_map()
xx, yy = map.grid.transform(shear.longitude.values,
shear.latitude.values,
crs=shear.salem.grid.proj)
xx, yy = np.meshgrid(xx, yy)
# Quiver only every 7th grid point
u = uyear.values[1::2, 1::2]
v = vyear.values[1::2, 1::2]
xx = xx[1::2, 1::2]
yy = yy[1::2, 1::2]
#ipdb.set_trace()
f = plt.figure(figsize=(15, 8), dpi=350)
ax1 = f.add_subplot(221)
map.set_data(tcorr['r'], interp='linear') # interp='linear'
map.set_contour(t2year - 273.15,
interp='linear',
levels=np.arange(24, 37, 4),
colors='k',
linewidths=0.5)
map.set_plot_params(
cmap='RdBu_r',
extend='both',
levels=[-0.7, -0.6, -0.5, -0.4, -0.3, 0.3, 0.4, 0.5, 0.6,
0.7]) # levels=np.arange(-0.5,0.51,0.1),
dic = map.visualize(ax=ax1,
title='2m temperature corr. | contours: mean T',
cbar_title='K decade-1')
contours = dic['contour'][0]
plt.clabel(contours, inline=True, fontsize=7, fmt='%1.1f')
ax2 = f.add_subplot(222)
map.set_data(qcorr['r'], interp='linear') # interp='linear'
map.set_contour(qyear,
interp='linear',
levels=np.arange(5, 19, 3),
colors='k',
linewidths=0.5)
map.set_plot_params(
cmap='RdBu_r',
extend='both',
levels=[-0.7, -0.6, -0.5, -0.4, -0.3, 0.3, 0.4, 0.5, 0.6,
0.7]) # levels=np.arange(-0.5,0.51,0.1),
dic = map.visualize(
ax=ax2,
title='800hPa Spec. humidity corr. | contours: mean q',
cbar_title='g kg-1 decade-1')
contours = dic['contour'][0]
plt.clabel(contours, inline=True, fontsize=7, fmt='%1.1f')
ax3 = f.add_subplot(223)
# map.set_data(shearcorr['r'], interp='linear') # interp='linear'
# map.set_plot_params(cmap='RdBu_r', extend='both', levels=[-0.7,-0.6,-0.5,-0.4, -0.3,0.3,0.4,0.5,0.6,0.7])
#map.set_contour(sheyear, interp='linear', levels=np.arange(-10,1,6), colors='k', linewidths=0.5)
map.set_data(tcorr['r'], interp='linear') # interp='linear'
map.set_plot_params(
cmap='RdBu_r',
extend='both',
levels=[-0.7, -0.6, -0.5, -0.4, -0.3, 0.3, 0.4, 0.5, 0.6, 0.7])
qu = ax3.quiver(xx, yy, u, v, scale=50, width=0.002)
qk = plt.quiverkey(qu,
0.4,
0.03,
4,
'4 m s$^{-1}$',
labelpos='E',
coordinates='figure')
# levels=np.arange(-0.5,0.51,0.1)
dic = map.visualize(
ax=ax3,
title='800-500hPa wind shear corr., mean 500hPa wind vectors',
cbar_title='m s-1 decade-1')
contours = dic['contour'][0]
plt.clabel(contours, inline=True, fontsize=7, fmt='%1.1f')
ax4 = f.add_subplot(224)
map.set_contour(dicmean[m[0]],
interp='linear',
levels=[0.1, 0.5, 1, 2.5],
colors='k',
linewidths=0.5)
map.set_data(dicm[m[0]]) #
#ax4.axhspan(-26,18) #[15,25,-26,-18]
coord = c_box #[17, 25, -28, -22]
geom = shpg.box(coord[0], coord[2], coord[1], coord[3])
map.set_geometry(geom,
zorder=99,
color='darkorange',
linewidth=3,
linestyle='--',
alpha=0.3)
# ax4.axvline(x=25, ymin=-26, ymax=-18)
# ax4.axhline(y=-26, xmin=15, xmax=25)
# ax4.axhline(y=-18, xmin=15, xmax=25)
map.set_plot_params(
cmap='viridis', extend='both', levels=np.arange(
10, 41,
10)) # levels=np.arange(20,101,20) #np.arange(20,101,20)
dic = map.visualize(ax=ax4,
title='-65C cloud cover change | >1000km2 -40C',
cbar_title='$\%$ decade-1')
contours = dic['contour'][0]
plt.clabel(contours, inline=True, fontsize=7, fmt='%1.1f')
plt.tight_layout()
plt.savefig(fp)
plt.close('all')
def plot(self):
if self.filetype == 'geotiff':
f, fname = tempfile.mkstemp()
os.close(f)
driver = gdal.GetDriverByName('GTiff')
outRaster = driver.Create(fname, self.latitude.shape[1],
self.longitude.shape[0], 1,
gdal.GDT_Float64)
x = [self.longitude[0, 0], self.longitude[-1, -1]]
y = [self.latitude[0, 0], self.latitude[-1, -1]]
outRasterSRS = osr.SpatialReference()
x, y = self.basemap(x, y)
outRasterSRS.ImportFromProj4(self.basemap.proj4string)
pixelWidth = (x[-1] - x[0]) / self.longitude.shape[0]
pixelHeight = (y[-1] - y[0]) / self.latitude.shape[0]
outRaster.SetGeoTransform(
(x[0], pixelWidth, 0, y[0], 0, pixelHeight))
outband = outRaster.GetRasterBand(1)
d = self.data.astype("Float64")
ndv = d.fill_value
outband.WriteArray(d.filled(ndv))
outband.SetNoDataValue(ndv)
outRaster.SetProjection(outRasterSRS.ExportToWkt())
outband.FlushCache()
outRaster = None
with open(fname, 'r', encoding="latin-1") as f:
buf = f.read()
os.remove(fname)
return (buf, self.mime, self.filename.replace(".geotiff", ".tif"))
# Figure size
figuresize = list(map(float, self.size.split("x")))
fig = plt.figure(figsize=figuresize, dpi=self.dpi)
ax = plt.gca()
if self.scale:
vmin = self.scale[0]
vmax = self.scale[1]
else:
vmin = np.amin(self.data)
vmax = np.amax(self.data)
if self.compare:
vmax = max(abs(vmax), abs(vmin))
vmin = -vmax
c = self.basemap.imshow(self.data,
vmin=vmin,
vmax=vmax,
cmap=self.cmap)
if len(self.quiver_data) == 2:
qx, qy = self.quiver_data
qx, qy, x, y = self.basemap.rotate_vector(qx,
qy,
self.quiver_longitude,
self.quiver_latitude,
returnxy=True)
quiver_mag = np.sqrt(qx**2 + qy**2)
if self.quiver['magnitude'] != 'length':
qx = qx / quiver_mag
qy = qy / quiver_mag
qscale = 50
else:
qscale = None
if self.quiver['magnitude'] == 'color':
if self.quiver['colormap'] is None or \
self.quiver['colormap'] == 'default':
qcmap = colormap.colormaps.get('speed')
else:
qcmap = colormap.colormaps.get(self.quiver['colormap'])
q = self.basemap.quiver(
x,
y,
qx,
qy,
quiver_mag,
width=0.0035,
headaxislength=4,
headlength=4,
scale=qscale,
pivot='mid',
cmap=qcmap,
)
else:
q = self.basemap.quiver(
x,
y,
qx,
qy,
width=0.0025,
headaxislength=4,
headlength=4,
scale=qscale,
pivot='mid',
)
if self.quiver['magnitude'] == 'length':
unit_length = np.mean(quiver_mag) * 2
unit_length = np.round(unit_length,
-int(np.floor(np.log10(unit_length))))
if unit_length >= 1:
unit_length = int(unit_length)
plt.quiverkey(q,
.65,
.01,
unit_length,
self.quiver_name.title() + " " +
str(unit_length) + " " +
utils.mathtext(self.quiver_unit),
coordinates='figure',
labelpos='E')
if self.show_bathymetry:
# Plot bathymetry on top
cs = self.basemap.contour(
self.longitude,
self.latitude,
self.bathymetry,
latlon=True,
linewidths=0.5,
norm=LogNorm(vmin=1, vmax=6000),
cmap=mcolors.LinearSegmentedColormap.from_list(
'transparent_gray', [(0, 0, 0, 0.5), (0, 0, 0, 0.1)]),
levels=[100, 200, 500, 1000, 2000, 3000, 4000, 5000, 6000])
plt.clabel(cs, fontsize='xx-small', fmt='%1.0fm')
if self.area and self.show_area:
for a in self.area:
polys = []
for co in a['polygons'] + a['innerrings']:
coords = np.array(co).transpose()
mx, my = self.basemap(coords[1], coords[0])
map_coords = list(zip(mx, my))
polys.append(Polygon(map_coords))
paths = []
for poly in polys:
paths.append(poly.get_path())
path = concatenate_paths(paths)
poly = PathPatch(path,
fill=None,
edgecolor='#ffffff',
linewidth=5)
plt.gca().add_patch(poly)
poly = PathPatch(path, fill=None, edgecolor='k', linewidth=2)
plt.gca().add_patch(poly)
if self.names is not None and len(self.names) > 1:
for idx, name in enumerate(self.names):
x, y = self.basemap(self.centroids[idx].y,
self.centroids[idx].x)
plt.annotate(
xy=(x, y),
s=name,
ha='center',
va='center',
size=12,
# weight='bold'
)
if len(self.contour_data) > 0:
if (self.contour_data[0].min() != self.contour_data[0].max()):
cmin, cmax = utils.normalize_scale(self.contour_data[0],
self.contour_name,
self.contour_unit)
levels = None
if self.contour.get('levels') is not None and \
self.contour['levels'] != 'auto' and \
self.contour['levels'] != '':
try:
levels = list(
set([
float(xx)
for xx in self.contour['levels'].split(",")
if xx.strip()
]))
levels.sort()
except ValueError:
pass
if levels is None:
levels = np.linspace(cmin, cmax, 5)
cmap = self.contour['colormap']
if cmap is not None:
cmap = colormap.colormaps.get(cmap)
if cmap is None:
cmap = colormap.find_colormap(self.contour_name)
if not self.contour.get('hatch'):
contours = self.basemap.contour(self.longitude,
self.latitude,
self.contour_data[0],
latlon=True,
linewidths=2,
levels=levels,
cmap=cmap)
else:
hatches = [
'//', 'xx', '\\\\', '--', '||', '..', 'oo', '**'
]
if len(levels) + 1 < len(hatches):
hatches = hatches[0:len(levels) + 2]
self.basemap.contour(self.longitude,
self.latitude,
self.contour_data[0],
latlon=True,
linewidths=1,
levels=levels,
colors='k')
contours = self.basemap.contourf(self.longitude,
self.latitude,
self.contour_data[0],
latlon=True,
colors=['none'],
levels=levels,
hatches=hatches,
vmin=cmin,
vmax=cmax,
extend='both')
if self.contour['legend']:
handles, l = contours.legend_elements()
labels = []
for i, lab in enumerate(l):
if self.contour.get('hatch'):
if self.contour_unit == 'fraction':
if i == 0:
labels.append(
"$x \\leq {0: .0f}\\%$".format(
levels[i] * 100))
elif i == len(levels):
labels.append("$x > {0: .0f}\\%$".format(
levels[i - 1] * 100))
else:
labels.append(
"${0:.0f}\\% < x \\leq {1:.0f}\\%$".
format(levels[i - 1] * 100,
levels[i] * 100))
else:
if i == 0:
labels.append("$x \\leq %.3g$" % levels[i])
elif i == len(levels):
labels.append("$x > %.3g$" % levels[i - 1])
else:
labels.append("$%.3g < x \\leq %.3g$" %
(levels[i - 1], levels[i]))
else:
if self.contour_unit == 'fraction':
labels.append("{0:.0%}".format(levels[i]))
else:
labels.append(
"%.3g %s" %
(levels[i],
utils.mathtext(self.contour_unit)))
ax = plt.gca()
if self.contour_unit != 'fraction' and not \
self.contour.get('hatch'):
contour_title = "%s (%s)" % (self.contour_name,
utils.mathtext(
self.contour_unit))
else:
contour_title = self.contour_name
leg = ax.legend(handles[::-1],
labels[::-1],
loc='lower left',
fontsize='medium',
frameon=True,
framealpha=0.75,
title=contour_title)
leg.get_title().set_fontsize('medium')
if not self.contour.get('hatch'):
for legobj in leg.legendHandles:
legobj.set_linewidth(3)
# Map Info
self.basemap.drawmapboundary(fill_color=(0.3, 0.3, 0.3), zorder=-1)
self.basemap.drawcoastlines(linewidth=0.5)
self.basemap.fillcontinents(color='grey', lake_color='dimgrey')
def find_lines(values):
if np.amax(values) - np.amin(values) < 1:
return [values.mean()]
elif np.amax(values) - np.amin(values) < 25:
return np.round(
np.arange(np.amin(values), np.amax(values),
round(np.amax(values) - np.amin(values)) / 5))
else:
return np.arange(round(np.amin(values), -1),
round(np.amax(values), -1), 5)
parallels = find_lines(self.latitude)
meridians = find_lines(self.longitude)
self.basemap.drawparallels(parallels,
labels=[1, 0, 0, 0],
color=(0, 0, 0, 0.5))
self.basemap.drawmeridians(meridians,
labels=[0, 0, 0, 1],
color=(0, 0, 0, 0.5),
latmax=85)
title = self.plotTitle
if self.plotTitle is None or self.plotTitle == "":
area_title = "\n".join(wrap(", ".join(self.names), 60)) + "\n"
title = "%s %s %s, %s" % (area_title, self.variable_name.title(),
self.depth_label,
self.date_formatter(self.timestamp))
plt.title(title.strip())
ax = plt.gca()
divider = make_axes_locatable(ax)
cax = divider.append_axes("right", size="5%", pad=0.05)
bar = plt.colorbar(c, cax=cax)
bar.set_label(
"%s (%s)" %
(self.variable_name.title(), utils.mathtext(self.variable_unit)),
fontsize=14)
if self.quiver is not None and \
self.quiver['variable'] != '' and \
self.quiver['variable'] != 'none' and \
self.quiver['magnitude'] == 'color':
bax = divider.append_axes("bottom", size="5%", pad=0.35)
qbar = plt.colorbar(q, orientation='horizontal', cax=bax)
qbar.set_label(self.quiver_name.title() + " " +
utils.mathtext(self.quiver_unit),
fontsize=14)
fig.tight_layout(pad=3, w_pad=4)
return super(MapPlotter, self).plot(fig)
index.append(i) #November index
uc = u[index[yr]][0][:] #surface layer 0 eastward flow
vc = v[index[yr]][0][:] #surface layer 0 northward flow
uwse = uws[index[yr]][:] #eastward windstress
vwsn = vws[index[yr]][:] #northward windstress
xi = np.arange(gbox[0], gbox[1], gridscale) #region of interest
yi = np.arange(gbox[2], gbox[3], gridscale)
xb, yb, ub_mean, ub_median, ub_std, ub_num = sh_bindata(lonc, latc, uc, xi, yi)
xb, yb, vb_mean, vb_median, vb_std, vb_num = sh_bindata(lonc, latc, vc, xi, yi)
xxb, yyb = np.meshgrid(xb, yb)
fig = plt.figure()
ax1 = fig.add_subplot(211, aspect=1.3)
Q = plt.quiver(xxb, yyb, ub_mean.T, vb_mean.T, scale=3.) #current vectors
qk = plt.quiverkey(Q,
0.7,
0.12,
.1,
r'$.1m/s$',
fontproperties={'weight': 'bold'})
ax1.plot(CL['lon'], CL['lat'])
ax1.set_xlim([gbox[0], gbox[1]])
ax1.set_ylim([gbox[2], gbox[3]])
ax1.set_title(str(2014 + yr) + ' mean surface current')
ax1.set_xticklabels('', visible=False) # shut off xticklabels
xb, yb, uw_mean, uw_median, uw_std, uw_num = sh_bindata(
lonc, latc, uwse, xi, yi)
xb, yb, vw_mean, vw_median, vw_std, vw_num = sh_bindata(
lonc, latc, vwsn, xi, yi)
ax2 = fig.add_subplot(212, aspect=1.3)
Q = plt.quiver(xxb, yyb, uw_mean.T, vw_mean.T, scale=3.) # wind stress vectors
qk = plt.quiverkey(Q,
0.7,
df.tail()
Let's take a look at our fake data.
%matplotlib inline
import matplotlib.pyplot as plt
from oceans.plotting import stick_plot
q = stick_plot([t.to_pydatetime() for t in df["time"]], df["u"], df["v"])
ref = 1
qk = plt.quiverkey(
q, 0.1, 0.85, ref, f"{ref} m s$^{-1}$", labelpos="N", coordinates="axes"
)
plt.xticks(rotation=70)
`pocean.dsg` is relatively simple to use. The user must provide a DataFrame, like the one above, and a dictionary of attributes that maps to the data and adhere to the DSG conventions desired.
Because we want the file to work seamlessly with ERDDAP we also added some ERDDAP specific attributes like `cdm_timeseries_variables`, and `subsetVariables`.
attributes = {
"global": {
"title": "Fake mooring",
"summary": "Vector current meter ADCP @ 10 m",
"institution": "Restaurant at the end of the universe",
"cdm_timeseries_variables": "station",
"subsetVariables": "depth",
# create a figure, add an axes.
fig = plt.figure(figsize=(8, 8))
ax = fig.add_axes([0.1, 0.1, 0.7, 0.7])
# rotate wind vectors to map projection coordinates.
# (also compute native map projections coordinates of lat/lon grid)
# only do Northern Hemisphere.
urot, vrot, x, y = m.rotate_vector(u[36:, :],
v[36:, :],
lons[36:, :],
lats[36:, :],
returnxy=True)
# plot filled contours over map.
cs = m.contourf(x, y, p[36:, :], 15, cmap=plt.cm.jet)
# plot wind vectors over map.
Q = m.quiver(x, y, urot, vrot) #or specify, e.g., width=0.003, scale=400)
qk = plt.quiverkey(Q, 0.95, 1.05, 25, '25 m/s', labelpos='W')
cax = plt.axes([0.875, 0.1, 0.05, 0.7]) # setup colorbar axes.
plt.colorbar(cax=cax) # draw colorbar
plt.axes(ax) # make the original axes current again
m.drawcoastlines()
m.drawcountries()
# draw parallels
delat = 20.
circles = np.arange(0.,90.+delat,delat).tolist()+\
np.arange(-delat,-90.-delat,-delat).tolist()
m.drawparallels(circles, labels=[1, 1, 1, 1])
# draw meridians
delon = 45.
meridians = np.arange(-180, 180, delon)
m.drawmeridians(meridians, labels=[1, 1, 1, 1])
plt.title('Surface Winds Winds and Pressure (lat-lon grid)', y=1.075)
'20170118.015_lp_2min-fitcal_2dVEF_001001',
'20170118.017_lp_2min-fitcal_2dVEF_001001',
'20170118.019_lp_2min-fitcal_2dVEF_001001',
'20170118.021_lp_2min-fitcal_2dVEF_001001']
for runname in runnames:
print runname
d=io_utils.read_whole_h5file(runname+'.h5')
plt.rcParams['figure.figsize']=10,10
plt.rcParams['font.size']=16
for r in range(d['/Fit2D']['DivE'].shape[0]):
fig=plt.figure()
div_clrs=plt.pcolormesh(d['/Grid']['x'][0,:],d['/Grid']['y'][0,:],d['/Fit2D']['DivE'][r,:,:],vmin=-1e-5,vmax=1e-5,cmap='RdBu_r')
qv=plt.quiver(d['/Grid']['x'][0,:],d['/Grid']['y'][0,:],d['/Fit2D']['Ex'][r,:,:],d['/Fit2D']['Ey'][r,:,:],d['/Fit2D']['Emag'][r,:,:],scale=2500,cmap='bone_r')
qk = plt.quiverkey(qv, 0.5, 0.875, 100, '100 mV/m',
labelpos='E',
coordinates='figure',
fontproperties={'weight': 'bold'})
plt.title(datetime.datetime(1970,1,1)+datetime.timedelta(seconds=int(d['/Time']['UnixTime'][r,0])))
plt.xlabel('Mag Longitude')
plt.ylabel('Mag Latitude')
hc=plt.colorbar(div_clrs)
hc.set_label('DivE')
plt.savefig('./figtmp/fig_'+runname+'_'+str(r)+'.png',format='png',dpi=100)
plt.close(fig)
os.system('ffmpeg -r 4 -i figtmp/fig_'+runname+'_%d.png -c:v libx264 -pix_fmt yuv420p ' + runname + '_divE.mp4')
def test(err=0, mknewcat=True, pattern_error=100, dev_pat=True, distort=True, debug_plots=False, order_pattern_error=False, trim_cam=False, fix_trans=False, fit=True, npos=3, rot_ang_l=[0, 90, 180, 270], step_size=250, Niter=5, plot_in=False, order=4, correct_ref=False, lab_offsets=False, plot_dist=True, Nmissing=None, pattern_from_distortion=True, order_pattern=1):
'''
Test function for disotriotn fitting routine that includes altering the refernece positions
The fit_all.simul_wref() takes a list of xpositoins, ypositions and offsets, compares them to a perfect square reference and then fits for both the distortion and the pattern deviation
err is the size of measurment error in pixels
pattern error is the size of the (random) deviations applied ot each pinhole
correct_ref(bool): If True, the reference coordinates used in the fit are chaged to the correct deviated values. This validates that the fit works if you give it the right answer
To simulate:
-First create a perfect square reference
-For each mask position:
-Apply a pattern deviation (function of reference pixel location as a single second order polynomial) TEST:redo using arbitrary deviations
-Apply a translation offset (~1000 pixels)
-Apply a distortion map (function of translated pixels)
-Add noise if desired
Note:Deviations (distortion and pattern) must be smaller than 30 pixels in total, as that is the matching radius in the code. To match measured data the distortion should be ~0.3 pixels and the pattern deviation should be ~ 0.016 pixels.
Do the tests in terms of the coeffiicients not just the residuals.
Walk up distoriton solutions from fits order in separate functions
'''
colors = ['black', 'blue', 'green', 'purple', 'brown', 'magenta', 'teal', 'yellow', 'gray', 'black', 'blue', 'green', 'purple', 'brown', 'magenta', 'teal', 'yellow', 'gray','black', 'blue', 'green', 'purple', 'brown', 'magenta', 'teal', 'yellow', 'gray', 'black', 'blue', 'green', 'purple', 'brown', 'magenta', 'teal', 'yellow', 'gray','black', 'blue', 'green', 'purple', 'brown', 'magenta', 'teal', 'yellow', 'gray', 'black', 'blue', 'green', 'purple', 'brown', 'magenta', 'teal', 'yellow', 'gray','black', 'blue', 'green', 'purple', 'brown', 'magenta', 'teal', 'yellow', 'gray', 'black', 'blue', 'green', 'purple', 'brown', 'magenta', 'teal', 'yellow', 'gray','black', 'blue', 'green', 'purple', 'brown', 'magenta', 'teal', 'yellow', 'gray', 'black', 'blue', 'green', 'purple', 'brown', 'magenta', 'teal', 'yellow', 'gray','black', 'blue', 'green', 'purple', 'brown', 'magenta', 'teal', 'yellow', 'gray', 'black', 'blue', 'green', 'purple', 'brown', 'magenta', 'teal', 'yellow', 'gray']
wd = os.getcwd()
if not 'tmp' in wd:
os.mkdir('tmp')
os.chdir('./tmp')
if mknewcat:
#make the reference catalog that the fitting code will use
fit_all.mkrefcat(ang=0)
#make a starting reference catalog that we will deviate and use to create simulated measurements.
#fit_all.mkrefcat(outf='ref_test.txt', ang=0)
ref = Table.read('reference.txt', format='ascii.basic')
#need to declare a pattern deviation
t = transforms.PolyTransform(np.ones(10), np.ones(10), np.ones(10), np.ones(10), 4)
#change this to directly call the astropy.models directly
#now we can declare the polynomial coefficients
#translation = 0
t.px.c0_0 = 0
#x scale
t.px.c1_0 = 0 #-0.00002
#linear cross term
t.px.c0_1 = 0 #0.00004
#quadratic terms
t.px.c2_0 = 2 * 10**-8
t.px.c0_2 = 0 #-4 * 10**-9
t.px.c1_1 = 0# 5 * 10**-10
t.px.c3_0 = 0 #10**-12
t.px.c2_1 = 0
t.px.c1_2 = 0
t.px.c0_3 = 0
t.px.c4_0 = 0 #10**-14
t.px.c3_1 = 0
t.px.c2_2 = 0
t.px.c1_3 = 0
t.px.c0_4 = 0
t.py.c0_0 = 0
t.py.c1_0 = 0 # 0.00009
t.py.c0_1 = 0 #-0.00005
t.py.c2_0 = 0 # 7 * 10**-10
t.py.c1_1 = 0 #6 * 10**-9
t.py.c0_2 = 0 #2* * 10**-9
t.py.c3_0 = 0 #10**-12
t.py.c2_1 = 0
t.py.c1_2 = 0
t.py.c0_3 = 0
t.py.c4_0 = 0# 10**-14
t.py.c3_1 = 0
t.py.c2_2 = 0
t.py.c1_3 = 0
t.py.c0_4 = 0
#now apply this as a function of reference position
xmin = 1000
xmax = 6000
ymin = 1000
ymax = 5500
cb = (ref['x'] < xmax) * (ref['x'] > xmin) * (ref['y'] < ymax) * (ref['y'] > ymin)
inco = Table.read('best_fit.txt', format='ascii.basic')
#only keep the linear terms
if order_pattern == 2:
#only keep the quadratic trerms from the distortion as pattern deviation
inco[-9:] = 0.0
inco[-21:-12] = 0.0
if order_pattern == 3:
#4th order Y terms
inco[-5:] = 0
#2nd order Y terms
inco[-12:-10] = 0
#4th order x terms
inco[-17:-12] = 0
#2nd order x terms
inco[-24:-21] = 0
if order_pattern == 4:
#3rd order Y terms
inco[-9:-5] = 0
#2nd order Y terms
inco[-12:-9] = 0
#3rd order x terms
inco[-21:-18] = 0
#2nd order x terms
inco[-24:-21] = 0
#chop out the linear parameters at the begining of this array
inco = inco[-30:]
xmin = 0
xmax = np.inf
ymin = 0
ymax = np.inf
xmin = 965.148
xmax = 7263.57
ymin = 490.87
ymax = 5218.0615
rb = (ref['x'] > xmin) * (ref['x'] < xmax) * (ref['y'] < ymax) * (ref['y'] > ymin)
print('input RMS deviations')
#import pdb;pdb.set_trace()
dx_pd, dy_pd = fit_all.com_mod(inco['col0'], [ref['x']], [ref['y']], [ref['x']], [ref['y']], order=4, evaluate=True, ret_dist=True)
print(np.std(dx_pd[0][rb])*6000, np.std(dy_pd[0][rb])*6000)
#rb2 = np.invert(rb)
#dx_pd[0][rb2] = 0
#dy_pd[0][rb2] = 0
if not pattern_from_distortion:
dx_pd = 0
dy_pd = 0
if order_pattern_error:
dx, dy = t.evaluate(ref['x']-np.median(ref['x']), ref['y']-np.median(ref['y']))
else:
dx = np.zeros(len(ref['x']))
dy = np.zeros(len(ref['y']))
# import pdb;pdb.set_trace()
print(np.std(dx[cb])*6000.0,np.std(dy[cb])*6000.0)
print(np.min(dx[cb])*6000.0, np.max(dx[cb])*6000.0, np.min(dy[cb])*6000.0, np.max(dy[cb])*6000.0)
_norm_pattern = scipy.stats.norm(loc=0, scale=pattern_error/6000.0)
_xerr = _norm_pattern.rvs(len(ref['x']))
_yerr = _norm_pattern.rvs(len(ref['x']))
xpin = ref['x'] + _xerr + dx + dx_pd
ypin = ref['y'] + _yerr + dy +dy_pd
xpin = np.array(xpin)[0]
ypin = np.array(ypin)[0]
plt.close('all')
if correct_ref:
_out = ref
_out['x'] = xpin
_out['y'] = ypin
_out.write('reference.txt', format='ascii.basic')
if debug_plots:
mkplots_1(ref, dx, dy, _xerr, _yerr, xpin, ypin)
#now we need to apply translation offsets and create the "average stacked catalogs"
#these are the offsets from s8, used in paper
#offsets = [[753, 333],[356,336],[7388-7096,5705-7015],[6203-7096,5707-7015],[6173-7055,300--40.6],[1192-40.6,5758-7055.0], [ 1500, 330], [1500, -1300], [0,0]]
rot_ang = []
if lab_offsets:
offsets_s = [[447-40.6, 5894-7055], [770-40.6, 5895-7055], [945-40.6, 5888-7055], [944-40.6, 5644-7055], [697-40.6, 5620-7055], [488-40.6, 5619-7055], [486-40.6, 5376-7055], [745-40.6, 5381-7055], [982-40.6, 5371-7055]]
#create a square gird (npos x npos) of obsevations at each rot_ang note these are now input keyword arguements
offsets = []
#rot_ang_l = [0, 90, 180, 270]
#import pdb;pdb.set_trace()
for _ang in rot_ang_l:
if not lab_offsets:
for i in range(npos):
for j in range(npos):
offsets.append([i * step_size, j * step_size])
rot_ang.append(_ang)
else:
for k in range(len(offsets_s)):
offsets.append(offsets_s[k])
rot_ang.append(_ang)
xlis = []
ylis = []
plt.figure(2)
plt.clf()
offsets_in = []
_norm = scipy.stats.norm(loc=0 , scale=err)
for _iii, _off in enumerate(offsets):
_ang = -1.0*np.deg2rad(rot_ang[_iii])
_xtmp = (xpin-4000)*np.cos(_ang) - (ypin-3000)*np.sin(_ang)
_ytmp = (ypin-3000)*np.cos(_ang) + (xpin-4000)*np.sin(_ang)
#now we need to move the measured coordiantes such that the lowest value points (lower left) is at offsets[i][0,1]
#import pdb;pdb.set_trace()
_dx = _off[0] + 4000
_dy = _off[1] + 3000
xlis.append(np.array(_xtmp + _dx))
ylis.append(np.array(_ytmp + _dy))
offsets_in.append(((xlis[-1][0]),ylis[-1][0]) )
#if _ang != 0:
# import pdb;pdb.set_trace()
print(offsets_in[-1])
if debug_plots:
plt.figure(2)
plt.scatter(xlis[-1], ylis[-1], label='catalog '+str(_iii))
plt.title('Measured Position with no distortion')
plt.legend(loc='upper right')
#this is a 4th order Legendre Polynomial -- measured for single stack s6/pos_1/
td = mkdist() #look in def mkdist for details of the current distortion applied
xmax = 8000
xmin = -1
ymax = 8000
ymin = -1
xln = []
yln = []
xrn = []
yrn = []
xrnC = []
yrnC = []
plt.figure(100)
plt.clf()
#import pdb;pdb.set_trace()
for i in range(len(xlis)):
cbool = (xlis[i] < xmax) * (xlis[i] > xmin) * (ylis[i] < ymax) * (ylis[i] > ymin)
cbool = np.ones(len(xlis[i]), dtype='bool')
dxd, dyd = td.evaluate(xlis[i][cbool]-4000.0, ylis[i][cbool]-3000.0)
print('RMS size of distortion', np.std(dxd)*6000, np.std(dyd)*6000.0, np.median(dxd)*6000, np.median(dyd)*6000)
#import pdb;pdb.set_trace()
if not distort:
dxd = np.zeros(np.sum(cbool))
dyd = np.zeros(np.sum(cbool))
if plot_dist:
plt.figure(2200)
q = plt.quiver(xlis[i][cbool], ylis[i][cbool],dxd, dyd, scale =10, color=colors[i])
plt.quiverkey(q, -50, -50, 1, '6000 nm', coordinates='data', color='red')
#add the distortion term to the measurments
xln.append(xlis[i][cbool]+dxd+ _norm.rvs(np.sum(cbool)))
yln.append(ylis[i][cbool]+dyd+ _norm.rvs(np.sum(cbool)))
#create the array of reference positions that is matched to the measurements
xrnC.append(xpin[cbool])
yrnC.append(ypin[cbool])
#create transformstion for the debugging plots
tl = transforms.PolyTransform(ref['x'], ref['y'], xln[-1], yln[-1], 1)
__xn, __yn = tl.evaluate(ref['x'], ref['y'])
xrn.append(__xn)
yrn.append(__yn)
if debug_plots:
#need
mk_debug_plots(ref, xln, yln)
#import pdb;pdb.set_trace()
#now we are ready to run the fitting routine
#we iterate to allow the reference positions to converge
#fit_all.simul_wref(xln,yln,offsets)
if not fit:
import pdb;pdb.set_trace()
init_guess = fit_all.guess_co(xln, yln, xrnC, yrnC, order=order)
res = leastsq(fit_all.com_mod, init_guess, args=(xln, yln, xrnC, yrnC, fix_trans, init_guess, order))
outres = fit_all.com_mod(res[0], xln, yln, xrnC, yrnC,fix_trans=fix_trans, order=order, evaluate=False, init_guess=init_guess)
return outres, res
if Nmissing is None:
Nmissing = len(xln)+1
res = fit_all.simul_wref(xln, yln, offsets_in, order=order, rot_ang=rot_ang, Niter=Niter, dev_pat=dev_pat, Nmissing=len(xln)+1, sig_clip=False, fourp=False, trim_cam=trim_cam, fix_trans=fix_trans, debug=True, plot_ind=plot_in, trim_pin=False)
#import pdb;pdb.set_trace()
#return
#if the fitting procedure has updated reference.txt with fixed coordiantes -> these should match xpin and ypin
refn = Table.read('reference_new.txt', format='ascii.basic')
cb = (refn['x'] - refn['xorig']) != 0.0
__dx = (refn['x'] - xpin) #this is the input deviation
__dy = (refn['y'] - ypin)
#make scatter plots of the recovered pinhole deviation errors
plt.figure(2000)
mkplots_2(refn, xpin, ypin, cb, __dx, __dy)
#now we compare coefficients to the fit
fit_all.mksamp(outf='dist_test.txt', order=order)
_dist = Table.read('dist_test.txt', format='ascii.basic')
if distort:
_dxin, _dyin = td.evaluate(_dist['x']-4000, _dist['y']-3000)
else:
_dxin = np.zeros(len(_dist['x']))
_dyin = np.zeros(len(_dist['y']))
#to do this comparrison you need to eliminate the linear terms in the input distortion
plt.figure(2005)
#_tl = transforms.PolyTransform(_dist['x']+_dxin, _dist['y']+_dyin, _dist['dx']+_dist['x'], _dist['dy']+_dist['y'], 1)
_tl = transforms.PolyTransform(_dist['x'], _dist['y'],_dist['dx']+_dxin,_dist['dy']+ _dyin, 1)
_xmd, _ymd = _tl.evaluate(_dist['x'], _dist['y'])
#_tl1 = transforms.PolyTransform(_dist['x'], _dist['y'],_dist['dx'], _dist['dy'], 1)
#_xmd1, _ymd1 = _tl.evaluate(_dist['x'], _dist['y'])
diffx = _dist['dx'] + _dxin - _xmd
diffy = _dist['dy'] + _dyin - _ymd
import pdb;pdb.set_trace()
#diffx = _dist['dx']+_dxin
#diffx = diffx - np.mean(diffx)
#diffy = _dist['dy']+_dyin
#diffy = diffy - np.mean(diffy)
plt.figure(2005)
plt.scatter(_dist['x'], _dist['y'], c=diffx*6000.0)
plt.title('X Camera Distortion Meaurement Mistake (model - input)')
plt.xlabel("X reference (pix)")
plt.ylabel("Y reference (pix)")
plt.colorbar()
plt.tight_layout()
plt.figure(2006)
plt.scatter(_dist['x'], _dist['y'], c=diffy*6000.0)
plt.title('Y Camera Distortion Measurement Mistake (model - input)')
plt.xlabel("X reference (pix)")
plt.ylabel("Y reference (pix)")
plt.colorbar()
plt.tight_layout()
plt.figure(2007)
plt.hist((diffx)*6000.0, histtype='step', label='x', lw=3)
plt.hist((diffy)*6000.0, histtype='step', label='y', lw=3)
plt.xlabel("Camera Distortion Meaurement Mistake (model - input)")
plt.ylabel("N")
plt.legend(loc='upper left')
co = Table.read('fit.txt', format='ascii.basic')
#Q1 = plt.quiver(x[::dec,::dec],y[::dec,::dec],Gx[::dec,::dec],Gy[::dec,::dec],
# scale=500,width=0.006)
plot_fig_label(ax, xc=0.95, yc=.05, label="b")
else:
plt.contour(x, y, qpsi / (Ue * ke), cq0[2:], colors='k')
plt.contour(x, y, qpsi / (Ue * ke), cq0[:2], colors='k')
Q = plt.quiver(x[::dec, ::dec],
y[::dec, ::dec],
Fwx[::dec, ::dec],
Fwy[::dec, ::dec],
scale=5e-2,
width=0.006)
qk = plt.quiverkey(Q,
0.175,
.8285,
5e-3,
r'$5\times10^{-3}\times\,\,{\mathcal{{\bf F}}}/F$',
labelpos='E',
coordinates='figure')
plot_fig_label(ax, xc=0.95, yc=.05, label="a")
plt.xlim(xlim)
plt.ylim(xlim)
ax.set_xlabel(r"$x\times k_e/2\pi$")
ax.set_xticks([-1., 0, 1])
if i == 0:
ax.set_ylabel(r"$y\times k_e/2\pi$")
ax.set_yticks([-1., 0, 1])
elif i == 1 or i == 2:
ax.set_yticks([])
else:
def bin_by_fov(ccd, x, y, dT, de1, de2, bands):
import numpy as np
import matplotlib.pyplot as plt
from toFocal import toFocal
all_x = np.array([])
all_y = np.array([])
all_e1 = np.array([])
all_e2 = np.array([])
all_T = np.array([])
nwhisk = 5
x_bins = np.linspace(0, 2048, nwhisk + 1)
y_bins = np.linspace(0, 4096, 2 * nwhisk + 1)
ccdnums = np.unique(ccd)
for ccdnum in ccdnums:
mask = np.where(ccd == ccdnum)[0]
print('ccdnum = ', ccdnum, ', nstar = ', mask.sum())
if mask.sum() < 100: continue
x_index = np.digitize(x[mask], x_bins)
y_index = np.digitize(y[mask], y_bins)
bin_de1 = np.array([
de1[mask][(x_index == i) & (y_index == j)].mean()
for i in range(1, len(x_bins)) for j in range(1, len(y_bins))
])
print('bin_de1 = ', bin_de1)
bin_de2 = np.array([
de2[mask][(x_index == i) & (y_index == j)].mean()
for i in range(1, len(x_bins)) for j in range(1, len(y_bins))
])
print('bin_de2 = ', bin_de2)
bin_dT = np.array([
dT[mask][(x_index == i) & (y_index == j)].mean()
for i in range(1, len(x_bins)) for j in range(1, len(y_bins))
])
print('bin_dT = ', bin_dT)
bin_x = np.array([
x[mask][(x_index == i) & (y_index == j)].mean()
for i in range(1, len(x_bins)) for j in range(1, len(y_bins))
])
print('bin_x = ', bin_x)
bin_y = np.array([
y[mask][(x_index == i) & (y_index == j)].mean()
for i in range(1, len(x_bins)) for j in range(1, len(y_bins))
])
print('bin_y = ', bin_y)
bin_count = np.array([((x_index == i) & (y_index == j)).sum()
for i in range(1, len(x_bins))
for j in range(1, len(y_bins))])
print('bin_count = ', bin_count)
focal_x, focal_y = toFocal(ccdnum, bin_x, bin_y)
mask2 = np.where(bin_count > 0)[0]
print('num with count > 0 = ', mask2.sum())
all_x = np.append(all_x, focal_x[mask2])
all_y = np.append(all_y, focal_y[mask2])
all_e1 = np.append(all_e1, bin_de1[mask2])
all_e2 = np.append(all_e2, bin_de2[mask2])
all_T = np.append(all_T, bin_dT[mask2])
plt.clf()
#plt.title('PSF Ellipticity residuals in DES focal plane')
theta = np.arctan2(all_e2, all_e1) / 2.
r = np.sqrt(all_e1**2 + all_e2**2)
u = r * np.cos(theta)
v = r * np.sin(theta)
plt.xlim(-250, 250)
plt.ylim(-250, 250)
print('all_x = ', all_x)
print('len(all_x) = ', len(all_x))
qv = plt.quiver(all_x,
all_y,
u,
v,
pivot='middle',
scale_units='xy',
headwidth=0.,
headlength=0.,
headaxislength=0.,
width=0.001,
scale=1.e-3,
color='blue')
ref_scale = 0.01
if 'raw' in bands:
ref_label = 'e = ' + str(ref_scale)
else:
ref_label = 'de = ' + str(ref_scale)
plt.quiverkey(qv,
0.10,
0.08,
ref_scale,
ref_label,
coordinates='axes',
color='darkred',
labelcolor='darkred',
labelpos='E',
fontproperties={'size': 'x-small'})
plt.axis('off')
plt.savefig('de_fov_' + bands + '.png')
plt.savefig('de_fov_' + bands + '.pdf')
plt.savefig('de_fov_' + bands + '.eps')
def plot(self,
timedata=None,
udata=None,
vdata=None,
ylabel=None,
**kwargs):
if kwargs['rotate'] != 0.0:
#when rotating vectors - positive(+) rotation is equal to cw of the axis (ccw of vector)
# - negative(+) rotation is equal to ccw of the axis (cw of the vector)
print "rotating vectors"
angle_offset_rad = np.deg2rad(kwargs['rotate'])
udata = udata * np.cos(angle_offset_rad) + vdata * np.sin(
angle_offset_rad)
vdata = -1. * udata * np.sin(angle_offset_rad) + vdata * np.cos(
angle_offset_rad)
magnitude = np.sqrt(udata**2 + vdata**2)
fig = plt.figure(1)
ax1 = plt.subplot2grid((2, 1), (0, 0), colspan=1, rowspan=1)
ax2 = plt.subplot2grid((2, 1), (1, 0), colspan=1, rowspan=1)
# Plot u and v components
# Plot quiver
ax1.set_ylim(-1 * np.nanmax(magnitude), np.nanmax(magnitude))
fill1 = ax1.fill_between(timedata, magnitude, 0, color='k', alpha=0.1)
# Fake 'box' to be able to insert a legend for 'Magnitude'
p = ax1.add_patch(plt.Rectangle((1, 1), 1, 1, fc='k', alpha=0.1))
leg1 = ax1.legend([p], ["Current magnitude [cm/s]"], loc='lower right')
leg1._drawFrame = False
# 1D Quiver plot
q = ax1.quiver(timedata,
0,
udata,
vdata,
color='r',
units='y',
scale_units='y',
scale=1,
headlength=1,
headaxislength=1,
width=0.04,
alpha=.95)
qk = plt.quiverkey(q,
0.2,
0.05,
5,
r'$5 \frac{cm}{s}$',
labelpos='W',
fontproperties={'weight': 'bold'})
# Plot u and v components
ax1.set_xticklabels(ax1.get_xticklabels(), visible=False)
ax2.set_xticklabels(ax2.get_xticklabels(), visible=True)
ax1.axes.get_xaxis().set_visible(False)
ax1.set_xlim(timedata.min() - 0.5, timedata.max() + 0.5)
ax1.set_ylabel("Velocity (cm/s)")
ax2.plot(timedata, vdata, 'b-', linewidth=0.25)
ax2.plot(timedata, udata, 'g-', linewidth=0.25)
ax2.set_xlim(timedata.min() - 0.5, timedata.max() + 0.5)
ax2.set_xlabel("Date (UTC)")
ax2.set_ylabel("Velocity (cm/s)")
ax2.xaxis.set_major_locator(MonthLocator())
ax2.xaxis.set_minor_locator(
MonthLocator(bymonth=range(1, 13), bymonthday=15))
ax2.xaxis.set_major_formatter(ticker.NullFormatter())
ax2.xaxis.set_minor_formatter(DateFormatter('%b %y'))
ax1.spines['bottom'].set_visible(False)
ax2.spines['top'].set_visible(False)
ax1.xaxis.set_ticks_position('top')
ax2.xaxis.set_ticks_position('bottom')
ax2.yaxis.set_ticks_position('both')
ax2.tick_params(axis='both', which='minor', labelsize=self.labelsize)
ax1.tick_params(axis='both', which='minor', labelsize=self.labelsize)
#manual time limit sets
#ax1.set_xlim([datetime.datetime(2016,2,1),datetime.datetime(2016,9,15)])
#ax2.set_xlim([datetime.datetime(2016,2,1),datetime.datetime(2016,9,15)])
# Set legend location - See: http://matplotlib.org/Volumes/WDC_internal/users/legend_guide.html#legend-location
leg2 = plt.legend(['v', 'u'], loc='upper left')
leg2._drawFrame = False
return plt, fig
ax.set_xticks(np.arange(40,80,10))
ax.set_xticklabels((r'$40^o$E', r'$50^o$E', r'$60^o$E', r'$70^o$E'))
ax.set_yticks(np.arange(-20,10,10))
ax.set_yticklabels((r'$20^o$S', r'$10^o$S', r'$0^o$S'))
ax.text(0.03, 0.88, 'h)',
transform=ax.transAxes, bbox=dict(facecolor='white',
alpha=0.5), color='k', fontsize=14)
#plt.axis([51.63, 58.36, -8.9, -1.06])
plt.axis([42, 65, -18, 3])
# fig.suptitle('ssh clim 1993-2009')
fig.subplots_adjust(left=0.07, right=0.9, hspace=0.03, wspace=0.01)
cbar_ax = fig.add_axes([0.91, 0.15, 0.02, 0.7])
cbar = fig.colorbar(ctop, cax=cbar_ax, extend='both', ticks=np.arange(-10,12,2))
cbar.set_label('[cm]')
qk = plt.quiverkey(Q, 0.90, 0.08, 10, r'$10 \frac{cm}{s}$', labelpos='E',
coordinates='figure')
plt.savefig('aviso_pop_comp_seas_large.pdf', bbox_inches='tight')
# Calculate the monthly average - the 19 year average
uavg_sat = u_sat.mean(0)
vavg_sat = v_sat.mean(0)
sshavg_sat = ssh_sat.mean(0)
uavg_pop = u_pop.mean(0)
vavg_pop = v_pop.mean(0)
sshavg_pop = ssh_pop.mean(0)
colori = cmocean.cm.balance
colori = cm.bwr
li = 4
q = ax1.quiver(xdate,
0,
ucomp,
vcomp,
color='r',
units='y',
scale_units='y',
scale=1,
headlength=2,
headaxislength=2,
width=0.1,
alpha=.95)
qk = plt.quiverkey(q,
0.2,
0.05,
5,
r'$5 \frac{m}{s}$',
labelpos='W',
fontproperties={'weight': 'bold'})
ax1.set_ylim(vcomp.min(), vcomp.max())
ax1.set_ylabel("(m/s)")
ax1.set_xlim(
datetime.datetime(2010 + i - 1, 8, 01).toordinal(),
datetime.datetime(2011 + i - 1, 10, 31).toordinal())
ax1.xaxis.set_major_locator(MonthLocator())
ax1.xaxis.set_minor_locator(
MonthLocator(bymonth=range(1, 13), bymonthday=15))
ax1.xaxis.set_major_formatter(ticker.NullFormatter())
ax1.xaxis.set_minor_formatter(DateFormatter('%b %y'))
ax1.tick_params(axis='both', which='minor', labelsize=12)
