def eq2gal(ra, dec):
rmat = numpy.array(
[
[-0.054875539726, -0.873437108010, -0.483834985808],
[+0.494109453312, -0.444829589425, +0.746982251810],
[-0.867666135858, -0.198076386122, +0.455983795705],
],
dtype="d",
)
cosb = math.cos(dec)
v1 = numpy.array([math.cos(ra) * cosb, math.sin(ra) * cosb, math.sin(dec)])
v2 = numpy.dot(rmat, v1)
x = v2[0]
y = v2[1]
z = v2[2]
r = math.sqrt(x * x + y * y)
if r == 0.0:
l = 0.0
else:
l = math.atan2(y, x)
if z == 0.0:
b = 0.0
else:
b = math.atan2(z, r)
ll = math.fmod(l, 2.0 * math.pi)
if ll < 0.0:
ll = ll + 2.0 * math.pi
bb = math.fmod(b, 2 * math.pi)
if abs(bb) >= math.pi:
print "Ugh!"
return ll, bb
def slice_linear(zmin, zmax, n, scale=None):
"""The size of result is (n-1)."""
COMBS = [
None, # not used
(0, ),
(0, 5, ),
(0, 3, 7, ),
(0, 3, 5, 7, ),
(0, 2, 4, 6, 8, ),
(0, 2, 3, 5, 7, 8, ),
(0, 1, 3, 4, 6, 7, 9, ),
(0, 1, 3, 4, 5, 6, 7, 9, ),
(0, 1, 2, 3, 4, 6, 7, 8, 9, ),
(0, 1, 2, 3, 4, 5, 6, 7, 8, 9, ),
]
if scale is None:
scale = 10 * ceil_pow10((zmax - zmin) / n)
step = scale // 10
def generate(comb, bases):
if comb is None:
return []
result = [base + _ * step for base in bases for _ in comb]
return [_ for _ in result if zmin < _ < zmax]
zmin_floored = math.floor(zmin - math.fmod(zmin, scale)) # XXX: these might be numerically unstable
zmax_ceiled = math.ceil(zmax - math.fmod(zmax, scale))
multiples = list(range(zmin_floored, zmax_ceiled + scale, scale))
multiples = [_ for _ in multiples if zmin < _ < zmax]
if len(multiples) == 0:
k = (zmax_ceiled - zmin_floored) // step
if k == 0:
return slice_linear(zmin, zmax, n, scale=(scale // 10))
result = generate(COMBS[k], [zmin_floored])
# TODO: compensate len(result) to be == (n - 1)
return result
k = n // len(multiples)
if k <= 0:
return []
if k > 10:
return slice_linear(zmin, zmax, n, scale=(scale // 10))
result_body = generate(COMBS[k], multiples[:-1])
result_head = []
result_tail = []
# len(result_head + result_body + result_tail) should be == (n - 1)
len_needed = (n - 1) - len(result_body)
assert len_needed >= 0
head_length = len_needed // 2
tail_length = (len_needed + 1) // 2
for comb in COMBS[:(k + 1)]:
candidate = generate(comb, [multiples[0] - scale])
if len(candidate) == head_length:
result_head = candidate
candidate = generate(comb, [multiples[-1]])
if len(candidate) == tail_length:
result_tail = candidate
result = result_head + result_body + result_tail
if len(result) != (n - 1):
# n is too large (e.g. zmin = 10, zmax = 1000, n = 50)
# Once again, do the linear slicing instead
return slice_linear(zmin, zmax, n, scale=(scale // 10))
return result
def _rotate_hcline(obj, objdict, cx, cy, ra):
_layer = obj.getParent()
if _layer is None:
raise RuntimeError, "HCLine parent is None"
_lp = obj.getLocation()
if _lp.getParent() is not _layer:
raise RuntimeError, "HCLine/Point parent object conflict!"
_x, _y = _calc_coords(_lp, cx, cy, ra)
_pts = _layer.find('point', _x, _y)
if len(_pts) == 0:
_np = Point(_x, _y)
_layer.addObject(_np)
else:
_np = _most_used(_pts)
_da = ra/_dtr
if abs(fmod(_da, 180.0)) < 1e-10:
obj.setLocation(_np)
if _adjust_dimension(_lp, _np):
_layer.delObject(_lp)
elif abs(fmod(_da, 90.0)) < 1e-10:
_layer.addObject(VCLine(_np))
if _adjust_dimension(_lp, _np):
_layer.delObject(obj)
else:
_layer.addObject(ACLine(_np, _da))
_layer.delObject(obj)
_pid = id(_lp)
if objdict.get(_pid) is not False:
objdict[_pid] = False
def pattern(self):
self.trap.send_decay(ALL, 90)
self.trap.start_pattern(ALL)
index = 0
hue_offset = 0.0
stop = False
color_rings = [ random_color(), random_color(), random_color() , random_color() ]
while not stop:
for bottle, angle in self.geo.enumerate_all_bottles(index % 2 == 0):
self.trap.set_color(bottle, color_rings[self.geo.get_ring_from_bottle(bottle)])
sleep(.01)
if self.stop_thread:
stop = True
break
index += 1
hue_offset = math.fmod(hue_offset + .02, 1.0)
shift = math.sin(index / self.color_shift_between_rings) / 2.0 + .50
new_offset = math.fmod(shift, 1.0)
color_rings.pop()
color_rings.insert(0, hue_to_color(new_offset))
self.trap.stop_pattern(ALL)
if self.transition:
sleep(.02)
transition_sweep_out(self.trap)
def draw_palette(H,height,width):
H = fmod(H,360) if H >= 360 else 360+fmod(H,360) if H < 0 else H
name = "_".join([str(H),str(height),str(width)])
if name not in lookup:
p2=[]
V_step = 100.0/height
S_step = 100.0/width
for row in range(height):
V = 100 - V_step * row
if V<=0 : V = 1
l=[]
for col in range(width):
S = 100 - S_step * col
if S<=0 : S = 1
hex = rgb2hex(hsv2rgb([H,S,V]))
l.append(hex)
p2.append(l)
lookup[name] = p2 # obmit coping as
# the list ref will not be changed
# when we use [] to creat a new one
else:
p2 = lookup[name]
vcmd("call s:clear_match('pal')")
for row in range(height):
for col in range(width):
hex = p2[row][col]
hi_grp = "".join(["cv_pal_",str(row),"_",str(col)])
pos_ptn = "".join(["\\%",str(row+H_OFF+1),"l\\%"
,str(col+W_OFF+1),"c"])
vcmd("call s:hi_color('{}','{}','{}',' ')".format(hi_grp,hex,hex))
vcmd("sil! let s:pal_dict['{0}'] = matchadd('{0}','{1}')"
.format( hi_grp,pos_ptn))
vcmd("".join(["let s:pal_clr_list=",str(p2)]))
def differentialWheelsSetSpeed(self, obj, left, right):
if self.leftWheelMaxSpeed < left :
left = self.leftWheelMaxSpeed
elif left < -self.leftWheelMaxSpeed :
left = -self.leftWheelMaxSpeed
if self.leftWheelSpeedUnit > self.Accueacy :
radiuse = math.fmod(math.fabs(left), self.leftWheelSpeedUnit)
if left > 0:
left -= radiuse
else:
left += radiuse
if self.rightWheelMaxSpeed < left :
left = self.rightWheelMaxSpeed
elif left < -self.rightWheelMaxSpeed :
left = -self.rightWheelMaxSpeed
if self.rightWheelSpeedUnit > self.Accueacy :
radiuse = math.fmod(math.fabs(left), self.rightWheelSpeedUnit)
if right > 0:
right -= radiuse
else:
right += radiuse
if self.leftWheelName:
obj.setAngularVelocityToParts(self.leftWheelName, left, self.leftMaxForce)
self.currentLeftWheelSpeed = left
if self.rightWheelName:
obj.setAngularVelocityToParts(self.rightWheelName, right, self.rightMaxForce)
self.currentRightWheelSpeed = right
return
def pCJDNToMilankovic(iCJDN, bDoYear=False, bDoMonth=False, bDoDay=False):
''' Returns a Revised Julian date is ISO 8601 YYYY-MM-DD format from a given
Chronological Julian Day Number (CJDN).
If only part of the date is required (e.g. just the day), this is returned as an integer.
'''
if not isinstance(iCJDN, int):
return False
#Perform the calculation
iK3 = (9 * (iCJDN - 1721120)) + 2
iX3 = floor(iK3 / 328718)
iK2 = (100 * floor(int(fmod(iK3, 328718)) / 9)) + 99
iX2 = floor(iK2 / 36525)
iK1 = (5 * floor(int(fmod(iK2, 36525)) / 100)) + 2
iX1 = floor(iK1 / 153)
iC0 = floor((iX1 + 2) / 12)
iYear = (100 * iX3) + iX2 + iC0
iMonth = (iX1 - (12 * iC0)) + 3
iDay = floor(int(fmod(iK1, 153)) / 5) + 1
#Return integer part, if only one part of the date is required.
#Start at year, and rudely ignore any subsequent integers requested.
if bDoYear:
return iYear
if bDoMonth:
return iMonth
if bDoDay:
return iDay
#Return the ISO 8601 date string
sISO8601Date = ('0000' + str(iYear))[-4:] + '-' + ('00' + str(iMonth))[-2:] + '-' + ('00' + str(iDay))[-2:]
return sISO8601Date
def wrap_angle(angle):
if angle <= math.pi and angle >= -math.pi:
return angle
elif angle < 0.0:
return math.fmod(angle-math.pi,2.0*math.pi)+math.pi
else:
return math.fmod(angle+math.pi,2.0*math.pi)-math.pi;
def complementaries(self, base_color):
# return some other colors that "go" with this one
hsv = RGBtoHSV(base_color)
(h,s,v,a) = hsv
# take 2 colors which are almost triads
h = hsv[0]
delta = random.gauss(0.0, 0.8)
h2 = math.fmod(h + 2.5 + delta, 6.0)
h3 = math.fmod(h + 3.5 - delta, 6.0)
# take darker and lighter versions
v = hsv[2]
vlight = self.clamp(v * 1.5, 0.0, 1.0)
vdark = v * 0.5
colors = [
[h, s, vdark, a],
[h, s, v, a],
[h, s, vlight, a],
[h2, s, vlight, a],
[h2, s, v, a],
[h2, s, vdark, a],
[h3, s, vdark, a],
[h3, s, v, a],
[h3, s, vlight, a]]
colors = [ HSVtoRGB(x) for x in colors]
return colors
def from_jd(cls, jd):
"""
Convert a Julian day number to a year/month/day tuple
of this calendar (matching jQuery calendars algorithm)
@param jd: the Julian day number
"""
jd = math.floor(jd) + 0.5;
depoch = jd - cls.to_jd(475, 1, 1)
cycle = math.floor(depoch / 1029983)
cyear = math.fmod(depoch, 1029983)
if cyear != 1029982:
aux1 = math.floor(cyear / 366)
aux2 = math.fmod(cyear, 366)
ycycle = math.floor(((2134 * aux1) + (2816 * aux2) + 2815) / 1028522) + aux1 + 1
else:
ycycle = 2820
year = ycycle + (2820 * cycle) + 474
if year <= 0:
year -= 1
yday = jd - cls.to_jd(year, 1, 1) + 1
if yday <= 186:
month = math.ceil(yday / 31)
else:
month = math.ceil((yday - 6) / 30)
day = jd - cls.to_jd(year, month, 1) + 1
return (int(year), int(month), int(day))
def pCJDNToJulian(iCJDN, bDoYear=False, bDoMonth=False, bDoDay=False):
''' Returns a Julian date is ISO 8601 YYYY-MM-DD format from a given
Chronological Julian Day Number (CJDN).
If only part of the date is required (e.g. just the day), this is returned as an integer.
'''
if not isinstance(iCJDN, int):
return False
#Perform the calculation
iY2 = iCJDN - 1721118
iK2 = (4 * iY2) + 3
iK1 = (5 * floor(int(fmod(iK2, 1461)) / 4)) + 2
iX1 = floor(iK1 / 153)
iC0 = floor((iX1 + 2) / 12)
iYear = floor(iK2 / 1461) + iC0
iMonth = (iX1 - (12 * iC0)) + 3
iDay = floor(int(fmod(iK1, 153)) / 5) + 1
#Return integer part, if only one part of the date is required.
#Start at year, and rudely ignore any subsequent integers requested.
if bDoYear:
return iYear
if bDoMonth:
return iMonth
if bDoDay:
return iDay
#Return the ISO 8601 date string
sISO8601Date = ('0000' + str(iYear))[-4:] + '-' + ('00' + str(iMonth))[-2:] + '-' + ('00' + str(iDay))[-2:]
return sISO8601Date
def getFrameByType(self, animType, animOffset, speed, frame):
def clamp(value, value_min, value_max):
return max(min(value, value_max), value_min)
animLength = len(self.frames)
animStart = 0
if animType in {'0', 'LOOP'}:
frame = fmod(animOffset+(frame-animStart)*speed, animLength)
if frame < 0:
frame += animLength
frame += animStart
elif animType in {'1', 'ONCE'}:
frame = clamp(animOffset+(frame-animStart)*speed, 0.0, animLength-1)+animStart
elif animType in {'2', 'PINGPONG'}:
frame = fmod(animOffset+(frame-animStart)*speed, animLength*2-2) # subtract 2 to remove the duplicate frames
if frame < 0:
frame += 2*animLength-2
if frame >= animLength:
frame = 2*animLength-2-frame
frame += animStart*speed
elif animType in {'3', 'STILL'}:
frame = clamp(animOffset+animStart, 0.0, animLength-1.0)
return int(frame)
def _adjust_point_users(pt, objdict, da):
_layer = pt.getParent()
for _user in pt.getUsers():
_uid = id(_user)
if _uid in objdict:
if isinstance(_user, HCLine) and _layer is not None:
if abs(fmod(da, 180.0)) < 1e-10:
objdict[_uid] = False
elif abs(fmod(da, 90.0)) < 1e-10:
_layer.addObject(VCLine(pt))
_layer.delObject(_user)
del objdict[_uid]
else:
_layer.addObject(ACLine(pt, da))
_layer.delObject(_user)
del objdict[_uid]
elif isinstance(_user, VCLine) and _layer is not None:
if abs(fmod(da, 180.0)) < 1e-10:
objdict[_uid] = False
elif abs(fmod(da, 90.0)) < 1e-10:
_layer.addObject(HCLine(pt))
_layer.delObject(_user)
del objdict[_uid]
else:
_layer.addObject(ACLine(pt, da))
_layer.delObject(_user)
del objdict[_uid]
elif isinstance(_user, ACLine) and _layer is not None:
_user.setAngle(_user.getAngle() + da)
objdict[_uid] = False
else:
if not isinstance(_user, Dimension):
objdict[_uid] = False
def get_block(self, x, z, y):
"""For any point in the map, return the type of block at that location.
y (int) represents altitude, positive is up and negative is down.
x and z (int) are the lattitude and logitude in the map.
"""
# Add simple noise to the coordinates to make it less rigid!
nx = x + 2*math.sin(z/4.7)
nz = z + 2*math.cos(x/5.9)
ny = y + math.sin(0.75 + x/7.8 + z/9.1)
nx = math.fmod(nx, 60)
nz = math.fmod(nz, 60)
ny = ny*8
# Manhattan distance field to center of map: floating iceberg.
if math.sqrt(nx*nx + ny*ny + nz*nz) < 17:
return c.MAT_DIRT
# Anything that's not solid but under the sea level?
if y == -1:
return c.MAT_SNOW
if y < -1:
return c.MAT_WATER
return c.MAT_AIR
def __init__(self, utc, longitude, latitude, altitude):
try:
super().__init__(longitude, latitude, altitude)
except TypeError:
super(TimeScale, self).__init__(longitude, latitude, altitude)
self.utc = utc
self.utc1, self.utc2 = strputc(self.utc)
self.tai1, self.tai2 = erfa.utctai(self.utc1, self.utc2)
self.tt1, self.tt2 = erfa.taitt(self.tai1, self.tai2)
self.tcg1, self.tcg2 = erfa.tttcg(self.tt1, self.tt2)
self.dut1 = -0.1
if (self.utc1+self.utc2) >= 2456708.5:
self.dut1 = -0.2
elif (self.utc1+self.utc2) >= 2456785.5:
self.dut1 = -0.3
elif (self.utc1+self.utc2) >= 2456925.5:
self.dut1 = -0.4
self.dt = 35+32.184-self.dut1
self.ut11, self.ut12 = erfa.utcut1(self.utc1, self.utc2, self.dut1)
# Extract fraction for TDB-TT calculation, later.
self.ut = math.fmod(math.fmod(self.ut11,1.0)+math.fmod(self.ut12,1.0),1.0)
# TDB-TT (using TT as a substitute for TDB).
self.dtr = erfa.dtdb(self.tt1, self.tt2, self.ut, self.elon, self.u, self.v)
self.tdb1, self.tdb2 = erfa.tttdb(self.tt1, self.tt2, self.dtr)
self.tcb1, self.tcb2 = erfa.tdbtcb(self.tdb1, self.tdb2)
def w_h_from_str(string, source_width, source_height):
if ':' in string: # used `w:h` syntax
w, h = string.split(':')
w = int(w)
h = int(h)
if w < -1 or h < -1:
raise ValueError('unknown negative component')
# keep aspect ratio if either component is -1
if w == -1 and h == -1: # ffmpeg allows this so we should too
return source_width, source_height
else:
if w == -1:
w = int(h * source_width / source_height) & ~1 # round to even
elif h == -1:
h = int(w * source_height / source_width) & ~1
elif float(string) != 1.0: # using a singlular int or float
# round to nearest even number
even_pixel = lambda x: \
int(math.floor(x * float(string) / 2) * 2)
w = even_pixel(source_width)
h = even_pixel(source_height)
else: # use source w,h by default
w = source_width
h = source_height
# w and h must be divisible by 2 for yuv420p outputs
# don't auto round when using the `w:h` syntax (with no -1 components)
# because the user may not expect the changes
if math.fmod(w, 2) != 0 or math.fmod(h, 2) != 0:
raise ValueError('components not divisible by two')
return w, h
def test_deg_km_accuracy(self):
c = quakelib.Conversion(quakelib.LatLonDepth(0,0))
# Check that 360 * length of 1 longitude degree is equal to the circumference of the equator
# Confirm accuracy is within 1 meter
one_deg_len = c.convert2xyz(quakelib.LatLonDepth(0,1)).mag()
self.assertAlmostEqual(one_deg_len*360.0/1000, 40075.016, 2)
# Check that 4 * length of 90 degree vertical arc is equal to the polar circumference
# Confirm accuracy is within 1 meter
ninety_deg_len = c.convert2xyz(quakelib.LatLonDepth(90,0)).mag()
self.assertAlmostEqual(ninety_deg_len*4.0/1000, 40007.860, 2)
# Check that inverse of conversion results in the same value
for base_lat in range(-90,91,5):
for base_lon in range(-180, 180, 5):
base_pt = quakelib.LatLonDepth(base_lat, base_lon)
conv = quakelib.Conversion(base_pt)
test_lat = math.fmod(base_lat+random.uniform(-45,45), 90)
test_lon = math.fmod(base_lon+random.uniform(-45,45), 180)
test_pt = quakelib.LatLonDepth(test_lat, test_lon)
new_xyz = conv.convert2xyz(test_pt)
rev_pt = conv.convert2LatLon(new_xyz)
# Ensure accuracy to within 1e-7 degrees (~1 cm)
self.assertAlmostEqual(test_lat, rev_pt.lat(), 7)
self.assertAlmostEqual(test_lon, rev_pt.lon(), 7)
def arange(start, stop, n):
start = fmod(start, 2*pi)
stop = fmod(start, 2*pi)
if(fabs(start - stop) > pi):
if start > stop: start -= 2*pi
else: stop -= 2*pi
return frange(start, stop, n)
def analyze(arrStack, mean, std):
print 'tracking.analyze ...'
shape = numpy.shape(std)
hsig = TH2F('hsig', '', shape[0], 0, shape[0]+1, shape[1], 0, shape[1]+1)
hsigw = TH1F('hsigw', '', 100, 0, 50)
# 2D to 1D
std = numpy.ravel(std)
mean = numpy.ravel(mean)
h3 = TH3F('h3', '', shape[0], 0, shape[0], shape[1], 0, shape[1], len(arrStack), 0, len(arrStack))
for i, arr in enumerate(arrStack):
if i%100 == 0:
print 'processing ... {0}/{1}'.format(i, len(arrStack))
hsig_tmp = TH2F('hsig_{0:04d}'.format(i), '', shape[0], 0, shape[0]+1, shape[1], 0, shape[1]+1)
# print 'hsig_{0:04d}'.format(i)
arr = numpy.ravel(arr)
pixels, pixel_indices = findPixels(arr, mean, std, i)
for index, x in numpy.ndenumerate(pixels):
hsig.Fill(math.floor(pixel_indices[index[0]]/shape[0]), math.fmod(pixel_indices[index[0]], shape[0]), x)
hsig_tmp.Fill(math.floor(pixel_indices[index[0]]/shape[0]), math.fmod(pixel_indices[index[0]], shape[0]), x)
hsig_tmp.Write()
hits = findHits(pixels, pixel_indices, shape[0], shape[1], i, h3)
h3.Write()
def mjd2gmst(mjd):
"""
Returns GMST given UT1 in the form of an MJD
The GMST is returned in radians from 0 to 2pi. This
was converted from Fortran source code of SOFA
"""
# Set some constants
DS2R = 7.272205216643039903848712e-5
DJ0 = 2451545e0
DJ1 = 2400000.5e0
DAYSEC = 86400e0
CENDAY = 36525e0
A = 24110.54841e0 - DAYSEC/2.
B = 8640184.812866e0
C = 0.093104e0
D = -6.2e-6
if DJ1 < mjd:
d1 = DJ1
d2 = mjd
else:
d1 = mjd
d2 = DJ1
t = (mjd + (DJ1-DJ0 ))/CENDAY
f = DAYSEC*(0.5 + m.fmod(mjd,1.))
return m.fmod(DS2R*((A+(B+(C+D*t)*t)*t)+f),2.*m.pi)
def round_to_sum(l, r):
"""
Round a list of numbers while maintaining the sum.
http://stackoverflow.com/questions/15769948/
round-a-python-list-of-numbers-and-maintain-the-sum
:param l: array
:type l: list(float)
:param r: decimal place
:type r: int
:returns: A list of rounded numbers whose sum is equal to the
sum of the list of input numbers.
:rtype: list
"""
q = 10 ** (-r)
d = (round(sum(l), r) - sum([round(x, r) for x in l])) * (10 ** r)
d = int(d)
if d == 0:
return [round(x, r) for x in l]
elif d in [-1, 1]:
c, _ = max(enumerate(l), key=lambda x: math.copysign(
1, d) * math.fmod(x[1] - 0.5 * q, q))
return [round(x, r) + q * math.copysign(1, d) if i == c else round(
x, r) for (i, x) in enumerate(l)]
else:
c = [i for i, _ in heapq.nlargest(abs(d), enumerate(
l), key=lambda x: math.copysign(1, d) * math.fmod(
x[1] - 0.5 * q, q))]
return [round(x, r) + q * math.copysign(
1, d) if i in c else round(x, r) for (i, x) in enumerate(l)]
def schwefel_func(x, Os=None, Mr=None, sr=None, adjust=1.0):
nx = len(x)
# z = sr_func(x, Os, Mr, 1000.0 / 100.0)
adjust = 0.2
z = sr_func(x, Os, Mr, 100000.0 / 100.0 * adjust)
f = 0.0
dim = float(len(x))
for i in range(nx):
z[i] += 4.209687462275036e+002
if z[i] > 500:
f -= (500.0 - fmod(z[i], 500)) * sin(pow(500.0 - fmod(z[i], 500),
0.5))
tmp = (z[i] - 500.0) / 100.0
f += tmp * tmp / nx
elif z[i] < -500:
f -= (-500.0 + fmod(fabs(z[i]), 500)) * sin(
pow(500.0 - fmod(fabs(z[i]), 500), 0.5))
tmp = (z[i] + 500.0) / 100
f += tmp * tmp / nx
else:
f -= z[i] * sin(pow(fabs(z[i]), 0.5))
f += 4.189828872724338e+002 * nx
# return max(f / 1000.0 - 0.838, 0.0)
# return max(f / 1000.0, 0.0)
return max((f - (dim * (dim - 1)) * 4.189e+002) / 1000.0, 0.0)
def onMouseMove(x, y):
global mouseDrag, mouseDragX, mouseDragY, mouseDragMove
global eyeX, eyeY, eyeZ, upX, upY, upZ, cam_theta, cam_phi, cam_r
if not mouseDrag:
return
mouseDragMove = True
# Mouse point to angle conversion
# cam_theta = (360.0/winHeight)*y*3.0#3.0 rotations possible
# cam_phi = (360.0/winWidth)*x*3.0
cam_phi += 360.0 * (mouseDragX - x) / winWidth * 2.0
cam_theta += 360.0 * (mouseDragY - y) / winHeight * 2.0
mouseDragX = x
mouseDragY = y
# Restrict the angles within 0~360 deg (optional)
if cam_theta > 360:
cam_theta = fmod(cam_theta, 360.0)
if cam_phi > 360:
cam_phi = fmod(cam_phi, 360.0)
newValues = lookInSphere(cam_r, cam_phi, cam_theta)
eyeX = newValues[0]
eyeY = newValues[1]
eyeZ = newValues[2]
upX = newValues[3]
upY = newValues[4]
upZ = newValues[5]
glutPostRedisplay()
def removeVars( varList ) :
# ======================
# remove unwanted vars
# ======================
done = False
varAddCounter = 0
while not done :
if varList :
varAddCounter += 1
curMsg = ' curVars : '
for ( i , curVar ) in enumerate( varList ) :
if i != 0 :
curMsg += ' , '
if int( fmod( i , 2 ) ) == 0 :
curMsg += ' \n '
curMsg += curVar.ljust( 14 )
if int( fmod( varAddCounter , 5 ) ) == 0 :
print varMsg
print curMsg + '\n'
varInput = raw_input( inputRequest )
print ''
# -------------------------------------
# check if varList has been completed
# -------------------------------------
if not varInput :
if varList :
done = True
else :
print '\n You need to insert at least one variable to hunt. \n'
continue
varInput = varInput.replace( ',' , '' )
varList.extend( varInput.split() )
return varList
def draw(self):
# speed defined here
h = math.fmod(self.time / 3, 2)
if h >= 1:
h = 2 - h
x = int(round(self.n))
offset = 1.0 / (len(self.text) + 1)
self.canvas.clear(*hsv_to_rgb(h, 1, 0.03))
h = math.fmod(h + offset, 1)
length = -1
for c in self.text:
length += letters[c].width + 1
x = (width - length + 1) / 2
for c in self.text:
r, g, b = hsv_to_rgb(h, 1, brightness)
h = math.fmod(h + offset, 1)
letter = letters[c]
self.canvas.add_letter(letter, x, 0, r, g, b)
x += letter.width + 1
if self.n > 15 or self.n < -15:
self.d = not self.d
def _mgrsString(zone, letters, easting, northing, precision):
""" Constructs an MGRS string from its component parts
@param zone - UTM zone
@param letters - MGRS coordinate string letters
@param easting - easting value
@param northing - northing value
@param precision - precision level of MGRS string
@returns - MGRS coordinate string
"""
mrgs = ''
if zone:
tmp = str(zone)
mgrs = tmp.zfill(3 - len(tmp))
else:
mgrs = ' '
for i in range(3):
mgrs += list(ALPHABET.keys())[list(ALPHABET.values()).index(letters[i])]
easting = math.fmod(easting + 1e-8, 100000.0)
if easting >= 99999.5:
easting = 99999.0
mgrs += str(int(easting)).rjust(5, '0')[:precision]
northing = math.fmod(northing + 1e-8, 100000.0)
if northing >= 99999.5:
northing = 99999.0
mgrs += str(int(northing)).rjust(5, '0')[:precision]
return mgrs
def halton(dim, nbpts):
"""
Generate `nbpts` points of the `dim`-dimensional Halton sequence.
Originally written in C by Sebastien Paris; translated to Python by
Josef Perktold.
"""
#pylint: disable=C0103
h = np.empty(nbpts * dim)
h.fill(np.nan)
p = np.empty(nbpts)
p.fill(np.nan)
P = [2, 3, 5, 7, 11, 13, 17, 19, 23, 29, 31]
if dim > len(P):
# For high-dimensional sequences, apply prime-number theorem to
# generate additional primes
P = _primes(int(dim * np.log(dim)))
lognbpts = log(nbpts + 1)
for i in range(dim):
b = P[i]
n = int(ceil(lognbpts / log(b)))
for t in range(n):
p[t] = pow(b, -(t + 1))
for j in range(nbpts):
d = j + 1
sum_ = fmod(d, b) * p[0]
for t in range(1, n):
d = floor(d / b)
sum_ += fmod(d, b) * p[t]
h[j*dim + i] = sum_
return h.reshape(nbpts, dim)
def spannstufe_koordinaten(self, start_run, end_run, depth):
"""Koordinaten fuer die Spannstufe werden berechnet
Anhand der maximalen Schnitttiefe werden die Koordinaten berechnet, die nachher zur Erzeugung des GCODES
benutzt werden.
:param start_run: Startkoordinate der aktuellen abzudrehenden Schicht, Wird mit jedem schnitt veraendert
:param end_run: Endkoordinate der aktuellen Stufe(hier die Spannstufe
:param depth: die maximale Schnitttiefe fuer die Bearbeitung
:return: Die Koordinaten der Spannstufe in einem Array, das wie folgt aufgebaut ist:
(((startx1,startz1),(endex1,endez1)schnittlaenge in mm, schnittdauer),...,
((startxn,startzn),(endexn,endezn)schnittlaenge in mm, schnittdauer)) fuer n Schnittebenen.
"""
block_area = 0
block_time = 0
end = []
area = 0
step = []
block_aufl = []
current_x = 0
current_z = 0
self.aufl_counter = 0
while(start_run[1] < end_run[1]):
index = 0
for i in self.old_profile:
index += 1
current_z = i[1]
if i[1] > start_run[1] :
break
current_x = i[0]
if round(math.fmod(end_run[1]-start_run[1], depth), 3) > 0.0:
end = [round(current_x-0.1, 3), round(start_run[1]+math.fmod(end_run[1]-start_run[1], depth), 3)]
for i in self.old_profile:
if i[1] < end[1] and i[0] < end[0]:
end[0] = round(i[0]-0.1, 3)
start_run = [start_run[0], round(start_run[1]+math.fmod(end_run[1]-start_run[1], depth), 3)]
if round(start_run[0]-end[0], 3) > round(0.1, 1):
area = round((start_run[0]-current_x-0.1), 3)
step_time = round(area/self.speed, 3)
step = [start_run, end, area, step_time]
block_area += area
block_time += step_time
self.aufl_counter += 1
block_aufl.append(step)
else:
end = [round(current_x-0.1, 3), round(start_run[1]+depth, 3)]
for i in self.old_profile:
if i[1] < end[1] and i[0] < end[0]:
end[0] = round(i[0]-0.1, 3)
start_run = [start_run[0], round(start_run[1]+depth, 3)]
if round(start_run[0]-end[0], 3) > round(0.1, 1):
area = round((start_run[0]-current_x-0.1), 3)
step_time = round(area/self.speed, 3)
step = [start_run, end, area, step_time]
block_area += area
block_time += step_time
self.aufl_counter += 1
block_aufl.append(step)
block_aufl.append(block_area)
block_aufl.append(block_time)
return block_aufl
def normalize(self): pi2 = 2 * pi self.start_angle = fmod(self.start_angle, pi2) if self.start_angle < 0: self.start_angle = self.start_angle + pi2 self.end_angle = fmod(self.end_angle, pi2) if self.end_angle < 0: self.end_angle = self.end_angle + pi2
def getLetter(c, k):
"""Take a number and turn it into a character"""
key = 27 - int(math.fmod(k, 27))
x = int(math.fmod(c+key, 27))
a = {0: 'a', 1: 'b', 2: 'c', 3: 'd', 4: 'e', 5: 'f', 6: 'g', 7: 'h', 8: 'i', 9: 'j', 10: 'k', 11: 'l', 12: 'm', 13: 'n', 14: 'o',
15: 'p', 16: 'q', 17: 'r', 18: 's', 19: 't', 20: 'u', 21: 'v', 22: 'w', 23: 'x', 24: 'y', 25: 'z'}
a = a.get(x, '')
return a
def mouseMotionFunc(self, x, y):
if (self.m_pickConstraint):
# move the constraint pivot
if (self.m_pickConstraint.getConstraintType() ==
bullet.D6_CONSTRAINT_TYPE):
print 'bullet.D6_CONSTRAINT_TYPE'
pickCon = bullet.btGeneric6DofConstraint.downcast(
self.m_pickConstraint)
if (pickCon):
# keep it at the same picking distance
newRayTo = self.getRayTo(x, y)
oldPivotInB = pickCon.getFrameOffsetA().getOrigin()
if (self.m_ortho):
newPivotB = oldPivotInB
newPivotB.setX(newRayTo.getX())
newPivotB.setY(newRayTo.getY())
else:
rayFrom = self.m_cameraPosition
dir = vector3.normalize(vector3.sub(newRayTo, rayFrom))
dir = vector3.mul(dir, self.m_oldPickingDist)
newPivotB = vector3.add(rayFrom, dir)
pickCon.getFrameOffsetA().setOrigin(newPivotB)
else:
print 'other'
pickCon = bullet.btPoint2PointConstraint.downcast(
self.m_pickConstraint)
if (pickCon):
# keep it at the same picking distance
newRayTo = self.getRayTo(x, y)
oldPivotInB = pickCon.getPivotInB()
if (self.m_ortho):
newPivotB = oldPivotInB
newPivotB.setX(newRayTo.getX())
newPivotB.setY(newRayTo.getY())
else:
rayFrom = self.m_cameraPosition
dir = vector3.normalize(vector3.sub(newRayTo, rayFrom))
dir = vector3.mul(dir, self.m_oldPickingDist)
newPivotB = vector3.add(rayFrom, dir)
pickCon.setPivotB(newPivotB)
dx = x - self.m_mouseOldX
dy = y - self.m_mouseOldY
print dx, dy
# only if ALT key is pressed (Maya style)
if (self.m_alt_key):
if (self.m_mouseButtons & 2):
hor = vector3.sub(self.getRayTo(0, 0), self.getRayTo(1, 0))
vert = vector3.sub(self.getRayTo(0, 0), self.getRayTo(0, 1))
multiplierX = 0.001
multiplierY = 0.001
if (self.m_ortho):
multiplierX = 1
multiplierY = 1
self.m_cameraTargetPosition = vector3.add(
self.m_cameraTargetPosition,
vector3.mul(hor, dx * multiplierX))
self.m_cameraTargetPosition = vector3.add(
self.m_cameraTargetPosition,
vector3.mul(vert, dy * multiplierY))
if (self.m_mouseButtons & (2 << 2) and self.m_mouseButtons & 1):
pass
elif (self.m_mouseButtons & 1):
self.m_azi += dx * 0.2
self.m_azi = math.fmod(self.m_azi, 360.0)
self.m_ele += dy * 0.2
self.m_ele = math.fmod(self.m_ele, 180.0)
elif (self.m_mouseButtons & 4):
self.m_cameraDistance -= dy * 0.020
if (self.m_cameraDistance < 0.1):
self.m_cameraDistance = 0.1
self.m_mouseOldX = x
self.m_mouseOldY = y
self.updateCamera()
'''
@Time : 2020/5/29 0:51
@Author : Mao Yuhuan
@FileName : 3.8 用Python改写语句并运行
@Software: PyCharm
'''
import math
print(math.sin(math.pi * 2))
print(math.floor(-2.5))
print(math.ceil(math.floor(-2.5) + 3.5))
print(round(math.fabs(-2.5)))
print(math.sqrt(math.pow(-2, 4)))
print(math.log(math.e))
print(math.gcd(12, 9))
print(math.fmod(36, 5))
scratch = env.scratchWorkspace
#Project doesn't like in_memory featureclasses, copy to scratch
copyInFeatures = os.path.join(scratch, "copyInFeatures")
arcpy.CopyFeatures_management(inFeature, copyInFeatures)
deleteme.append(copyInFeatures)
prjInFeature = os.path.join(scratch, "prjInFeature")
srInputPoints = arcpy.Describe(copyInFeatures).spatialReference
arcpy.AddMessage("Projecting input points to Web Mercator ...")
arcpy.Project_management(copyInFeatures, prjInFeature, webMercator)
deleteme.append(prjInFeature)
tempFans = os.path.join(scratch, "tempFans")
# put bearing into 0 - 360 range
geoBearing = math.fmod(geoBearing, 360.0)
if debug == True: arcpy.AddMessage("geoBearing: " + str(geoBearing))
arithmeticBearing = Geo2Arithmetic(
geoBearing
) # need to convert from geographic angles (zero north clockwise) to arithmetic (zero east counterclockwise)
if debug == True:
arcpy.AddMessage("arithmeticBearing: " + str(arithmeticBearing))
if traversal == 0.0:
traversal = 1.0 # modify so there is at least 1 degree of angle.
arcpy.AddWarning(
"Traversal is zero! Forcing traversal to 1.0 degrees.")
leftAngle = arithmeticBearing + (traversal / 2.0
) # get left angle (arithmetic)
leftBearing = geoBearing - (traversal / 2.0
) # get left bearing (geographic)
l = 0
k = 1
f = open('track_1.txt');
for line in f.readlines():
line_massive = line.split(',');
t.append(float(line_massive[0]))
x.append(line_massive[2]);
y.append(line_massive[3]);
try:
angle.append(math.degrees(math.atan2(float(line_massive[3]),float(line_massive[2]))));
except ValueError:
angle.append(angle[i-1])
i = i+1
newGrid[0] = ((float(t[0])*1000 - math.fmod(float(t[0])*1000, 50))/1000)
newGrid[1] = (newGrid[0]+ 0.05)
while newGrid[k] < (t[i-1]):
newGrid.append(newGrid[k-1]+ 0.05)
k = k+1
k = 0
while newGrid[k] < (t[i-1]):
newData.append(np.interp (newGrid[k],t,angle))
k = k+1
f.close()
f = open('results.txt', 'w');
f.write(strftime("%Y-%m-%d %H:%M:%S") + '\n')
def fn(f, y):
return math.fmod(f, y)
def draw(self, ctx):
self.progress.setValue(math.fmod(time.time() / 10, 1))
super(TestApp, self).draw(ctx)
def calc_rem_interval(base_task, inter_task):
rem_interval = math.fmod(base_task.deadline, inter_task.period)
return rem_interval
"starts programs until you type 'q'"
import os, math
test = ['hi', 'ya', 'there', 'bloke']
parm = 0
while True:
parm += 1
pid = os.fork()
if pid == 0: # copy process
os.execlp('python3', 'python3', 'child.py',\
str(test[int(math.fmod(parm,len(test)))]), str(parm)) # overlay program
assert False, 'error starting program' # shouldn't return
else:
print('Child is', pid)
if input() == 'q': break
def train():
cfg = args.cfg
data = args.data
if len(args.image_size) == 2:
image_size, image_size_val = args.image_size[0], args.image_size[1]
else:
image_size, image_size_val = args.image_size[0], args.image_size[0]
epochs = args.epochs
batch_size = args.batch_size
accumulate = args.accumulate
weights = args.weights
# Initialize
gs = 32 # (pixels) grid size
assert math.fmod(image_size,
gs) == 0, f"--image-size must be a {gs}-multiple"
init_seeds()
image_size_min = 6.6 # 320 / 32 / 1.5
image_size_max = 28.5 # 320 / 32 / 28.5
if args.multi_scale:
image_size_min = round(image_size / gs / 1.5) + 1
image_size_max = round(image_size / gs * 1.5)
image_size = image_size_max * gs # initiate with maximum multi_scale size
print(f"Using multi-scale {image_size_min * gs} - {image_size}")
# Configure run
dataset_dict = parse_data_config(data)
train_path = dataset_dict["train"]
valid_path = dataset_dict["valid"]
num_classes = 1 if args.single_cls else int(dataset_dict["classes"])
# Remove previous results
for files in glob.glob("results.txt"):
os.remove(files)
# Initialize model
model = Darknet(cfg).to(device)
# Optimizer
pg0, pg1, pg2 = [], [], [] # optimizer parameter groups
for model_key, model_value in dict(model.named_parameters()).items():
if ".bias" in model_key:
pg2 += [model_value] # biases
elif "Conv2d.weight" in model_key:
pg1 += [model_value] # apply weight_decay
else:
pg0 += [model_value] # all else
optimizer = torch.optim.SGD(pg0,
lr=parameters["lr0"],
momentum=parameters["momentum"],
nesterov=True)
optimizer.add_param_group({
"params": pg1,
# add pg1 with weight_decay
"weight_decay": parameters["weight_decay"]
})
optimizer.add_param_group({"params": pg2}) # add pg2 with biases
del pg0, pg1, pg2
epoch = 0
start_epoch = 0
best_fitness = 0.0
context = None
if weights.endswith(".pth"):
state = torch.load(weights, map_location=device)
# load model
try:
state["state_dict"] = {
k: v
for k, v in state["state_dict"].items()
if model.state_dict()[k].numel() == v.numel()
}
model.load_state_dict(state["state_dict"], strict=False)
except KeyError as e:
error_msg = f"{args.weights} is not compatible with {args.cfg}. "
error_msg += f"Specify --weights `` or specify a --cfg "
error_msg += f"compatible with {args.weights}. "
raise KeyError(error_msg) from e
# load optimizer
if state["optimizer"] is not None:
optimizer.load_state_dict(state["optimizer"])
best_fitness = state["best_fitness"]
# load results
if state.get("training_results") is not None:
with open("results.txt", "w") as file:
file.write(state["training_results"]) # write results.txt
start_epoch = state["epoch"] + 1
del state
elif len(weights) > 0:
# possible weights are "*.weights", "yolov3-tiny.conv.15", "darknet53.conv.74" etc.
load_darknet_weights(model, weights)
else:
print("Pre training model weight not loaded.")
# Mixed precision training https://github.com/NVIDIA/apex
if mixed_precision:
# skip print amp info
model, optimizer = amp.initialize(model,
optimizer,
opt_level="O1",
verbosity=0)
# source https://arxiv.org/pdf/1812.01187.pdf
lr_lambda = lambda x: ((
(1 + math.cos(x * math.pi / epochs)) / 2)**1.0) * 0.95 + 0.05
scheduler = torch.optim.lr_scheduler.LambdaLR(optimizer,
lr_lambda=lr_lambda,
last_epoch=start_epoch - 1)
# Initialize distributed training
if device.type != "cpu" and torch.cuda.device_count(
) > 1 and torch.distributed.is_available():
dist.init_process_group(
backend="nccl", # "distributed backend"
# distributed training init method
init_method="tcp://127.0.0.1:9999",
# number of nodes for distributed training
world_size=1,
# distributed training node rank
rank=0)
model = torch.nn.parallel.DistributedDataParallel(model)
model.yolo_layers = model.module.yolo_layers
# Dataset
# Apply augmentation hyperparameters (option: rectangular training)
train_dataset = LoadImagesAndLabels(train_path,
image_size,
batch_size,
augment=True,
hyp=parameters,
rect=args.rect,
cache_images=args.cache_images,
single_cls=args.single_cls)
# No apply augmentation hyperparameters and rectangular inference
valid_dataset = LoadImagesAndLabels(valid_path,
image_size_val,
batch_size,
augment=False,
hyp=parameters,
rect=True,
cache_images=args.cache_images,
single_cls=args.single_cls)
collate_fn = train_dataset.collate_fn
# Dataloader
train_dataloader = torch.utils.data.DataLoader(train_dataset,
batch_size=batch_size,
num_workers=args.workers,
shuffle=not args.rect,
pin_memory=True,
collate_fn=collate_fn)
valid_dataloader = torch.utils.data.DataLoader(valid_dataset,
batch_size=batch_size,
num_workers=args.workers,
shuffle=False,
pin_memory=True,
collate_fn=collate_fn)
# Model parameters
model.nc = num_classes # attach number of classes to model
model.hyp = parameters # attach hyperparameters to model
model.gr = 1.0 # giou loss ratio (obj_loss = 1.0 or giou)
# attach class weights
model.class_weights = labels_to_class_weights(train_dataset.labels,
num_classes).to(device)
# Model EMA
ema = ModelEMA(model, decay=0.9998)
# Start training
batches_num = len(train_dataloader) # number of batches
burns = max(3 * batches_num,
500) # burn-in iterations, max(3 epochs, 500 iterations)
maps = np.zeros(num_classes) # mAP per class
# "P", "R", "mAP", "F1", "val GIoU", "val Objectness", "val Classification"
results = (0, 0, 0, 0, 0, 0, 0)
print(f"Using {args.workers} dataloader workers.")
print(f"Starting training for {args.epochs} epochs...")
start_time = time.time()
for epoch in range(start_epoch, args.epochs):
model.train()
# Update image weights (optional)
if train_dataset.image_weights:
# class weights
class_weights = model.class_weights.cpu().numpy() * (1 - maps)**2
image_weights = labels_to_image_weights(
train_dataset.labels,
num_classes=num_classes,
class_weights=class_weights)
# rand weighted index
train_dataset.indices = random.choices(
range(train_dataset.image_files_num),
weights=image_weights,
k=train_dataset.image_files_num)
mean_losses = torch.zeros(4).to(device)
print("\n")
print(("%10s" * 8) % ("Epoch", "memory", "GIoU", "obj", "cls", "total",
"targets", " image_size"))
progress_bar = tqdm(enumerate(train_dataloader), total=batches_num)
for index, (images, targets, paths, _) in progress_bar:
# number integrated batches (since train start)
ni = index + batches_num * epoch
# uint8 to float32, 0 - 255 to 0.0 - 1.0
images = images.to(device).float() / 255.0
targets = targets.to(device)
# Hyperparameter Burn-in
if ni <= burns * 2:
# giou loss ratio (obj_loss = 1.0 or giou)
model.gr = np.interp(ni, [0, burns * 2], [0.0, 1.0])
for j, x in enumerate(optimizer.param_groups):
# bias lr falls from 0.1 to lr0, all other lrs rise from 0.0 to lr0
x["lr"] = np.interp(ni, [0, burns], [
0.1 if j == 2 else 0.0,
x["initial_lr"] * lr_lambda(epoch)
])
if "momentum" in x:
x["momentum"] = np.interp(
ni, [0, burns], [0.9, parameters["momentum"]])
# Multi-Scale training
if args.multi_scale:
# adjust img_size (67% - 150%) every 1 batch
if ni / accumulate % 1 == 0:
image_size = random.randrange(image_size_min,
image_size_max + 1) * gs
scale_ratio = image_size / max(images.shape[2:])
if scale_ratio != 1:
# new shape (stretched to 32-multiple)
new_size = [
math.ceil(size * scale_ratio / gs) * gs
for size in images.shape[2:]
]
images = F.interpolate(images,
size=new_size,
mode="bilinear",
align_corners=False)
# Run model
output = model(images)
# Compute loss
loss, loss_items = compute_loss(output, targets, model)
if not torch.isfinite(loss):
warnings.warn(
f"WARNING: Non-finite loss, ending training {loss_items}")
return results
# Scale loss by nominal batch_size of (16 * 4 = 64)
loss *= batch_size / (batch_size * accumulate)
# Compute gradient
if mixed_precision:
with amp.scale_loss(loss, optimizer) as scaled_loss:
scaled_loss.backward()
else:
loss.backward()
# Optimize accumulated gradient
if ni % accumulate == 0:
optimizer.step()
optimizer.zero_grad()
ema.update(model)
# Print batch results
# update mean losses
mean_losses = (mean_losses * index + loss_items) / (index + 1)
memory = f"{torch.cuda.memory_cached() / 1E9 if torch.cuda.is_available() else 0:.2f}G"
context = ("%10s" * 2 + "%10.3g" * 6) % ("%g/%g" %
(epoch, args.epochs - 1),
memory, *mean_losses,
len(targets), image_size)
progress_bar.set_description(context)
# Update scheduler
scheduler.step()
# Process epoch results
ema.update_attr(model)
final_epoch = epoch + 1 == epochs
if not args.notest or final_epoch: # Calculate mAP
coco = any([
coco_name in data for coco_name in
["coco.data", "coco2014.data", "coco2017.data"]
]) and model.nc == 80
results, maps = evaluate(cfg,
data,
batch_size=batch_size,
image_size=image_size_val,
model=ema.ema,
save_json=final_epoch and coco,
single_cls=args.single_cls,
dataloader=valid_dataloader)
# Write epoch results
with open("results.txt", "a") as f:
# P, R, mAP, F1, test_losses=(GIoU, obj, cls)
f.write(context + "%10.3g" * 7 % results)
f.write("\n")
# Write Tensorboard results
if tb_writer:
tags = [
"train/giou_loss", "train/obj_loss", "train/cls_loss",
"metrics/precision", "metrics/recall", "metrics/mAP_0.5",
"metrics/F1", "val/giou_loss", "val/obj_loss", "val/cls_loss"
]
for x, tag in zip(list(mean_losses[:-1]) + list(results), tags):
tb_writer.add_scalar(tag, x, epoch)
# Update best mAP
# fitness_i = weighted combination of [P, R, mAP, F1]
fitness_i = fitness(np.array(results).reshape(1, -1))
if fitness_i > best_fitness:
best_fitness = fitness_i
# Save training results
save = (not args.nosave) or (final_epoch and not args.evolve)
if save:
with open("results.txt", "r") as f:
# Create checkpoint
state = {
"epoch":
epoch,
"best_fitness":
best_fitness,
"training_results":
f.read(),
"state_dict":
ema.ema.module.state_dict()
if hasattr(model, "module") else ema.ema.state_dict(),
"optimizer":
None if final_epoch else optimizer.state_dict()
}
# Save last checkpoint
torch.save(state, "weights/checkpoint.pth")
# Save best checkpoint
if (best_fitness == fitness_i) and not final_epoch:
state = {
"epoch": -1,
"best_fitness": None,
"training_results": None,
"state_dict": model.state_dict(),
"optimizer": None
}
torch.save(state, "weights/model_best.pth")
# Delete checkpoint
del state
if not args.evolve:
plot_results() # save as results.png
print(f"{epoch - start_epoch} epochs completed "
f"in "
f"{(time.time() - start_time) / 3600:.3f} hours.\n")
dist.destroy_process_group() if torch.cuda.device_count() > 1 else None
torch.cuda.empty_cache()
return results
parameters = BilbyCustomFunctions_Reduction.FilesListReduce(csv_file_name)
files_to_reduce = BilbyCustomFunctions_Reduction.FilesToReduce(
parameters, index_files_to_reduce)
############################################
# Check of input wavelength range
if (wav1 + wav_delta) > wav2:
print('wav_delta is too large for the upper range of wavelength')
sys.exit()
############################################
#calculate number of steps n =============================================
if math.fmod((wav2 - wav1), wav_delta) == 0.0: # if reminder is 0
n = (wav2 - wav1) / wav_delta
else: # if reminder is greater than 0, to trancate the maximum wavelength in the range
n = math.floor((wav2 - wav1) / wav_delta)
max_wave_length = wav1 + n * wav_delta
print(
'\n WARNING: because of your set-up, maximum wavelength to consider is only %4.2f \n'
% max_wave_length)
n = int(n) # number of wavelength intervals
for current_file in files_to_reduce:
file_name = current_file['T_Sample'] + '.tar' # transmission sample
blocked_beam_name = current_file['T_BlockedBeam'] + '.tar' # blocked beam
ws_tranMsk = current_file[
'mask_transmission_estimate_multiple'] + '.xml' # transmission mask
import math
print("ceil(4.4)", math.ceil(4.4))
print("floor(4.4)", math.floor(4.4))
print("fabs(4.4)", math.fabs(4.4))
#Factorial = 1 * 2 * 3 * 4
print("factorial(4)", math.factorial(4))
#Return remainder of division
print("fmod(5, 4)", math.fmod(5, 4))
#Receive a float and return an int
print("trunc(4.2)", math.trunc(4.2))
#Return x^y
print("pow(2,2)", math.pow(2, 2))
#return the square root
print("sqrt(4)", math.sqrt(4))
#Special values
print("math.e = ", math.e)
print("math.pi = ", math.pi)
#return e^x
print("exp(4)", math.factorial(4))
#Return the natural locarithm e* e *e ~= 20 so log(20) tells
#you that e^3 ~=20
print("log(20) = ", math.log(20))
from itertools import combinations
from numpy import product
from operator import mul,add
import sys
from decimal import Decimal
from math import fmod
T=int(sys.stdin.readline())
M=10**9+7
for i in range(T):
N=int(sys.stdin.readline())
L=map(Decimal, sys.stdin.readline().split())
if len(L)==2:
A=L
res=(product(L)/sum(L))%M
else:
A=sum([map(list,combinations(L,x)) for x in range(2,N+1)],[])[1:]
R=map(lambda x:fmod(product(x)/sum(x),M),A)
print(R)
res=max(R)
print("Case #"+str(i+1)+": "+"%.f"%(res))
T-=1
def plot_dataset(trial_param_file, time_data_file, comment_str, pref_stim):
print(trial_param_file, time_data_file, pref_stim)
# Get information from the trial_data_file header
pfp = open(trial_param_file, 'r')
lines = pfp.readlines()
# check if first line is a header line starting with '#'
# This should be in the format:
#RUNID stim_delay stim_length trial_interval sample_length
header = lines[0].split()
if header[0][0] == "#":
RUNID = header[0][1:]
stim_delay = float(header[1])
stim_length = float(header[2])
trial_interval = float(header[3])
sample_length = float(header[4])
else:
print("No header information found!")
sys.exit()
# print RUNID, stim_delay, stim_length, trial_interval, sample_length
ntrials = len(lines) - 1
# count only the trials with this stimulus type
# allocate array space for the stimulus parameter data
trial_time = np.zeros(ntrials)
stim_type = np.zeros(ntrials)
# Then fill arrays from remaining lines
first_pref_trial = -1
for i in range(1, ntrials + 1):
data = lines[i].split()
j = i - 1 # trial number 0 is line 1
trial_time[j] = float(data[0])
stim_type[j] = int(data[1])
if (first_pref_trial < 0) and (stim_type[j] == pref_stim):
first_pref_trial = j
# print trial_time[j], stim_type[j]
pfp.close()
file_out = True
print('Reading %s' % time_data_file)
fp = open(time_data_file, 'r')
lines = fp.readlines()
count = len(lines)
print(count, " lines")
# determine size of the time step
line_0 = lines[0].split(" ")
line_1 = lines[1].split(" ")
dt = float(line_1[0]) - float(line_0[0])
print("time step = ", dt)
# determine size of the sample data
sample_items = int(sample_length / dt + 0.5) + 1
# Before the first trial, allocate space
tn = np.zeros(sample_items)
yn = np.zeros(sample_items)
# print len(tn), sample_items
# Now read the data
i = 0
trial_num = 0
nsamples = 0
line_num = 0
finished = False
# last trial to count is the one before final enty in trial_param_file
last_trial = ntrials - 2
trial_end = trial_time[trial_num + 1]
stype = stim_type[trial_num]
if stype == pref_stim:
nsamples += 1
for line in lines:
data = line.split(" ")
t = dt * line_num
line_num += 1
# see if we have passed the end of the trial
if t > trial_end:
if trial_num < last_trial:
# start over at the begining of the next sample
trial_num += 1
i = 0
trial_end = trial_time[trial_num + 1]
stype = stim_type[trial_num]
if stype == pref_stim:
nsamples += 1
else: # skip (likely incomplete) data for following trial
finished = True
sample_t = math.fmod(t, trial_interval)
# Add to the array if the sample time is within the sample_length
if not finished and (i < sample_items) and (stype == pref_stim):
# Note that tn[i] is replaced, and yn[i] is added to
tn[i] = sample_t
yn[i] = yn[i] + float(data[1])
i += 1
# end of loop over lines
if (nsamples < 1):
return
t_final = trial_end * trial_interval # run duration to print
# Average the data over number of samples having 'pref_stim' stim type
avg_LFP = yn / nsamples
# Option to subtract the base level LFP (averaged over t < stim_delay)
# from LFP(t)
normalize_baseline = True
n_base_samples = 0
LFPbase = 0.0
imax = int(stim_delay / dt)
if (normalize_baseline):
for i in range(0, imax):
LFPbase += yn[i]
n_base_samples += 1
LFPbase /= (n_base_samples * nsamples)
# print ("baseline average ", LFPbase, " over pref_stim ", pref_stim)
avg_LFP -= LFPbase
if (file_out):
outfile_name = 'LFP-out' + str(pref_stim) + '_' + time_data_file
print('Writing ', outfile_name)
outfp = open(outfile_name, 'w')
imax = int(sample_length / dt)
for i in range(0, imax):
outfp.write(str(tn[i]) + " " + str(avg_LFP[i]) + "\n")
# now do the calculation
print('alculating average of ', nsamples,
' preferred stimulus samples from ', RUNID)
print("number of trials = ", ntrials - 1, " preferred stimulus type = ",
pref_stim)
print('run duration (sec): ', t_final, ' data aquisition interval: ', dt)
# print run description to the "plot" ax3
text_str = 'Run ' + runid + ' with trial and stimulus parameters from: ' + \
trial_param_file +'\n' + 'summed Excitatory Local Field Potentials from: ' \
+ time_data_file + '\n' + str(nsamples) + ' preferred stimulus samples from ' + \
str(ntrials-1) + ' trials with preferred stiumulus type ' + str(pref_stim) + '\n' + \
'sample length (sec): ' + str(sample_length) + '; stimulus delay: ' + str(stim_delay) + \
'; pulse width: ' + str(stim_length) + '\n' + \
'trial interval: ' + str(trial_interval) + '; data interval: ' + str(dt) + \
'; run time ' + str(t_final) + '\n\n' + 'Comment: ' + comment_str
if (pref_stim == 1):
print(text_str)
print('N:{0}\nf:{1}\ne:{2}'.format(N,f,e))
"""
p=12347
q=13001
N=p*q
e=60728973
mas=[]
n=N
E=e
for i in range(0,20):
"""Дробь может быть бесконечной"""
mas.append(N//e)
if N%e==0:
break
e1=e
e=fmod(N,e)
N=e1
P,Q=[],[]
P.append(0)
P.append(1)
Q.append(0)
Q.append(0)
Q.append(1)
for i in range(2,len(mas)+2):
P.append(mas[i-2]*P[i-1]+P[i-2])
for i in range(2,len(mas)+1):
Q.append(mas[i-1]*Q[i]+Q[i-1])
#print(mas)
#print(P)
#print(Q)
def normalizeAngle(rad):
rad = math.fmod(rad, 2*math.pi)
if rad > math.pi:
rad -= math.pi
return rad
def normalize_angle(a):
a = math.fmod(a, 2. * math.pi)
return a if a >= 0. else a + 2. * math.pi
def SLC(k, f, e, X, V1, V2):
f0 = copy.deepcopy(f)
f1 = copy.deepcopy(f)
k1 = copy.deepcopy(k)
e1 = copy.deepcopy(e)
X1 = copy.deepcopy(X)
V1bis = copy.deepcopy(V1)
V2bis = copy.deepcopy(V2)
#initialisation E et norme E
E = np.zeros((N, Nbt), dtype=complex)
Enum = np.zeros((1, Nbt), dtype=complex)
#première colonne E et première valeur norme E
E[:, 0:1] = e
Enum[0] = np.linalg.norm(e1)
#calcul masse initiale
m_ini = 0
for k in range(N - 1):
for i in range(M1):
for j in range(M2):
m_ini += f1[k][i, j]
real_m_ini = m_ini * dx * dv1 * dv2
l = [0]
for t in range(1, Nbt):
start = time.time()
if (t % mod == 0):
print("Time=", t * dt, "et Niter=", t)
#affichage masse initiale
print(" masse initiale= ", real_m_ini / L)
#affichage masse à chaque instant
masse_non_norma = 0
for k in range(N - 1):
for i in range(M1 - 1):
for j in range(M2 - 1):
masse_non_norma += f1[k][i, j]
masse = masse_non_norma * dx * dv1 * dv2
print(" masse courante= ", masse / L)
print(" Erreur relative de masse= ",
(masse - real_m_ini) / real_m_ini)
masse_quadra = 0
for k in range(N - 1):
for i in range(M1 - 1):
for j in range(M2 - 1):
masse_quadra += abs(f1[k][i, j])**2
masse_quadra = masse_quadra * dx * dv1 * dv2
masse_quadra_E = 0
for k in range(N - 1):
masse_quadra_E += abs(E[k, t - 1:t])**2
masse_quadra_E = masse_quadra_E * dx
print(" énergie quadratique= ", masse_quadra + masse_quadra_E)
mf0 = [np.abs(np.max(f0[i])) for i in range(len(f1))]
mff0 = max(mf0)
f_diff = [f1[i] - f0[i] for i in range(len(f0))]
mf = [
max(np.abs(np.max(f_diff[i])), np.abs(np.min(f_diff[i])))
for i in range(len(f1))
]
#mf=[np.linalg.norm(f_diff[i]) for i in range(len(f1))]
mff = max(mf)
l.append(mff)
mE = linalg.norm(E[:, t - 1:t], np.inf)
print(" Max Densité f-f0= ", mff)
print(" Max Champ électrique E= ", mE)
if (t % modbis == 0):
Time = np.array([i * dt for i in range(t)])
Enumt = Enum[0, 0:t]
Ethet = 4 * 0.424666 * np.exp(-0.0661 * Time) * np.linalg.norm(
np.sin(0.4 * Xbis)) * np.cos(1.2850 * Time - 0.3357725)
plt.figure(figsize=(30, 20))
plt.plot(Time, np.log(Enumt), color='black', label=r'$E$ num')
axes = plt.gca()
axes.xaxis.set_ticks([i * t * dt / 10 for i in range(11)])
axes.xaxis.set_tick_params(length=5, width=3, labelsize=20)
axes.yaxis.set_tick_params(length=5, width=3, labelsize=20)
if flag == 2:
plt.plot(Time,
np.log(np.abs(Ethet)),
color='red',
label=r"$E$ theo $k=$" + str(k1))
plt.title(r'Landau Damping with $k=$' + str(k1), fontsize=40)
N_t = math.floor(t * dt / (L / dv1))
for i in range(1, N_t + 1):
plt.axvline(x=i * L / dv1, color='green')
if flag == 1:
plt.plot(Time,
np.log(np.abs(Ethet)),
color='red',
label=r"$E$ theo $k=$" + str(k))
plt.title(r'Landau-Bernstein paradox with $k=$' + str(k1) +
" et $\omega_c=$ " + str(omega_c),
fontsize=40)
N_t = math.floor(t * dt / (2 * np.pi / omega_c))
for i in range(1, N_t + 1):
plt.axvline(x=i * 2 * np.pi / omega_c, color='green')
plt.ylabel('Norm of the electric field', fontsize=30)
plt.xlabel('Time', fontsize=30)
plt.legend(loc='upper right', prop={'size': 20})
LocalDestinationPath = '/home/sidd/Bureau/Recherche/Landau Bernstein Scattering/Partie numérique' # Changer here for your local directory
os.chdir(LocalDestinationPath)
plt.savefig("Norme du Champ électrique jusqu'à l'iter " + str(t))
"""
"""
#résolution à v1 et v2 constants
for i in range(M1):
Xp = X1 - V1bis[i] * dt
#périodisation des pieds de caractéristiques
Xp = Xp - X1[0]
Xp = [math.fmod(x, X1[-1] - X1[0]) for x in Xp]
for p in range(len(Xp)):
if Xp[p] < 0:
Xp[p] += X1[-1]
else:
Xp[p] += X1[0]
"""
"""
#Xp=Xp+(Xp<0)*X1[-1]-(Xp>X1[-1])*X1[-1]
#print(Xp)
for j in range(M2):
fij = [f1[k][i, j] for k in range(N)]
fij[-1] = fij[0]
#interpolation par splines cubiques
a = scipy.interpolate.CubicSpline(X1, fij,
bc_type='periodic')(Xp)
for k in range(N):
f1[k][i, j] = a[k]
"""
masse_non_norma=0
for k in range(N-1):
for i in range(M1-1):
for j in range(M2-1):
masse_non_norma+=f1[k][i,j]
masse=masse_non_norma*dx*dv1*dv2
print(" masse courante phase 1= ",masse/L)
print(" Erreur relative de masse phase 1= ", (masse-real_m_ini)/real_m_ini)
"""
masse_quadra = 0
for k in range(N - 1):
for i in range(M1 - 1):
for j in range(M2 - 1):
masse_quadra += abs(f1[k][i, j])**2
masse_quadra = masse_quadra * dx * dv1 * dv2
masse_quadra_E = 0
for k in range(N - 1):
masse_quadra_E += abs(E[k, t - 1:t])**2
masse_quadra_E = masse_quadra_E * dx
print(" énergie quadratique phase 1= ",
masse_quadra + masse_quadra_E)
#résolution de Poisson
E[:, t:t + 1] = Poisson_trap(f1)
# print ('E=',Poisson_trap(dx,dv,f1))
if (t % mod == 0):
I = 0.
for j in range(N - 1):
I = I + E[:, t:t + 1][j]
#print (' Integrale E= ', I*dx)
Enum[0, t] = np.linalg.norm(E[0:N - 1, t:t + 1])
#résolution étape avec terme source
for k in range(N):
f1[k] = f1[k] - dt * second_membre(E[:, t:t + 1])[k]
masse_quadra = 0
for k in range(N - 1):
for i in range(M1 - 1):
for j in range(M2 - 1):
masse_quadra += abs(f1[k][i, j])**2
masse_quadra = masse_quadra * dx * dv1 * dv2
masse_quadra_E = 0
for k in range(N - 1):
masse_quadra_E += abs(E[k, t - 1:t])**2
masse_quadra_E = masse_quadra_E * dx
print(" énergie quadratique phase 2= ",
masse_quadra + masse_quadra_E)
#Seconde actualisation champ électrique
E[:, t:t + 1] = Poisson_trap(f1)
# print ('E=',Poisson_trap(dx,dv,f1))
if (t % mod == 0):
I = 0.
for j in range(N - 1):
I = I + E[:, t:t + 1][j]
#print (' Integrale E= ', I*dx)
Enum[0, t] = np.linalg.norm(E[0:N - 1, t:t + 1])
"""
"""
#résolution à x et v2 constants
for j in range(M2):
V1bisp = V1bis + omega_c * V2bis[j] * dt
#périodisation des pieds de caractéristiques
V1bisp = V1bisp - V1bis[0]
V1bisp = [math.fmod(x, V1bis[-1] - V1bis[0]) for x in V1bisp]
for p in range(len(V1bisp)):
if V1bisp[p] < 0:
V1bisp[p] += V1bis[-1]
else:
V1bisp[p] += V1bis[0]
"""
"""
#V1bisp=V1bisp+(V1bisp<V1bis[0])*(V1bis[-1]-V1bis[0])-(V1bisp>V1bis[-1])*(V1bis[-1]-V1bis[0])
for k in range(N):
fkj = [f1[k][i, j] for i in range(M1)]
fkj[0] = fkj[-1]
"""
for i in range(M1):
if (V1bisp[i]>=V1[-1] or V1bisp[i]<=V1[0]):
fkj[i]=0
"""
#interpolation par spline cubique
#a=scipy.interpolate.CubicSpline(V1bis,fkj,bc_type='clamped')(V1bisp)
a = scipy.interpolate.CubicSpline(V1bis,
fkj,
bc_type='periodic')(V1bisp)
f1[k][:, j:j + 1] = np.transpose(
np.array([[a[i] for i in range(M1)]]))
"""
masse_non_norma=0
for k in range(N-1):
for i in range(M1-1):
for j in range(M2-1):
masse_non_norma+=f1[k][i,j]
masse=masse_non_norma*dx*dv1*dv2
print(" masse courante phase 2= ",masse/L)
print(" Erreur relative de masse phase 2= ", (masse-real_m_ini)/real_m_ini)
"""
masse_quadra = 0
for k in range(N - 1):
for i in range(M1 - 1):
for j in range(M2 - 1):
masse_quadra += abs(f1[k][i, j])**2
masse_quadra = masse_quadra * dx * dv1 * dv2
masse_quadra_E = 0
for k in range(N - 1):
masse_quadra_E += abs(E[k, t - 1:t])**2
masse_quadra_E = masse_quadra_E * dx
print(" énergie quadratique phase 3= ",
masse_quadra + masse_quadra_E)
#résolution à x et v1 constants
for i in range(M1):
V2bisp = V2bis - omega_c * V1bis[i] * dt
#périodisation des pieds de caractéristiques
V2bisp = V2bisp - V2bis[0]
V2bisp = [math.fmod(x, V2bis[-1] - V2bis[0]) for x in V2bisp]
for p in range(len(V2bisp)):
if V2bisp[p] < 0:
V2bisp[p] += V2bis[-1]
else:
V2bisp[p] += V2bis[0]
#V2bisp=V2bisp+(V2bisp<V2bis[0])*(V2bis[-1]-V2bis[0])-(V2bisp>V2bis[-1])*(V2bis[-1]-V2bis[0])
for k in range(N):
fki = [f1[k][i, j] for j in range(M2)]
fki[0] = fki[-1]
"""
for j in range(M2):
if (V2bisp[j]>=V2[-1] or V2bisp[j]<=V2[0]):
fki[j]=0
"""
#interpolation par spline cubique
a = scipy.interpolate.CubicSpline(V2bis,
fki,
bc_type='periodic')(V2bisp)
f1[k][i:i + 1, :] = np.array([[a[j] for j in range(M2)]])
"""
masse_non_norma=0
for k in range(N-1):
for i in range(M1-1):
for j in range(M2-1):
masse_non_norma+=f1[k][i,j]
masse=masse_non_norma*dx*dv1*dv2
print(" masse courante phase 3= ",masse/L)
print(" Erreur relative de masse phase 3= ", (masse-real_m_ini)/real_m_ini)
"""
masse_quadra = 0
for k in range(N - 1):
for i in range(M1 - 1):
for j in range(M2 - 1):
masse_quadra += abs(f1[k][i, j])**2
masse_quadra = masse_quadra * dx * dv1 * dv2
masse_quadra_E = 0
for k in range(N - 1):
masse_quadra_E += abs(E[k, t - 1:t])**2
masse_quadra_E = masse_quadra_E * dx
print(" énergie quadratique phase 4= ",
masse_quadra + masse_quadra_E)
"""
if(t % mod==0):
fxv3=np.real(f0[n])
fxv4=np.imag(f0[n])
fxv5=np.absolute(f0[n])
fxv3end=np.real(f1[n])
fxv4end=np.imag(f1[n])
fxv5end=np.absolute(f1[n])
er=np.real(e1)
ei=np.imag(e1)
Erend=np.real(E[:,t:t+1])
Eiend=np.imag(E[:,t:t+1])
plt.figure()
plt.figure(figsize = (30, 20))
plt.subplot(2, 3, 1)
plt.pcolormesh(V2, V1, fxv3,cmap='RdBu')
plt.title("densité u initiale REELLE dans le plan V1-V2 pour x="+str(0))
plt.colorbar()
plt.ylabel('V2')
plt.xlabel('V1')
axes = plt.gca()
axes.xaxis.set_tick_params(length=5, width=3,labelsize=20)
axes.yaxis.set_tick_params(length=5, width=3,labelsize=20)
plt.legend()
plt.subplot(2, 3, 2)
plt.pcolormesh(V2, V1, np.cos(lambda_m*t*dt)*fxv3-np.sin(lambda_m*t*dt)*fxv4,cmap='RdBu')
plt.title("densité u théorique REELLE au temps "+str(t)+" dans le plan V1-V2 pour x="+str(0))
plt.colorbar()
plt.ylabel('V2')
plt.xlabel('V1')
axes = plt.gca()
axes.xaxis.set_tick_params(length=5, width=3,labelsize=20)
axes.yaxis.set_tick_params(length=5, width=3,labelsize=20)
plt.legend()
plt.subplot(2, 3, 3)
plt.pcolormesh(V2, V1, fxv3end,cmap='RdBu')
plt.title("densité u numérique REELLE au temps "+str(t)+" dans le plan V1-V2 pour x="+str(0))
plt.colorbar()
plt.ylabel('V2')
plt.xlabel('V1')
axes = plt.gca()
axes.xaxis.set_tick_params(length=5, width=3,labelsize=20)
axes.yaxis.set_tick_params(length=5, width=3,labelsize=20)
plt.legend()
plt.subplot(2, 3, 4)
plt.pcolormesh(V2, V1, fxv4,cmap='RdBu')
plt.title("densité u initiale IMAGINAIRE dans le plan V1-V2 pour x="+str(0))
plt.colorbar()
plt.ylabel('V2')
plt.xlabel('V1')
axes = plt.gca()
axes.xaxis.set_tick_params(length=5, width=3,labelsize=20)
axes.yaxis.set_tick_params(length=5, width=3,labelsize=20)
plt.legend()
plt.subplot(2, 3, 5)
plt.pcolormesh(V2, V1, np.sin(lambda_m*t*dt)*fxv3+np.cos(lambda_m*t*dt)*fxv4,cmap='RdBu')
plt.title("densité u théorique IMAGINAIRE au temps "+str(t)+" dans le plan V1-V2 pour x="+str(0))
plt.colorbar()
plt.ylabel('V2')
plt.xlabel('V1')
axes = plt.gca()
axes.xaxis.set_tick_params(length=5, width=3,labelsize=20)
axes.yaxis.set_tick_params(length=5, width=3,labelsize=20)
plt.legend()
plt.subplot(2, 3, 6)
plt.pcolormesh(V2, V1, fxv4end,cmap='RdBu')
plt.title("densité u numérique IMAGINAIRE au temps "+str(t)+" dans le plan V1-V2 pour x="+str(0))
plt.colorbar()
plt.ylabel('V2')
plt.xlabel('V1')
axes = plt.gca()
axes.xaxis.set_tick_params(length=5, width=3,labelsize=20)
axes.yaxis.set_tick_params(length=5, width=3,labelsize=20)
plt.legend()
LocalDestinationPath = '/home/sidd/Bureau/Programmation/Python/Images NumKin 2019/VPlin'
os.chdir(LocalDestinationPath)
plt.savefig("u_VP_"+str(t))
plt.figure()
plt.figure(figsize = (30, 20))
plt.subplot(2, 2, 1)
plt.pcolormesh(V2, V1, fxv5,cmap='RdBu')
plt.title("densité u initiale MODULE dans le plan V1-V2 pour x="+str(0))
plt.colorbar()
plt.ylabel('V2')
plt.xlabel('V1')
axes = plt.gca()
axes.xaxis.set_tick_params(length=5, width=3,labelsize=20)
axes.yaxis.set_tick_params(length=5, width=3,labelsize=20)
plt.legend()
plt.subplot(2, 2, 2)
plt.pcolormesh(V2, V1, fxv5end,cmap='RdBu')
plt.title("densité u numérique MODULE au temps "+str(t)+" dans le plan V1-V2 pour x="+str(0))
plt.colorbar()
plt.ylabel('V2')
plt.xlabel('V1')
axes = plt.gca()
axes.xaxis.set_tick_params(length=5, width=3,labelsize=20)
axes.yaxis.set_tick_params(length=5, width=3,labelsize=20)
plt.legend()
plt.subplot(2, 3, 4)
plt.plot(X, er,'x',label="initial")
plt.plot(X,np.cos(lambda_m*t*dt)*er-np.sin(lambda_m*t*dt)*ei,label="théorique au temps"+str(t))
plt.plot(X, Erend,label="numérique au temps"+str(t))
plt.title("champ électrique REELLE")
plt.ylabel('E réel')
plt.xlabel('X')
axes = plt.gca()
plt.xticks([0,np.pi/2, np.pi, 3*np.pi/2,2*np.pi], [r'$0$',r'$\frac{\pi}{2}$', r'$\pi$', r'$\frac{3\pi}{2}$', r'$2\pi$'])
axes.xaxis.set_tick_params(length=5, width=3,labelsize=20)
axes.yaxis.set_tick_params(length=5, width=3,labelsize=20)
plt.legend()
plt.grid()
plt.subplot(2, 3, 5)
plt.plot(X, ei,'x',label="initial")
plt.plot(X,np.sin(lambda_m*t*dt)*er+np.cos(lambda_m*t*dt)*ei,label="théorique au temps"+str(t))
plt.plot(X, Eiend,label="numérique au temps "+str(t))
plt.title("champ électrique IMAGINAIRE")
plt.ylabel('E imaginaire')
plt.xlabel('X')
axes = plt.gca()
plt.xticks([0,np.pi/2, np.pi, 3*np.pi/2,2*np.pi], [r'$0$',r'$\frac{\pi}{2}$', r'$\pi$', r'$\frac{3\pi}{2}$', r'$2\pi$'])
axes.xaxis.set_tick_params(length=5, width=3,labelsize=20)
axes.yaxis.set_tick_params(length=5, width=3,labelsize=20)
plt.legend()
plt.grid()
plt.subplot(2, 3, 6)
plt.axis([0,2*np.pi,0, 1.2])
plt.plot(X, np.absolute(er+1j*ei),label="initial")
#plt.plot(X,np.absolute(np.sin(lambda_m*T)*er+np.cos(lambda_m*T)*ei),label="théorique final")
plt.plot(X, np.absolute(E[:,t:t+1]),label="numérique au temps "+str(t))
plt.title("champ électrique MODULE")
plt.ylabel('E module')
plt.xlabel('X')
axes = plt.gca()
plt.xticks([0,np.pi/2, np.pi, 3*np.pi/2,2*np.pi], [r'$0$',r'$\frac{\pi}{2}$', r'$\pi$', r'$\frac{3\pi}{2}$', r'$2\pi$'])
axes.xaxis.set_tick_params(length=5, width=3,labelsize=20)
axes.yaxis.set_tick_params(length=5, width=3,labelsize=20)
plt.legend()
plt.grid()
LocalDestinationPath = '/home/sidd/Bureau/Programmation/Python/Images NumKin 2019/VPlin'
os.chdir(LocalDestinationPath)
plt.savefig("mu_F_VP_"+str(t))
"""
end = time.time()
print(" Elapsed for one iteration = %s" % (end - start))
return [E, Enum, f1]
def _compute_extra_keys(self):
"""Compute our extra keys."""
global unknown_string
self.extra_keys = {}
forecastTime = self.startStep
# regular or rotated grid?
try:
longitudeOfSouthernPoleInDegrees = \
self.longitudeOfSouthernPoleInDegrees
latitudeOfSouthernPoleInDegrees = \
self.latitudeOfSouthernPoleInDegrees
except AttributeError:
longitudeOfSouthernPoleInDegrees = 0.0
latitudeOfSouthernPoleInDegrees = 90.0
centre = gribapi.grib_get_string(self.grib_message, "centre")
# default values
self.extra_keys = {'_referenceDateTime': -1.0,
'_phenomenonDateTime': -1.0,
'_periodStartDateTime': -1.0,
'_periodEndDateTime': -1.0,
'_levelTypeName': unknown_string,
'_levelTypeUnits': unknown_string,
'_firstLevelTypeName': unknown_string,
'_firstLevelTypeUnits': unknown_string,
'_firstLevel': -1.0,
'_secondLevelTypeName': unknown_string,
'_secondLevel': -1.0,
'_originatingCentre': unknown_string,
'_forecastTime': None,
'_forecastTimeUnit': unknown_string,
'_coord_system': None,
'_x_circular': False,
'_x_coord_name': unknown_string,
'_y_coord_name': unknown_string,
# These are here to avoid repetition in the rules
# files, and reduce the very long line lengths.
'_x_points': None,
'_y_points': None,
'_cf_data': None}
# cf phenomenon translation
# Get centre code (N.B. self.centre has default type = string)
centre_number = gribapi.grib_get_long(self.grib_message, "centre")
# Look for a known grib1-to-cf translation (or None).
cf_data = gptx.grib1_phenom_to_cf_info(
table2_version=self.table2Version,
centre_number=centre_number,
param_number=self.indicatorOfParameter)
self.extra_keys['_cf_data'] = cf_data
# reference date
self.extra_keys['_referenceDateTime'] = \
datetime.datetime(int(self.year), int(self.month), int(self.day),
int(self.hour), int(self.minute))
# forecast time with workarounds
self.extra_keys['_forecastTime'] = forecastTime
# verification date
processingDone = self._get_processing_done()
# time processed?
if processingDone.startswith("time"):
validityDate = str(self.validityDate)
validityTime = "{:04}".format(int(self.validityTime))
endYear = int(validityDate[:4])
endMonth = int(validityDate[4:6])
endDay = int(validityDate[6:8])
endHour = int(validityTime[:2])
endMinute = int(validityTime[2:4])
# fixed forecastTime in hours
self.extra_keys['_periodStartDateTime'] = \
(self.extra_keys['_referenceDateTime'] +
datetime.timedelta(hours=int(forecastTime)))
self.extra_keys['_periodEndDateTime'] = \
datetime.datetime(endYear, endMonth, endDay, endHour,
endMinute)
else:
self.extra_keys['_phenomenonDateTime'] = \
self._get_verification_date()
# originating centre
# TODO #574 Expand to include sub-centre
self.extra_keys['_originatingCentre'] = CENTRE_TITLES.get(
centre, "unknown centre %s" % centre)
# forecast time unit as a cm string
# TODO #575 Do we want PP or GRIB style forecast delta?
self.extra_keys['_forecastTimeUnit'] = self._timeunit_string()
# shape of the earth
# pre-defined sphere
if self.shapeOfTheEarth == 0:
geoid = coord_systems.GeogCS(semi_major_axis=6367470)
# custom sphere
elif self.shapeOfTheEarth == 1:
geoid = coord_systems.GeogCS(
self.scaledValueOfRadiusOfSphericalEarth *
10 ** -self.scaleFactorOfRadiusOfSphericalEarth)
# IAU65 oblate sphere
elif self.shapeOfTheEarth == 2:
geoid = coord_systems.GeogCS(6378160, inverse_flattening=297.0)
# custom oblate spheroid (km)
elif self.shapeOfTheEarth == 3:
geoid = coord_systems.GeogCS(
semi_major_axis=self.scaledValueOfEarthMajorAxis *
10 ** -self.scaleFactorOfEarthMajorAxis * 1000.,
semi_minor_axis=self.scaledValueOfEarthMinorAxis *
10 ** -self.scaleFactorOfEarthMinorAxis * 1000.)
# IAG-GRS80 oblate spheroid
elif self.shapeOfTheEarth == 4:
geoid = coord_systems.GeogCS(6378137, None, 298.257222101)
# WGS84
elif self.shapeOfTheEarth == 5:
geoid = \
coord_systems.GeogCS(6378137, inverse_flattening=298.257223563)
# pre-defined sphere
elif self.shapeOfTheEarth == 6:
geoid = coord_systems.GeogCS(6371229)
# custom oblate spheroid (m)
elif self.shapeOfTheEarth == 7:
geoid = coord_systems.GeogCS(
semi_major_axis=self.scaledValueOfEarthMajorAxis *
10 ** -self.scaleFactorOfEarthMajorAxis,
semi_minor_axis=self.scaledValueOfEarthMinorAxis *
10 ** -self.scaleFactorOfEarthMinorAxis)
elif self.shapeOfTheEarth == 8:
raise ValueError("unhandled shape of earth : grib earth shape = 8")
else:
raise ValueError("undefined shape of earth")
gridType = gribapi.grib_get_string(self.grib_message, "gridType")
if gridType in ["regular_ll", "regular_gg", "reduced_ll",
"reduced_gg"]:
self.extra_keys['_x_coord_name'] = "longitude"
self.extra_keys['_y_coord_name'] = "latitude"
self.extra_keys['_coord_system'] = geoid
elif gridType == 'rotated_ll':
# TODO: Confirm the translation from angleOfRotation to
# north_pole_lon (usually 0 for both)
self.extra_keys['_x_coord_name'] = "grid_longitude"
self.extra_keys['_y_coord_name'] = "grid_latitude"
southPoleLon = longitudeOfSouthernPoleInDegrees
southPoleLat = latitudeOfSouthernPoleInDegrees
self.extra_keys['_coord_system'] = \
coord_systems.RotatedGeogCS(
-southPoleLat,
math.fmod(southPoleLon + 180.0, 360.0),
self.angleOfRotation, geoid)
elif gridType == 'polar_stereographic':
self.extra_keys['_x_coord_name'] = "projection_x_coordinate"
self.extra_keys['_y_coord_name'] = "projection_y_coordinate"
if self.projectionCentreFlag == 0:
pole_lat = 90
elif self.projectionCentreFlag == 1:
pole_lat = -90
else:
raise TranslationError("Unhandled projectionCentreFlag")
# Note: I think the grib api defaults LaDInDegrees to 60 for grib1.
self.extra_keys['_coord_system'] = \
coord_systems.Stereographic(
pole_lat, self.orientationOfTheGridInDegrees, 0, 0,
self.LaDInDegrees, ellipsoid=geoid)
elif gridType == 'lambert':
self.extra_keys['_x_coord_name'] = "projection_x_coordinate"
self.extra_keys['_y_coord_name'] = "projection_y_coordinate"
flag_name = "projectionCenterFlag"
if getattr(self, flag_name) == 0:
pole_lat = 90
elif getattr(self, flag_name) == 1:
pole_lat = -90
else:
raise TranslationError("Unhandled projectionCentreFlag")
LambertConformal = coord_systems.LambertConformal
self.extra_keys['_coord_system'] = LambertConformal(
self.LaDInDegrees, self.LoVInDegrees, 0, 0,
secant_latitudes=(self.Latin1InDegrees, self.Latin2InDegrees),
ellipsoid=geoid)
else:
raise TranslationError("unhandled grid type: {}".format(gridType))
if gridType in ["regular_ll", "rotated_ll"]:
self._regular_longitude_common()
j_step = self.jDirectionIncrementInDegrees
if not self.jScansPositively:
j_step = -j_step
self._y_points = (np.arange(self.Nj, dtype=np.float64) * j_step +
self.latitudeOfFirstGridPointInDegrees)
elif gridType in ['regular_gg']:
# longitude coordinate is straight-forward
self._regular_longitude_common()
# get the distinct latitudes, and make sure they are sorted
# (south-to-north) and then put them in the right direction
# depending on the scan direction
latitude_points = gribapi.grib_get_double_array(
self.grib_message, 'distinctLatitudes').astype(np.float64)
latitude_points.sort()
if not self.jScansPositively:
# we require latitudes north-to-south
self._y_points = latitude_points[::-1]
else:
self._y_points = latitude_points
elif gridType in ["polar_stereographic", "lambert"]:
# convert the starting latlon into meters
cartopy_crs = self.extra_keys['_coord_system'].as_cartopy_crs()
x1, y1 = cartopy_crs.transform_point(
self.longitudeOfFirstGridPointInDegrees,
self.latitudeOfFirstGridPointInDegrees,
ccrs.Geodetic())
if not np.all(np.isfinite([x1, y1])):
raise TranslationError("Could not determine the first latitude"
" and/or longitude grid point.")
self._x_points = x1 + self.DxInMetres * np.arange(self.Nx,
dtype=np.float64)
self._y_points = y1 + self.DyInMetres * np.arange(self.Ny,
dtype=np.float64)
elif gridType in ["reduced_ll", "reduced_gg"]:
self._x_points = self.longitudes
self._y_points = self.latitudes
else:
raise TranslationError("unhandled grid type")
def phi(self, phi):
self._set_orientation(math.fmod(self._theta, 360.0), math.fmod(phi, 360.0))
def measureKronInPython(self,
objImg,
xcen,
ycen,
nsigma,
kfac,
nIterForRadius,
makeImage=None):
"""Measure the Kron quantities of an elliptical Gaussian in python.
N.b. only works for XY0 == (0, 0)
"""
#
# Measure moments using SDSS shape algorithm
#
# Note: this code was converted to the new meas_framework, but is not exercised.
msConfig = makeMeasurementConfig(False, nsigma, nIterForRadius, kfac)
center = geom.Point2D(xcen, ycen)
source = self.measureFree(objImg, center, msConfig)
algMeta = source.getTable().getMetadata()
self.assertTrue(
algMeta.exists('EXT_PHOTOMETRYKRON_KRONFLUX_NRADIUSFORFLUX'))
Mxx = source.getIxx()
Mxy = source.getIxy()
Myy = source.getIyy()
#
# Calculate principal axes
#
Muu_p_Mvv = Mxx + Myy
Muu_m_Mvv = math.sqrt((Mxx - Myy)**2 + 4 * Mxy**2)
Muu = 0.5 * (Muu_p_Mvv + Muu_m_Mvv)
Mvv = 0.5 * (Muu_p_Mvv - Muu_m_Mvv)
theta = 0.5 * math.atan2(2 * Mxy, Mxx - Myy)
a = math.sqrt(Muu)
b = math.sqrt(Mvv)
ab = a / b
#
# Get footprint
#
ellipse = afwEllipses.Ellipse(
afwEllipses.Axes(nsigma * a, nsigma * b, theta),
geom.Point2D(xcen, ycen))
fpEllipse = afwDetection.Footprint(ellipse)
sumI = 0.0
sumR = (0.38259771140356325 / ab *
(1 + math.sqrt(2) *
math.hypot(math.fmod(xcen, 1), math.fmod(ycen, 1))) *
objImg.image[int(xcen), int(ycen), afwImage.LOCAL])
gal = objImg.image
c, s = math.cos(theta), math.sin(theta)
for sp in fpEllipse.getSpans():
y, x0, x1 = sp.getY(), sp.getX0(), sp.getX1()
for x in range(x0, x1 + 1):
dx, dy = x - xcen, y - ycen
u = c * dx + s * dy
v = -s * dx + c * dy
r = math.hypot(u, v * ab)
try:
val = gal[x, y, afwImage.LOCAL]
except Exception:
continue
sumI += val
sumR += val * r
R_K = sumR / sumI
sumI = 0.0
for y in range(self.height):
for x in range(self.width):
dx, dy = x - xcen, y - ycen
u = c * dx + s * dy
v = -s * dx + c * dy
if math.hypot(u / a, v / b) < kfac:
sumI += gal[x, y, afwImage.LOCAL]
return R_K, sumI, 0, False, False, False
print('ceil(x) Return the smallest integral value >= x')
for x in [0, 0.01, 0.49, 0.5, 0.51, 0.9, -0.9, -0.5, -0.1]:
ceiled_x = math.ceil(x)
print('ceil({0: 6.2f}) = {1: 6.2f}'.format(x, ceiled_x))
# floor(x) Return the floor of x as a float. This is the largest integral value <= x.
print('floor(x) Return the largest integral value <= x')
for x in [-1.1, -0.9, -0.1, 0, 0.1, 0.9, 1.1]:
print('x={0: 6.4f}, math.floor(x)={1: 6.4f}'.format(x, math.floor(x)))
# fabs(x) Return the absolute value of the float x.
for x in [-2, -0.5, 0, 2, 4.5]:
print('x = {0}, math.fabs(x) = {1}'.format(x, math.fabs(x)))
# fmod(x, y) Return fmod(x, y), according to platform C. x % y may differ.
print('\nmath.fmod(10, 3):', math.fmod(10, 3))
print('10 % 3:', 10 % 3)
# factorial(x) -> Integral Find x!. Raise a ValueError if x is negative or non-integral.
print('\nmath.factorial(5) =', math.factorial(5))
# fsum(iterable) Return an accurate floating point sum of values in the iterable. Assumes IEEE-754 floating point arithmetic.
print('\nmath.fsum(range(1, 5)) = 1+2+3+4 =', math.fsum(range(1, 5)))
# modf(x) Return the fractional and integer parts of x. Both results carry the sign of x and are floats.
print('\nmath.modf(2.5) =', math.modf(2.5))
# isinf(x) -> bool Check if float x is infinite (positive or negative).
# isnan(x) -> bool Check if float x is not a number (NaN).
# pow(x, y) Return x**y (x to the power of y).
def theta(self, theta):
self._set_orientation(math.fmod(theta, 360.0), math.fmod(self._phi, 360.0))
def __init__(self, windSpeedMetersPerSecond, windDirectionDegrees):
assert (windSpeedMetersPerSecond >= 0.0)
assert (windDirectionDegrees >= 0.0) and (windDirectionDegrees <= 360.0)
self.windSpeedMetersPerSecond = windSpeedMetersPerSecond
self.windDirectionDegrees = math.fmod(windDirectionDegrees + 180.0, 360.0)
def get_point(self, degree):
angle_from_start = (self.ccw * 2 - 1) * self.rad_len * degree
angle = math.fmod(self.rad_start + angle_from_start + 2 * math.pi, 2 * math.pi)
return self.center + self.radius * np.array([math.cos(angle), math.sin(angle)])
def stairs(t, n_stair=10, dt_stair=0.5, _min=0, _max=20):
a = int(math.fmod(t, dt_stair * n_stair) / dt_stair)
return _min + (_max - _min) * a / n_stair
def CWOA(objf,lb,ub,dim,SearchAgents_no,Max_iter):
#dim=30
#SearchAgents_no=50
#lb=-100
#ub=100
#Max_iter=500
if not isinstance(lb, list):
lb = [lb] * dim
if not isinstance(ub, list):
ub = [ub] * dim
# initialize position vector and score for the leader
Leader_pos=numpy.zeros(dim)
Leader_score=float("inf") #change this to -inf for maximization problems
#Initialize the positions of search agents
Positions = numpy.zeros((SearchAgents_no, dim))
for i in range(dim):
Positions[:, i] = numpy.random.uniform(0,1,SearchAgents_no) *(ub[i]-lb[i])+lb[i]
#Initialize convergence
convergence_curve=numpy.zeros(Max_iter)
############################
s=solution()
print("CWOA is optimizing \""+objf.__name__+"\"")
timerStart=time.time()
s.startTime=time.strftime("%Y-%m-%d-%H-%M-%S")
############################
t=0 # Loop counter
# Main loop
while t<Max_iter:
for i in range(0,SearchAgents_no):
# Return back the search agents that go beyond the boundaries of the search space
#Positions[i,:]=checkBounds(Positions[i,:],lb,ub)
for j in range(dim):
Positions[i,j]=numpy.clip(Positions[i,j], lb[j], ub[j])
# Calculate objective function for each search agent
fitness=objf(Positions[i,:])
# Update the leader
if fitness<Leader_score: # Change this to > for maximization problem
Leader_score=fitness; # Update alpha
Leader_pos=Positions[i,:].copy() # copy current whale position into the leader position
a=2-t*((2)/Max_iter); # a decreases linearly fron 2 to 0 in Eq. (2.3)
# a2 linearly decreases from -1 to -2 to calculate t in Eq. (3.12)
a2=-1+t*((-1)/Max_iter);
# Update the Position of search agents
for i in range(0,SearchAgents_no):
r1=random.random() # r1 is a random number in [0,1]
r2=random.random() # r2 is a random number in [0,1]
A=2*a*r1-a # Eq. (2.3) in the paper
C=2*r2 # Eq. (2.4) in the paper
b=1; # parameters in Eq. (2.5)
l=(a2-1)*random.random()+1 # parameters in Eq. (2.5)
p = random.random() # p in Eq. (2.6)
# Chaotic maps
# cm = numpy.random.choice(numpy.arange(8))
cm = 8
if cm == 1:
# Logistic
Positions[i,j] = a*Positions[i,j]*(1-Positions[i,j])
elif cm == 2:
# Cubic
Positions[i,j] = a*Positions[i,j]*(1-(Positions[i,j]**2))
elif cm == 3:
# Sine
Positions[i,j] = (a/4)*math.sin(math.pi*Positions[i,j])
elif cm == 4:
# Sinusoidal
Positions[i,j] = a*(Positions[i,j]**2)*math.sin(math.pi*Positions[i,j])
elif cm == 5:
# Singer
u = 1.07
Positions[i,j] = u*(7.86*Positions[i,j]-23.31*(Positions[i,j]**2)+28.75*(Positions[i,j]**3)-13.302875*(Positions[i,j]**4))
elif cm == 6:
# Circle
b = 1
k = dim -1
Positions[i,j] = math.fmod(Positions[i,j]+b-(a/2*math.pi)*math.sin(2*math.pi*Positions[i,k]), 1)
elif cm == 7:
# Iterative
Positions[i,j] = math.sin((a*math.pi)/Positions[i,j])
elif cm == 8:
# Tent Chaotic Map
if(Positions[i,j] < 0.7):
Positions[i,j] = Positions[i,j] / 0.7
else:
Positions[i,j] = (10/3)*(1-Positions[i,j])
for j in range(0,dim):
if p<0.5:
if abs(A)>=1:
rand_leader_index = math.floor(SearchAgents_no*random.random());
X_rand = Positions[rand_leader_index, :]
D_X_rand=abs(C*X_rand[j]-Positions[i,j])
Positions[i,j]=X_rand[j]-A*D_X_rand
elif abs(A)<1:
D_Leader=abs(C*Leader_pos[j]-Positions[i,j])
Positions[i,j]=Leader_pos[j]-A*D_Leader
elif p>=0.5:
distance2Leader=abs(Leader_pos[j]-Positions[i,j])
# Eq. (2.5)
Positions[i,j]=distance2Leader*math.exp(b*l)*math.cos(l*2*math.pi)+Leader_pos[j]
convergence_curve[t]=Leader_score
if (t%1==0):
print(['At iteration '+ str(t)+ ' the best fitness is '+ str(Leader_score)]);
t=t+1
timerEnd=time.time()
s.endTime=time.strftime("%Y-%m-%d-%H-%M-%S")
s.executionTime=timerEnd-timerStart
s.convergence=convergence_curve
s.optimizer="CWOA"
s.objfname=objf.__name__
s.best = Leader_score
s.bestIndividual = Leader_pos
s.std = numpy.std(convergence_curve)
s.mean = numpy.average(convergence_curve)
return s
import math
print('{:^4} {:^4} {:^5} {:^5}'.format('x', 'y', '%', 'fmod'))
print('{:-^4} {:-^4} {:-^5} {:-^5}'.format('-', '-', '-', '-'))
INPUTS = [
(5, 2),
(5, -2),
(-5, 2),
]
for x, y in INPUTS:
print('{:4.1f} {:4.1f} {:5.2f} {:5.2f}'.format(
x,
y,
x % y,
math.fmod(x, y),
))
def testFmod(self):
self.assertRaises(TypeError, math.fmod)
self.ftest('fmod(10,1)', math.fmod(10,1), 0)
self.ftest('fmod(10,0.5)', math.fmod(10,0.5), 0)
self.ftest('fmod(10,1.5)', math.fmod(10,1.5), 1)
self.ftest('fmod(-10,1)', math.fmod(-10,1), 0)
self.ftest('fmod(-10,0.5)', math.fmod(-10,0.5), 0)
self.ftest('fmod(-10,1.5)', math.fmod(-10,1.5), -1)
self.assertTrue(math.isnan(math.fmod(NAN, 1.)))
self.assertTrue(math.isnan(math.fmod(1., NAN)))
self.assertTrue(math.isnan(math.fmod(NAN, NAN)))
self.assertRaises(ValueError, math.fmod, 1., 0.)
self.assertRaises(ValueError, math.fmod, INF, 1.)
self.assertRaises(ValueError, math.fmod, NINF, 1.)
self.assertRaises(ValueError, math.fmod, INF, 0.)
self.assertEqual(math.fmod(3.0, INF), 3.0)
self.assertEqual(math.fmod(-3.0, INF), -3.0)
self.assertEqual(math.fmod(3.0, NINF), 3.0)
self.assertEqual(math.fmod(-3.0, NINF), -3.0)
self.assertEqual(math.fmod(0.0, 3.0), 0.0)
self.assertEqual(math.fmod(0.0, NINF), 0.0)
def step(t, a0=-1, a1=1, dt=4, t0=0):
return a0 if math.fmod(t + t0, dt) > dt / 2 else a1
def intersection_point(a_lat,
a_lon,
a_bearing,
b_lat,
b_lon,
b_bearing,
debug=False):
a_lat = math.radians(a_lat)
a_lon = math.radians(a_lon)
b_lat = math.radians(b_lat)
b_lon = math.radians(b_lon)
brng13 = math.radians(a_bearing)
brng23 = math.radians(b_bearing)
dLat = (b_lat - a_lat)
dLon = (b_lon - a_lon)
dist12 = 2.0 * math.asin(
math.sqrt(
math.sin(dLat / 2.0) * math.sin(dLat / 2.0) + math.cos(a_lat) *
math.cos(b_lat) * math.sin(dLon / 2.0) * math.sin(dLon / 2.0)))
if (dist12 == 0.0):
if (debug): print "Intersection ERROR: points are too close!"
return None
# initial/final bearings between points
try:
brngA = math.acos(
(math.sin(b_lat) - math.sin(a_lat) * math.cos(dist12)) /
(math.sin(dist12) * math.cos(a_lat)))
except Exception as inst:
if (debug): print "Intersection EXCEPTION: " + str(inst)
return None
# protect against rounding
if (math.isnan(brngA)):
brngA = 0.0
try:
brngB = math.acos(
(math.sin(a_lat) - math.sin(b_lat) * math.cos(dist12)) /
(math.sin(dist12) * math.cos(b_lat)))
except Exception as inst:
if (debug): print "Intersection EXCEPTION: " + str(inst)
return None
if (math.sin(b_lon - a_lon) > 0):
brng12 = brngA
brng21 = 2.0 * math.pi - brngB
else:
brng12 = 2.0 * math.pi - brngA
brng21 = brngB
alpha1 = (brng13 - brng12 + math.pi) % (2.0 * math.pi) - math.pi
alpha2 = (brng21 - brng23 + math.pi) % (2.0 * math.pi) - math.pi
# infinite intersections
if ((math.sin(alpha1) == 0.0) and (math.sin(alpha2) == 0.0)):
if (debug): print "Intersection ERROR: infinite intersections!"
return None
# ambiguous intersection
if ((math.sin(alpha1) * math.sin(alpha2)) < 0.0):
if (debug): print "Intersection ERROR: ambiguous intersection!"
return None
alpha3 = math.acos(-1.0 * math.cos(alpha1) * math.cos(alpha2) +
math.sin(alpha1) * math.sin(alpha2) * math.cos(dist12))
dist13 = math.atan2(
math.sin(dist12) * math.sin(alpha1) * math.sin(alpha2),
math.cos(alpha2) + math.cos(alpha1) * math.cos(alpha3))
c_lat = math.asin(
math.sin(a_lat) * math.cos(dist13) +
math.cos(a_lat) * math.sin(dist13) * math.cos(brng13))
dLon13 = math.atan2(
math.sin(brng13) * math.sin(dist13) * math.cos(a_lat),
math.cos(dist13) - math.sin(a_lat) * math.sin(c_lat))
c_lon = a_lon + dLon13
c_lon = math.fmod((c_lon + math.pi), (2.0 * math.pi)) - math.pi
return (math.degrees(c_lat), math.degrees(c_lon))
