예제 #1
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gridtype = 'gaussian'
dt = 3600. # time step in seconds
rsphere = 6.37122e6 # earth radius

# fix random seed for reproducibility.
np.random.seed(42)

# model nature run to sample initial ensemble and draw additive noise.
modelclimo_file = 'truth_twolevel_t%s_12h.nc' % ntrunc
# 'truth' nature run to sample obs
# (these two files can be the same for perfect model expts)
# file to sample additive noise.
truth_file = 'truth_twolevel_t32_12h.nc'

# create spherical harmonic transform instance
sp = Spharmt(nlons,nlats,ntrunc,rsphere,gridtype=gridtype)
spout = sp

models = []
for nanal in range(nanals):
    models.append(TwoLevel(sp,dt))

# weights for computing global means.
globalmeanwts = models[0].globalmeanwts

# read nature run, create obs.
nct = Dataset(truth_file)
lats = nct.variables['lat'][:]
lons = nct.variables['lon'][:]
spin = Spharmt(len(lons),len(lats),int(nct.ntrunc),rsphere,gridtype=gridtype)
samegrid = spin.nlons == spout.nlons and spin.nlats == spout.nlats
예제 #2
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#ntrunc = 64
#dt = 1800. # time step in seconds

nlons = 96
nlats = nlons / 2  # number of longitudes/latitudes
ntrunc = 32
dt = 3600.  # time step in seconds

fhout = 12.  # output interval (hours)

gridtype = 'gaussian'  # 'regular' or 'gaussian'
output_file = 'truth_twolevel_t%s_%sh_tst.nc' % (ntrunc, int(fhout))

# create spherical harmonic instance.
rsphere = 6.37122e6  # earth radius
sp = Spharmt(nlons, nlats, ntrunc, rsphere, gridtype=gridtype)

nstart = int((200. * 86400.) / dt)  # end of spinup period
nmax = int((1300. * 86400.) / dt)  # total duration of run

# create model instance
model = TwoLevel(sp, dt)
print 'pole/equator temp diff = ', model.thetaref.max() - model.thetaref.min()

# vort, div initial conditions
psipert = np.zeros((2, model.nlat, model.nlon), np.float)
psipert[1, :, :] = 5.e6 * np.sin(
    (model.lons - np.pi))**12 * np.sin(2. * model.lats)**12
psipert = np.where(model.lons[np.newaxis, :, :] > 0., 0, psipert)
psipert[1, :, :] += np.random.normal(scale=1.e6, size=(sp.nlats, sp.nlons))
ug = np.zeros((2, model.nlat, model.nlon), np.float)
예제 #3
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            varspect[indxn[n]] += norm[n] * vrtmag
            varspect[indxn[n]] += norm[n] * divmag
        else:
            varspect[indxn[n]] += 2. * norm[n] * vrtmag
            varspect[indxn[n]] += 2. * norm[n] * divmag
    return varspect


f = Dataset('/Volumes/Drobo/truth_twolevel_t63_12h.nc')
lats = f.variables['lat'][:]
lons = f.variables['lon'][:]
u = f.variables['u']
v = f.variables['v']
ntimes, nlevs, nlats, nlons = u.shape
print nlons, nlats, f.ntrunc, f.rsphere
sp = Spharmt(nlons, nlats, int(f.ntrunc), f.rsphere, gridtype='gaussian')
kenorm = (-0.25 * sp.invlap).astype(np.float)
kespecmean = None
nout = 0
for ntime in range(ntimes):
    print ntime
    vrtspec, divspec = sp.getvrtdivspec(u[ntime, 1, ...], v[ntime, 1, ...])
    kespec = getvarspectrum(vrtspec, divspec, kenorm, sp.order, sp.degree,
                            sp.ntrunc)
    if kespecmean is None:
        kespecmean = kespec
    else:
        kespecmean += kespec
    nout += 1
kespecmean = kespecmean / nout
plt.loglog(np.arange(f.ntrunc+1),kespec,linewidth=2,\