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normalmodes_rhoz.py
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147 lines (131 loc) · 5.64 KB
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# this is a library for calculating the normal mode decomposition of vertical profiles of
# atmospheric variables.
#depends on numpy
# this supersedes normalmodes.py
import numpy as np
from vstats import *
def get_vertical_modes(N_sq,rhoz,z, zi_full, rigidlid = []):
'''solve the vertical structure equation 1/rho d/dz rhoz d/dz W = -\lambda N_sq W \
and return set of eigenfunctions W_n and eigenvalues \lambda_n'''
if(rigidlid):
lid = rigidlid
else:
lid = zi_full[-1]
index = np.where((zi_full<lid) & (zi_full>0))
zi = zi_full[index]
Nsqgrd= N_sq[index]
#make rhoz on the interfaces
rhoint = scale2int(rhoz,z)[index]
ddzrho_tmp = (rhoz[1:]-rhoz[0:-1])/(z[1:]-z[0:-1])
ddzrho = 1./rhoint*ddzrho_tmp[0:len(index)]
#set up matrix for interface levels
M = np.zeros((len(zi), len(zi)))
for i in range(1,len(zi)-1):
M[i,i] = 2./(zi[i+1]-zi[i-1])*(-1./(zi[i+1]-zi[i]) - 1./(zi[i]-zi[i-1]) )
M[i,i-1] = 2./(zi[i+1]-zi[i-1])*(1./(zi[i]-zi[i-1])) - ddzrho[i]/(zi[i+1]-z[i-1])
M[i,i+1] = 2./(zi[i+1]-zi[i-1])*(1./(zi[i+1]-zi[i])) + ddzrho[i]/(zi[i+1]-z[i-1])
M[i,:] = 1./(Nsqgrd[i])*M[i,:]
#boundary conditions
M[0,0] = 2./(zi[1]-0.)*(-1./(zi[1]-zi[0]) - 1./(zi[0]-0.))
M[0,1] = 2./(zi[1]-0.)*(1./(zi[1]-zi[0])) + ddzrho[0]/(zi[1]-0.)
M[0,:] = 1./(Nsqgrd[0])*M[0,:]
M[-1,-1] = 2./(lid -zi[-2])*(- 1./(lid - zi[-1]) - 1./(zi[-1]-zi[-2]))
M[-1,-2] = 2./(lid -zi[-2])*(1./(zi[-1]-zi[-2])) - ddzrho[-1]/(lid -zi[-2])
M[-1,:] = 1./(Nsqgrd[-1])*M[-1,:]
c_w, Z_w = np.linalg.eig(-M)
X = zip(c_w,Z_w.transpose())
X_sort = sorted(X,key=lambda val: val[0]) # sort by eigenvalue
return (X_sort, zi)
def get_projections(var_profile, EIGVECS, NSQ, ZP):
'''project a given profile(prof), onto eigenvalues(EIGS) found using NSQ on grid ZP.
returns projection'''
w_proj = []
trunc = EIGVECS[0].shape[0]
for i in range(0,trunc):
w_proj.append(project_onto_vertical(var_profile, EIGVECS,NSQ,ZP,i))
return w_proj
def get_projection_coeffs(var_profile, EIGVECS, NSQ, ZP):
'''project a given profile(prof), onto eigenvalues(EIGS) found using NSQ on grid ZP.
returns projection coefficients'''
w_proj_coeffs = []
trunc = EIGVECS[0].shape[0]
for i in range(0,trunc):
w_proj_coeffs.append(projection_coeff(var_profile, EIGVECS,NSQ,ZP,i))
return w_proj_coeffs
def get_phase_speeds(EIGS):
'''calculates phase speeds from eigenvalues contained in list EIGS,
c = 1/np.sqrt(EIGS[i][0])'''
speeds=[]
trunc = EIGS[0][1].shape[0]
for i in range(0,trunc):
speeds.append(1./np.sqrt(EIGS[i][0]))
return speeds
def innerproduct(EIGVECS,NSQ,ZP,val1,val2):
''' calculate the inner product of vertical normal modes val1 and val2 '''
tot = EIGVECS[val1][0]*EIGVECS[val2][0]*NSQ[0]*(ZP[0])
for i in range(1,len(ZP)):
tot = tot + EIGVECS[val1][i]*EIGVECS[val2][i]*NSQ[i]*(ZP[i]-ZP[i-1])
return tot
def normalize(EIGVECS,NSQ, ZP, val1):
''' ****THIS MIGHT BE THE WRONG THING TO DO****
returns the normalized eigenfunction for val1'''
coeff = 1/np.sqrt(innerproduct(EIGVECS,NSQ,ZP, val1, val1))
normalized_eig = coeff * EIGVECS[val1][:]
return normalized_eig
def project_onto_vertical(var_profile, EIGVECS, NSQ, ZP,mode):
'''project an observed profile onto eigenfunction *mode* '''
eigvec=EIGVECS[mode][:]
normed_eig = normalize(EIGVECS,NSQ,ZP, mode)
eigvec = normed_eig
coeff = eigvec[0]*var_profile[0]*NSQ[0]*(ZP[0])
for i in range(1,len(ZP)):
coeff = coeff + eigvec[i]*var_profile[i]*NSQ[i]*(ZP[i]-ZP[i-1])
projection = coeff*eigvec
return projection
def projection_coeff(var_profile, EIGVECS, NSQ, ZP,mode):
'''return the coefficient to
project an observed profile onto eigenfunction *mode* '''
eigvec=EIGVECS[mode][:]
normed_eig = normalize(EIGVECS,NSQ,ZP, mode)
eigvec = normed_eig
coeff = eigvec[0]*var_profile[0]*NSQ[0]*(ZP[0])
for i in range(1,len(ZP)):
coeff = coeff + eigvec[i]*var_profile[i]*NSQ[i]*(ZP[i]-ZP[i-1])
#projection = coeff*eigvec
return coeff
#### utilities #####
def brunt_vaisala(thetav_prof, z):
'''construct N^2 = -g/thetav d/dz(thetav) on the interface levels'''
N_sq_prof = np.zeros(len(z)+1)
ggr = 9.81
thetav_int = scale2int(thetav_prof,z)
for i in range(1,len(z)):
N_sq_prof[i] = ggr/thetav_int[i] * (thetav_prof[i]-thetav_prof[i-1])/(z[i]-z[i-1])
N_sq_prof[len(z)] = N_sq_prof[len(z)-1]
N_sq_prof[0] = N_sq_prof[1]
return N_sq_prof
def make_zi_full(z):
'''makes a vector of grid interfaces vector (including top and bottom) from z on the scalar levels '''
zi_full = np.zeros(len(z)+1)
for i in range(1,len(z)):
zi_full[i] = 0.5*(z[i]+z[i-1])
zi_full[len(z)]= zi_full[len(z)-1] + (z[len(z)-1]-zi_full[len(z)-2])
return zi_full
def plot_projection(projection,ZP,speeds,w_proj_coeffs, n=7):
'''plot the first n components of the projection against grid ZP
and the phase speeds vs the projection coefficient'''
if (n>len(projection)):
n=len(projection)
print 'sorry,n=',n,'exceeds number of eigenfunctions',len(projection)
raise ValueError
fig, (ax1,ax2) = plt.subplots(1,2, figsize=(10,3), sharey=False)
i = 0
for p in projection[0:n]:
ax1.plot(p,ZP, label='mode '+str(i), lw=2)
i+=1
ax2.scatter(speeds[0:trunc],np.abs(w_proj_coeffs), marker = 'o')
ax2.set_xlabel('c (m/s)')
ax1.set_title('vertical mode projection')
ax2.set_title('projection coefficient vs. c')
ax1.legend()
return fig