def get_demodulated_data_from_list(filelist,freq=10,supply_index=True,phase_offset=0): filelist.sort() #just in case dd=[] for f in filelist: #only use full size files stats=os.stat(f) if stats.st_size == 10752000: print f d=demod.demodulate_dat(f,freq,supply_index=True,phase_offset=phase_offset) #filename is start of data taking (I think) and we'll just add 1/samprate seconds per rev h=np.float64(f[-12:-10]) m=np.float64(f[-10:-8]) s=np.float64(f[-8:-6]) t=h+m/60.+(s+(d['rev']-d['rev'][0])/samprate)/3600. d=recf.append_fields(d,'localtime',t) ut=np.mod(t+7.,24.) if len(f)>21: y=np.zeros(len(d),dtype=np.int)+np.int(f[-21:-17]) mo=np.zeros(len(d),dtype=np.int)+np.int(f[-17:-15]) dy=np.zeros(len(d),dtype=np.int)+np.int(f[-15:-13]) ut=np.mod(t+7.,24.) utt=t+7. dy[utt>ut]=dy[utt>ut]+1 d=recf.append_fields(d,['year','month','day'],[y,mo,dy]) d=recf.append_fields(d,'ut',ut) dd.append(d) return np.concatenate(dd)
zsky1[1][zsky1[0] == 50]) + np.sqrt(zsky3[1][zsky3[0] == 50])) epsilons[ch] = epsilon[0] for ch in ['ch1', 'ch3', 'ch5']: calsecco[ch] = (tamb - tsky) / (np.mean(cal[ch].flatten()[secco]) / np.mean(cal[ch].flatten()[ssky2])) calsecco['ch0'] = calsecco['ch1'] / bbgain['ch0'] calsecco['ch2'] = calsecco['ch3'] / bbgain['ch2'] calsecco['ch4'] = calsecco['ch5'] / bbgain['ch4'] #now get the other sky data get_ipython().magic(u"cd 'c:/cofe/cofe_ground_fall_2012/data/20121113'") fl = glob('*.dat') dsky = [] for f in fl: dsky.append(demod.demodulate_dat(f, 10)) dsky = np.concatenate(dsky) for ch in chans: zsky1t = cu.nps(dsky[ch]['T'][:5200], rotrate, minfreq=.1) zsky1q = cu.nps(dsky[ch]['Q'][:5200], rotrate, minfreq=.1) zsky1u = cu.nps(dsky[ch]['U'][:5200], rotrate, minfreq=.1) plt.figure(figsize=(12, 6)) hold(True) plt.plot(zsky1t[0], np.sqrt(zsky1t[1]) * calsecco[ch] * 1000., label='T') plt.plot(zsky1q[0], np.sqrt(zsky1q[1]) * calsecco[ch] * 1000., label='Q') plt.plot(zsky1u[0], np.sqrt(zsky1u[1]) * calsecco[ch] * 1000., label='U') plt.title( 'Sky test Nov 13, 2012 (Rough cal to 300K). 10 GHz COFE detector ' +
zecco=cu.nps(cal[ch].flatten()[secco],samprate,minfreq=1) epsilon=np.sqrt((zfoam1[1][zfoam1[0]==50] + zfoam2[1][zfoam2[0]==50]))/(np.sqrt(zsky1[1][zsky1[0]==50]) + np.sqrt(zsky3[1][zsky3[0]==50])) epsilons[ch]=epsilon[0] for ch in ['ch1','ch3','ch5']: calsecco[ch]=(tamb-tsky)/(np.mean(cal[ch].flatten()[secco])/np.mean(cal[ch].flatten()[ssky2])) calsecco['ch0']=calsecco['ch1']/bbgain['ch0'] calsecco['ch2']=calsecco['ch3']/bbgain['ch2'] calsecco['ch4']=calsecco['ch5']/bbgain['ch4'] #now get the other sky data get_ipython().magic(u"cd 'c:/cofe/cofe_ground_fall_2012/data/20121113'") fl=glob('*.dat') dsky=[] for f in fl: dsky.append(demod.demodulate_dat(f,10)) dsky=np.concatenate(dsky) for ch in chans: zsky1t=cu.nps(dsky[ch]['T'][:5200],rotrate,minfreq=.1) zsky1q=cu.nps(dsky[ch]['Q'][:5200],rotrate,minfreq=.1) zsky1u=cu.nps(dsky[ch]['U'][:5200],rotrate,minfreq=.1) plt.figure(figsize=(12,6)) hold(True) plt.plot(zsky1t[0],np.sqrt(zsky1t[1])*calsecco[ch]*1000.,label='T') plt.plot(zsky1q[0],np.sqrt(zsky1q[1])*calsecco[ch]*1000.,label='Q') plt.plot(zsky1u[0],np.sqrt(zsky1u[1])*calsecco[ch]*1000.,label='U') plt.title('Sky test Nov 13, 2012 (Rough cal to 300K). 10 GHz COFE detector '+ch) plt.xlabel('Frequency, Hz')