示例#1
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文件: saf.py 项目: 1014511134/src
def imixt(ss,wav,rr,n,par):
    pari = iparam(par)
    
    # model and geometry
    common('wav','vsm','den',ss,rr,'qq',par)
    random('gg',par)

    randomvel('vsm','vrn','gg',0.30,ss,rr,'qq',par)

    # FDmodeling
    modeling('wav',
             'vrn','den',
             ss,rr,'qq',
             'dat','wfl',par)
    
    Flow('rev',
         'dat',
         'reverse which=2 opt=i verb=y | pad end2=%(tpad)d' % pari)
    
    i = n-1
    j = int(pow(2,i))
    l = "%01d" %i
    
    Flow(rr+l,rr,'window j2=%d' %j)
    Plot(rr+l,fdmod.rrplot('plotfat=12',par))
    Result('vsm'+l,['vsm',ss,rr+l,'qq'],'Overlay')
    
    Flow('rev'+l,'rev','window j1=%d' %j)
    
    # FDmigration      
    migration('rev'+l,
              'vsm','den',
              rr+l,rr,'qq',
              'uuu'+l,'wig'+l,
              'cic'+l,'iic'+l,pari)
示例#2
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def imixt(ss, wav, rr, n, par):
    pari = iparam(par)

    # model and geometry
    common('wav', 'vsm', 'den', ss, rr, 'qq', par)
    random('gg', par)

    randomvel('vsm', 'vrn', 'gg', 0.30, ss, rr, 'qq', par)

    # FDmodeling
    modeling('wav', 'vrn', 'den', ss, rr, 'qq', 'dat', 'wfl', par)

    Flow('rev', 'dat',
         'reverse which=2 opt=i verb=y | pad end2=%(tpad)d' % pari)

    i = n - 1
    j = int(pow(2, i))
    l = "%01d" % i

    Flow(rr + l, rr, 'window j2=%d' % j)
    Plot(rr + l, fdmod.rrplot('plotfat=12', par))
    Result('vsm' + l, ['vsm', ss, rr + l, 'qq'], 'Overlay')

    Flow('rev' + l, 'rev', 'window j1=%d' % j)

    # FDmigration
    migration('rev' + l, 'vsm', 'den', rr + l, rr, 'qq', 'uuu' + l, 'wig' + l,
              'cic' + l, 'iic' + l, pari)
示例#3
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def isparse(ss, wav, rr, n, par):
    pari = iparam(par)

    # model and geometry
    common('wav', 'vsm', 'den', ss, rr, 'qq', par)

    # ------------------------------------------------------------
    # FDmodeling
    modeling('wav', 'vsm', 'den', ss, rr, 'qq', 'dat', 'wfl', par)

    Flow('rev', 'dat',
         'reverse which=2 opt=i verb=y | pad end2=%(tpad)d' % pari)

    # ------------------------------------------------------------
    for i in range(n):
        j = int(pow(2, i))
        l = "%01d" % i

        Flow(rr + l, rr, 'window j2=%d' % j)
        Plot(rr + l, fdmod.rrplot('plotfat=12', par))
        Result('vsm' + l, ['vsm', ss, rr + l, 'qq'], 'Overlay')

        for f in range(0, par['nt'] / par['jsnap'], 2):
            tag = "-%02d" % f
            Result('wfl' + l + tag, ['wflom-' + tag, ss, rr + l, 'qq'],
                   'Overlay')

        Flow('rev' + l, 'rev', 'window j1=%d' % j)

        # FDmigration
        migration('rev' + l, 'vsm', 'den', rr + l, rr, 'qq', 'uuu' + l,
                  'wig' + l, 'cic' + l, 'iic' + l, pari)
示例#4
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文件: saf.py 项目: 1014511134/src
def geometry(ss,rr,qq,par):
    # source coordinates
    Plot(ss,fdmod.ssplot('',par))
    Plot('win'+ss,ss,winss('',par))
    
    # receiver coordinates
    Plot(rr,fdmod.rrplot('plotfat=12',par))
    
    # image coordinates
    fdmod.makebox(qq,par['zminq'],par['zmaxq'],par['xminq'],par['xmaxq'],par)
    Plot(qq,fdmod.bbplot('plotcol=1',par))
示例#5
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文件: micro.py 项目: psava/cwp12
def windowreceivers(rr,groups,keys,par):

    for group,gpars in groups.items():
        nwin = gpars['nr']
        owin = gpars['or']
        dwin = gpars['dr']
        Flow('rr-'+group,gpars['group'],'window n2=%d f2=%d j2=%d squeeze=n' % (nwin,owin,dwin))
        Plot('rr-'+group,fdmod.rrplot('plotcol=%d plotfat=10' % gpars['color'],par))

    Flow(rr,['rr-'+group for group in keys],
        'cat axis=2 ${SOURCES[1:%d]}' % len(groups))
    Plot(rr,['rr-'+group for group in keys],'Overlay')
示例#6
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def geometry(ss, rr, qq, par):
    # source coordinates
    Plot(ss, fdmod.ssplot('', par))
    Plot('win' + ss, ss, winss('', par))

    # receiver coordinates
    Plot(rr, fdmod.rrplot('plotfat=12', par))

    # image coordinates
    fdmod.makebox(qq, par['zminq'], par['zmaxq'], par['xminq'], par['xmaxq'],
                  par)
    Plot(qq, fdmod.bbplot('plotcol=1', par))
示例#7
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def sampling(vo, rm, dat, rec, ico, cic, iic, par):

    for k in range(0, 3):
        ktag = "-s%01d" % k
        knum = pow(2, k + 1)

        Flow(rec + ktag, rec, 'window j2=%d' % (knum))
        Plot(rec + ktag, 'window |' + fdmod.rrplot('', par))

        Flow(dat + ktag, dat, 'window j1=%d' % (knum))
        Result(
            dat + ktag, 'window j2=5 | transp |' + fdmod.dgrey(
                'pclip=99 screenratio=1.5 min1=%(mintplot)g' % par, par))

        pimage(cic + ktag, iic + ktag, dat + ktag, vo, rm, rec + ktag, ico,
               par)
示例#8
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文件: iic.py 项目: 1014511134/src
def sampling(vo,rm,
             dat,rec,ico,
             cic,iic,
             par):

    for k in range(0,3):
        ktag = "-s%01d" % k
        knum = pow(2,k+1)

        Flow(rec+ktag,rec,'window j2=%d' % (knum))
        Plot(rec+ktag,'window |' + fdmod.rrplot('',par))
        
        Flow(dat+ktag,dat,'window j1=%d' % (knum))
        Result(dat+ktag, 'window j2=5 | transp |' +
               fdmod.dgrey('pclip=99 screenratio=1.5 min1=%(mintplot)g'%par, par))
        
        pimage(cic+ktag,iic+ktag,dat+ktag,vo,rm,rec+ktag,ico,par)
示例#9
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文件: saf.py 项目: 1014511134/src
def isparse(ss,wav,rr,n,par):
    pari = iparam(par)
    
    # model and geometry
    common('wav','vsm','den',ss,rr,'qq',par)

    # ------------------------------------------------------------
    # FDmodeling
    modeling('wav',
             'vsm','den',
             ss,rr,'qq',
             'dat','wfl',par)

    Flow('rev',
         'dat',
         'reverse which=2 opt=i verb=y | pad end2=%(tpad)d' % pari)
    
    # ------------------------------------------------------------
    for i in range(n):
        j = int(pow(2,i))
        l = "%01d" %i

        Flow(rr+l,rr,'window j2=%d' %j)
        Plot(rr+l,fdmod.rrplot('plotfat=12',par))
        Result('vsm'+l,['vsm',ss,rr+l,'qq'],'Overlay')

        for f in range(0,par['nt']/par['jsnap'],2):
            tag = "-%02d"%f
            Result('wfl'+l+tag,['wflom-'+tag,ss,rr+l,'qq'],'Overlay')
       
        Flow('rev'+l,'rev','window j1=%d' %j)

        # FDmigration      
        migration('rev'+l,
                  'vsm','den',
                  rr+l,rr,'qq',
                  'uuu'+l,'wig'+l,
                  'cic'+l,'iic'+l,pari)
示例#10
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def receivers(rr, par):
    fdmod.horizontal(rr, par['oz'] + par['lo'], par)
    Plot(rr, 'window |' + fdmod.rrplot('', par))
示例#11
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def wdfic(cii, uxx, uyy, wxx, wyy, dat, vel, den, rec, ico, par):

    # ------------------------------------------------------------
    par['jrec'] = 5
    par['nrec'] = 320
    par['orec'] = 0
    par['jrec'] = 10
    par['nrec'] = 160

    receivers = range(par['orec'], par['orec'] + par['nrec'] * par['jrec'],
                      par['jrec'])
    # ------------------------------------------------------------

    for k in receivers:
        ktag = "-%04d" % k

        # source coordinates
        Flow(rec + ktag, rec, 'window n2=1 f2=%g' % k)
        Plot(rec + ktag, 'window |' + fdmod.rrplot('', par))

        # velocity (overlay)
        Plot(vel + ktag, [vel, rec + ktag, ico], 'Overlay')
    allvxx = map(lambda x: vel + '-%04d' % x, receivers)
    Plot('allvxx', allvxx, 'Movie')

    # ------------------------------------------------------------
    iwindow = ' ' + \
              '''
              nqz=%(nqz)d oqz=%(oqz)g
              nqx=%(nqx)d oqx=%(oqx)g
              jsnap=%(jdata)d jdata=%(jdata)d
              ''' % par + ' '
    # ------------------------------------------------------------

    # ------------------------------------------------------------
    # image all traces at once

    # wavefield
    # z-x-t
    Flow(
        uyy, dat + '-' + vel + '-wfl', '''
         window n3=%d f3=%g |
         reverse which=4 opt=i verb=y |
         put o3=%g label3=t unit3=s
         ''' % (2 * par['tcut'] + 1, par['nt'] - par['kt'] - par['tcut'],
                -par['tcut'] * par['dt']))
    Result(uyy, 'byte gainpanel=a pclip=100 |' + igrey('', par))

    # WDF over y
    # z-x-t
    Flow(wyy, uyy, 'wdf verb=y nh1=%(nhz)d nh2=%(nhx)d nh3=%(nht)d' % par)
    Result(wyy, 'byte gainpanel=a pclip=100 |' + igrey('', par))
    # ------------------------------------------------------------

    # ------------------------------------------------------------
    # image each trace separately
    for k in receivers:
        ktag = "-%04d" % k

        # data trace
        Flow(dat + ktag, dat, 'window squeeze=n n1=1 f1=%g' % k)
        Flow(dat + ktag + '-rev', dat + ktag,
             'reverse which=2 opt=i verb=y | pad end2=%(tpad)d' % par)

        fdmod.awefd(dat + ktag + '-bck', dat + ktag + '-wfl',
                    dat + ktag + '-rev', vel, den, rec + ktag, rec + ktag,
                    iwindow, par)

        # z-x-t
        Flow(
            uyy + ktag, dat + ktag + '-wfl', '''
             window n3=%d f3=%g |
             reverse which=4 opt=i verb=y |
             put o3=%g label3=t unit3=s
             ''' % (2 * par['tcut'] + 1, par['nt'] - par['kt'] - par['tcut'],
                    -par['tcut'] * par['dt']))
        Result(uyy + ktag, 'byte gainpanel=a pclip=100 |' + igrey('', par))

        # z*x-.-t
        Flow(uxx + ktag, uyy + ktag,
             'put n1=%d n2=1' % (par['nqz'] * par['nqx']))

    # collect traces at the image point for all receiver locations
    # wavefield
    # z*x-xs-t
    Flow(uxx + '-all', map(lambda x: uxx + '-%04d' % x, receivers),
         'cat axis=2 space=n ${SOURCES[1:%d]}' % (par['nrec']))

    # WDF over x
    # z*x-xs-t
    Flow(wxx + '-all', uxx + '-all', '''
         wdf verb=y nh1=0 nh2=100 nh3=%(nht)d
         ''' % par)

    for k in (uxx, wxx):

        # all traces around the target
        # z-x-t
        Flow(
            k + '-cub', k + '-all', '''
             stack |
             transp plane=23 |
             put
             n1=%d o1=%g d1=%g label1=z unit1=''
             n2=%d o2=%g d2=%g label2=x unit2=''
             ''' % (par['nqz'], par['oqz'], par['dqz'], par['nqx'], par['oqx'],
                    par['dqx']))

        # one trace at the target
        # xs-t
        Flow(k, k + '-all',
             'window n1=1 f1=%d | transp' % (par['nqz'] * par['nqx'] / 2))

        Result(
            k, '''
               put o2=%g d2=%g | 
               grey title="" pclip=98 labelsz=6 labelfat=2
               label1=%s unit1=%s
               label2=%s unit2=%s
               screenratio=0.3 screenht=4
               %s
               ''' %
            (par['ox'] + par['orec'] * par['dx'], par['jrec'] * par['dx'],
             par['lt'], par['ut'], par['lx'], par['ux'], par['labelattr']))

    # z-x
    Flow(cii, wxx + '-cub', 'window n3=1 f3=%d' % par['tcut'])
    Plot(cii, fdmod.cgrey('pclip=100', par))
    Result(cii, [cii, 'rr'], 'Overlay')
    Result(
        'win' + cii, cii,
        fdmod.cgrey(
            'min1=%g max1=%g min2=%g max2=%g screenratio=%g wantaxis=y' %
            (par['wzmin'], par['wzmax'], par['wxmin'], par['wxmax'],
             par['wratio']), par))
示例#12
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def run(par):
    # experiments
    fdmod.horizontal('rr', 0, par)

    Plot('rr', 'window j2=10|' + fdmod.rrplot('', par))
    Plot('ss', 'window      |' + fdmod.ssplot('', par))
    Plot('sx', 'window      |' + fdmod.ssplot('plotcol=5', par))

    # wavelet
    fdmod.wavelet('wav_', par['frq'], par)
    Flow('wav', 'wav_', 'transp')
    Result('wav', 'window n2=200 |' + fdmod.waveplot('', par))

    # velocity
    Flow(
        'vbck', None, '''
         math n1=%(nz)d o1=%(oz)g d1=%(dz)g output="2000" |
         spray axis=2 n=%(nx)d o=%(ox)g d=%(dx)g
         ''' % par)
    Flow(
        'vprt', None, '''
         spike nsp=1 mag=1
         n1=%(nz)d o1=%(oz)g d1=%(dz)g k1=%(kz)d l1=%(mz)d
         n2=%(nx)d o2=%(ox)g d2=%(dx)g k2=%(kx)d l2=%(mx)d |
         smooth rect1=25 rect2=25 repeat=3 |
         scale axis=123 |
         scale rscale=%(vprt)g
         ''' % par)
    Flow('velo', 'vbck vprt', 'add ${SOURCES[1]}')
    Plot('velo', fdmod.cgrey('allpos=y bias=1200 pclip=100 color=g', par))
    Result('velo', ['velo', 'ss', 'sx'], 'Overlay')

    # density
    Flow('dens', 'velo', 'math output=1')

    # reflector
    Plot(
        'refl', 'refl velo', '''
         depth2time velocity=${SOURCES[1]} dt=%(dt)g nt=%(nt)d |
         scale rscale=-1 |
         ricker1 frequency=%(frq)g |
         time2depth velocity=${SOURCES[1]} dz=%(dz)g nz=%(nz)d |
         ''' % par + fdmod.cgrey('pclip=100', par))
    Result('refl', ['refl', 'ss', 'sx'], 'Overlay')

    # mask
    Flow(
        'mask', None, '''
         spike nsp=1 mag=1
         n1=%(nx)d o1=%(ox)g d1=%(dx)g k1=101 l1=900
         n2=%(nt)d o2=%(ot)g d2=%(dt)g |
         smooth rect1=100 |
         scale axis=123
         ''' % par)
    Result('mask', 'transp |' + fdmod.dgrey('allpos=y pclip=100', par))

    # F-D modeling (born)
    fdmod.lwefd1('do', 'wo', 'dd', 'wd', 'wav', 'velo', 'dens', 'refl', 'ss',
                 'rr', 'jsnap=100', par)
    Result(
        'do', 'transp | window min1=0.25 |' +
        fdmod.dgrey('min1=0.25 pclip=100', par))
    Result(
        'dd', 'transp | window min1=0.25 |' +
        fdmod.dgrey('min1=0.25 pclip=100', par))
    Result('wo', fdmod.wgrey('', par))
    Result('wd', fdmod.wgrey('', par))

    # source data and wavefield
    fdmod.awefd1('ds', 'ws', 'wav', 'velo', 'dens', 'sx', 'rr', '', par)
    Result('ws', 'window j3=20 |' + fdmod.wgrey('', par))

    # receiver wavefield
    Flow('du', 'dd mask',
         'add mode=p ${SOURCES[1]} | reverse which=2 opt=i verb=y')
    fdmod.awefd('dx', 'wx', 'du', 'velo', 'dens', 'rr', 'rr', '', par)
    Flow('dr', 'dx', 'reverse which=2 opt=i verb=y')
    Flow('wr', 'wx', 'reverse which=4 opt=i verb=y')
    Result('wr', 'window j3=20 |' + fdmod.wgrey('', par))

    for i in range(0, par['nt'] / 100, 1):
        fdmod.wframe('wo' + '-' + str(i), 'wo', i, 'pclip=99.9', par)
        fdmod.wframe('wd' + '-' + str(i), 'wd', i, 'pclip=100', par)

    for i in range(0, par['nt'] / 100, 1):
        fdmod.wframe('wx' + '-' + str(i), 'wx', i * 25, 'pclip=99.9', par)

    # ------------------------------------------------------------
    minx = 500
    maxx = 1500
    minz = par['oz'] + par['nz'] * par['dz'] / 2
    numz = par['nz'] / 2

    mint = 0.1
    numt = 150
    maxt = mint + numt * par['dt'] * par['jsnap']

    # wavefield
    for i in ('s', 'r'):
        Flow(
            'u' + i, 'w' + i, '''
             window min1=%(zmin)g max1=%(zmax)g min2=%(xmin)g max2=%(xmax)g |
             scale axis=123
             ''' % par)
        Plot('u' + i, 'window j3=10 |' + fdmod.wgrey('pclip=99', par), view=1)

        for k in range(0, par['nt'] / par['jsnap'], 25):
            fdmod.wframe('u' + i + '-' + str(k / 25), 'u' + i, k, 'pclip=99',
                         par)

        # windowed wavefields
        Flow(
            'p' + i, 'u' + i, '''
             window min1=%g n1=%g min2=%g max2=%g min3=%g n3=%g
             ''' % (minz, numz, minx, maxx, mint, numt))
        Flow('q' + i, 'p' + i, 'transp plane=13 memsize=500')
        Flow('o' + i, 'q' + i, 'transp plane=23 memsize=500')

    Flow('qi', 'qs qr', 'add mode=p ${SOURCES[1]}')
    Flow('oi', 'os or', 'add mode=p ${SOURCES[1]}')

    for i in ('s', 'r', 'i'):
        Plot('q' + i,
             'window j3=10 |' + fdmod.dgrey('gainpanel=a pclip=100', par),
             view=1)
        Plot('o' + i,
             'window j3=10 | transp |' +
             fdmod.egrey('gainpanel=a pclip=100', par),
             view=1)

        Flow(['q' + i + 'plt', 'q' + i + 'bar'], 'q' + i,
             'byte bar=${TARGETS[1]} gainpanel=a pclip=100')
        for k in range(10):
            Result(
                'q' + i + 'plt' + str(k), ['q' + i + 'plt', 'q' + i + 'bar'],
                'window n3=1 f3=%d |' % (10 * k) + fdmod.dgrey(
                    '''
                bar=${SOURCES[1]} min1=%g max1=%g min2=%g max2=%g
                labelsz=8 labelfat=3 screenratio=1.5
                ''' % (mint, maxt, minx, maxx), par))

    # cut along the reflectors
    Flow(
        'cut', 'refl', '''
         window min1=%g n1=%g min2=%g max2=%g |
         spray axis=3 n=%d o=%g d=%g |
         transp plane=13 memsize=500
         ''' % (minz, numz, minx, maxx, numt, 0.1, par['dt'] * 4))

    for i in ('s', 'r'):
        Flow(
            'c' + i, ['q' + i, 'cut'], '''
             add mode=p ${SOURCES[1]} |
             transp plane=23 |
             stack
             ''')
        Result('c' + i, fdmod.dgrey('', par))

        Flow('f' + i, 'q' + i, 'window n3=1 min3=300')
        Result('f' + i, fdmod.dgrey('', par))

    # ------------------------------------------------------------
    # conventional IC
    Flow('ii', ['ps', 'pr'], 'ic ur=${SOURCES[1]} version=0 nbuf=500 verb=y')
    Plot('ii', fdmod.cgrey('pclip=99.9', par))
    Result('ii', ['ii', 'ss', 'sx'], 'Overlay')
示例#13
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 def rrplot(self,custom,scalar,horizontal=True):
   self.scale(horizontal)
   return fdmod.rrplot(custom,self.par)
示例#14
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文件: itest.py 项目: 1014511134/src
def run(par):
    # experiments
    fdmod.horizontal('rr',0,par)

    Plot('rr','window j2=10|' + fdmod.rrplot('',par))
    Plot('ss','window      |' + fdmod.ssplot('',par))
    Plot('sx','window      |' + fdmod.ssplot('plotcol=5',par))
    
    # wavelet
    fdmod.wavelet('wav_',par['frq'],par)
    Flow('wav','wav_','transp')
    Result('wav','window n2=200 |' + fdmod.waveplot('',par))
    
    # velocity
    Flow('vbck',None,
         '''
         math n1=%(nz)d o1=%(oz)g d1=%(dz)g output="2000" |
         spray axis=2 n=%(nx)d o=%(ox)g d=%(dx)g
         ''' % par)
    Flow('vprt',None,
         '''
         spike nsp=1 mag=1
         n1=%(nz)d o1=%(oz)g d1=%(dz)g k1=%(kz)d l1=%(mz)d
         n2=%(nx)d o2=%(ox)g d2=%(dx)g k2=%(kx)d l2=%(mx)d |
         smooth rect1=25 rect2=25 repeat=3 |
         scale axis=123 |
         scale rscale=%(vprt)g
         ''' % par)
    Flow(  'velo','vbck vprt','add ${SOURCES[1]}')
    Plot(  'velo',fdmod.cgrey('allpos=y bias=1200 pclip=100 color=g',par))
    Result('velo',['velo','ss','sx'],'Overlay')
    
    # density
    Flow('dens','velo','math output=1')
    
    # reflector
    Plot('refl','refl velo',
         '''
         depth2time velocity=${SOURCES[1]} dt=%(dt)g nt=%(nt)d |
         scale rscale=-1 |
         ricker1 frequency=%(frq)g |
         time2depth velocity=${SOURCES[1]} dz=%(dz)g nz=%(nz)d |
         ''' % par + fdmod.cgrey('pclip=100',par))
    Result('refl',['refl','ss','sx'],'Overlay')

    # mask
    Flow('mask',None,
         '''
         spike nsp=1 mag=1
         n1=%(nx)d o1=%(ox)g d1=%(dx)g k1=101 l1=900
         n2=%(nt)d o2=%(ot)g d2=%(dt)g |
         smooth rect1=100 |
         scale axis=123
         ''' % par)
    Result('mask','transp |' + fdmod.dgrey('allpos=y pclip=100',par))
        
    # F-D modeling (born)
    fdmod.lwefd1(
        'do','wo',
        'dd','wd',
        'wav','velo','dens','refl','ss','rr','jsnap=100',par)
    Result('do','transp | window min1=0.25 |' + fdmod.dgrey('min1=0.25 pclip=100',par))
    Result('dd','transp | window min1=0.25 |' + fdmod.dgrey('min1=0.25 pclip=100',par))
    Plot('wo',fdmod.wgrey('',par),view=1)
    Plot('wd',fdmod.wgrey('',par),view=1)

    # source data and wavefield
    fdmod.awefd1(
        'ds','ws',
        'wav','velo','dens','sx','rr','',par)
    Plot('ws','window j3=20 |' + fdmod.wgrey('',par),view=1)

    # receiver wavefield
    Flow('du','dd mask',
         'add mode=p ${SOURCES[1]} | reverse which=2 opt=i verb=y')
    fdmod.awefd(
        'dx','wx',
        'du','velo','dens','rr','rr','',par)
    Flow('dr','dx','reverse which=2 opt=i verb=y')
    Flow('wr','wx','reverse which=4 opt=i verb=y')
    Plot('wr','window j3=20 |' + fdmod.wgrey('',par),view=1)

    for i in range(0,par['nt']/100,1):
        fdmod.wframe('wo'+'-'+str(i),'wo',i,'pclip=99.9',par)
        fdmod.wframe('wd'+'-'+str(i),'wd',i,'pclip=100',par)

    for i in range(0,par['nt']/100,1):
        fdmod.wframe('wx'+'-'+str(i),'wx',i*25,'pclip=99.9',par)
    
    # ------------------------------------------------------------
    minx=500
    maxx=1500
    minz=par['oz']+par['nz']*par['dz']/2
    numz=par['nz']/2

    mint=0.1
    numt=150
    maxt=mint+numt*par['dt']*par['jsnap']

    # wavefield
    for i in ('s','r'):
        Flow('u'+i,'w'+i,
             '''
             window min1=%(zmin)g max1=%(zmax)g min2=%(xmin)g max2=%(xmax)g |
             scale axis=123
             ''' % par)
        Plot('u'+i,'window j3=10 |' + fdmod.wgrey('pclip=99',par),view=1)

        for k in range(0,par['nt']/par['jsnap'],25):
            fdmod.wframe('u'+i+'-'+str(k/25),'u'+i,k,'pclip=99',par)
        
        # windowed wavefields
        Flow('p'+i,'u'+i,
             '''
             window min1=%g n1=%g min2=%g max2=%g min3=%g n3=%g
             ''' % (minz,numz,
                    minx,maxx,
                    mint,numt))
        Flow('q'+i,'p'+i,'transp plane=13 memsize=500')
        Flow('o'+i,'q'+i,'transp plane=23 memsize=500')
        
    Flow(  'qi','qs qr','add mode=p ${SOURCES[1]}')
    Flow(  'oi','os or','add mode=p ${SOURCES[1]}')
    
    for i in ('s','r','i'):
        Plot('q'+i,'window j3=10 |'
             + fdmod.dgrey('gainpanel=a pclip=100',par),view=1)    
        Plot('o'+i,'window j3=10 | transp |'
             + fdmod.egrey('gainpanel=a pclip=100',par),view=1)
        
        Flow(['q'+i+'plt','q'+i+'bar'],'q'+i,
             'byte bar=${TARGETS[1]} gainpanel=a pclip=100')
        for k in range(10):
            Result('q'+i+'plt'+str(k),['q'+i+'plt','q'+i+'bar'],
                   'window n3=1 f3=%d |' % (10*k) +
                   fdmod.dgrey(
                '''
                bar=${SOURCES[1]} min1=%g max1=%g min2=%g max2=%g
                labelsz=8 labelfat=3 screenratio=1.5
                ''' %(mint,maxt,minx,maxx),par))
        
    # cut along the reflectors
    Flow('cut','refl',
         '''
         window min1=%g n1=%g min2=%g max2=%g |
         spray axis=3 n=%d o=%g d=%g |
         transp plane=13 memsize=500
         ''' % (minz,numz,
                minx,maxx,
                numt,0.1,par['dt']*4) )
    
    for i in ('s','r'):
        Flow('c'+i,['q'+i,'cut'],
             '''
             add mode=p ${SOURCES[1]} |
             transp plane=23 |
             stack
             ''')
        Result('c'+i,fdmod.dgrey('',par))

        Flow(  'f'+i,'q'+i,'window n3=1 min3=300')
        Result('f'+i,fdmod.dgrey('',par))

    # ------------------------------------------------------------
    # conventional IC
    Flow(  'ii',['ps','pr'],'ic ur=${SOURCES[1]} version=0 nbuf=500 verb=y')
    Plot(  'ii',fdmod.cgrey('pclip=99.9',par))
    Result('ii',['ii','ss','sx'],'Overlay')
示例#15
0
文件: iic.py 项目: 1014511134/src
def wdfic(cii,
          uxx,uyy,
          wxx,wyy,
          dat,vel,den,rec,ico,par):
    
    # ------------------------------------------------------------
    par['jrec']=5
    par['nrec']=320
    par['orec']=0
    par['jrec']=10
    par['nrec']=160
    
    receivers = range(par['orec'],par['orec']+par['nrec']*par['jrec'],par['jrec'])
    # ------------------------------------------------------------

    for k in receivers:
        ktag = "-%04d" % k
        
        # source coordinates
        Flow(rec+ktag,rec,'window n2=1 f2=%g' % k )
        Plot(rec+ktag,    'window |' + fdmod.rrplot('',par))
        
        # velocity (overlay)
        Plot(vel+ktag,[vel,rec+ktag,ico],'Overlay')
    allvxx = map(lambda x: vel+'-%04d' % x,receivers)
    Plot('allvxx',allvxx,'Movie')

    # ------------------------------------------------------------ 
    iwindow = ' ' + \
              '''
              nqz=%(nqz)d oqz=%(oqz)g
              nqx=%(nqx)d oqx=%(oqx)g
              jsnap=%(jdata)d jdata=%(jdata)d
              ''' % par + ' '
    # ------------------------------------------------------------

    # ------------------------------------------------------------
    # image all traces at once

    # wavefield
    # z-x-t
    Flow(uyy,
         dat+'-'+vel+'-wfl',
         '''
         window n3=%d f3=%g |
         reverse which=4 opt=i verb=y |
         put o3=%g label3=t unit3=s
         ''' % (2*par['tcut']+1,
                par['nt']-par['kt']-par['tcut'],
                -par['tcut']*par['dt']))
    Result(uyy,'byte gainpanel=a pclip=100 |' + igrey('',par))

    # WDF over y
    # z-x-t
    Flow(wyy,
         uyy,
         'wdf verb=y nh1=%(nhz)d nh2=%(nhx)d nh3=%(nht)d' % par)
    Result(wyy,'byte gainpanel=a pclip=100 |' + igrey('',par))
    # ------------------------------------------------------------

    # ------------------------------------------------------------
    # image each trace separately
    for k in receivers:
        ktag = "-%04d" % k
        
        # data trace
        Flow(dat+ktag,
             dat,'window squeeze=n n1=1 f1=%g' % k )
        Flow(dat+ktag+'-rev',
             dat+ktag,'reverse which=2 opt=i verb=y | pad end2=%(tpad)d' % par)
        
        fdmod.awefd(dat+ktag+'-bck',
                    dat+ktag+'-wfl',
                    dat+ktag+'-rev',
                    vel,den,
                    rec+ktag,rec+ktag,iwindow,par)

        # z-x-t
        Flow(uyy+ktag,
             dat+ktag+'-wfl',
             '''
             window n3=%d f3=%g |
             reverse which=4 opt=i verb=y |
             put o3=%g label3=t unit3=s
             ''' % (2*par['tcut']+1,
                    par['nt']-par['kt']-par['tcut'],
                    -par['tcut']*par['dt']))
        Result(uyy+ktag,'byte gainpanel=a pclip=100 |' + igrey('',par))

        # z*x-.-t
        Flow(uxx+ktag,
             uyy+ktag,
             'put n1=%d n2=1' % (par['nqz']*par['nqx']) )
        
    # collect traces at the image point for all receiver locations
    # wavefield
    # z*x-xs-t
    Flow(uxx+'-all',
         map(lambda x: uxx+'-%04d' % x,receivers),
         'cat axis=2 space=n ${SOURCES[1:%d]}' % (par['nrec']))

    # WDF over x
    # z*x-xs-t
    Flow(wxx+'-all',
         uxx+'-all',
         '''
         wdf verb=y nh1=0 nh2=100 nh3=%(nht)d
         ''' % par)

    for k in (uxx,wxx):

        # all traces around the target
        # z-x-t
        Flow(k+'-cub',
             k+'-all',
             '''
             stack |
             transp plane=23 |
             put
             n1=%d o1=%g d1=%g label1=z unit1=''
             n2=%d o2=%g d2=%g label2=x unit2=''
             ''' % (par['nqz'],par['oqz'],par['dqz'],
                    par['nqx'],par['oqx'],par['dqx']))

        # one trace at the target
        # xs-t
        Flow(k,
             k+'-all',
             'window n1=1 f1=%d | transp' % (par['nqz']*par['nqx']/2) )        
        
        Result(k,
               '''
               put o2=%g d2=%g | 
               grey title="" pclip=98 labelsz=6 labelfat=2
               label1=%s unit1=%s
               label2=%s unit2=%s
               screenratio=0.3 screenht=4
               %s
               ''' % (par['ox']+par['orec']*par['dx'],
                      par['jrec']*par['dx'],
                      par['lt'],par['ut'],
                      par['lx'],par['ux'],
                      par['labelattr']) )

    # z-x
    Flow(cii,
         wxx+'-cub',
         'window n3=1 f3=%d' % par['tcut'])
    Plot(cii,fdmod.cgrey('pclip=100',par))
    Result(cii,[cii,'rr'],'Overlay')        
    Result('win'+cii,
           cii,
           fdmod.cgrey('min1=%g max1=%g min2=%g max2=%g screenratio=%g wantaxis=y' %
                       (par['wzmin'],par['wzmax'],par['wxmin'],par['wxmax'],par['wratio']),par))
示例#16
0
文件: iic.py 项目: 1014511134/src
def receivers(rr,par):    
    fdmod.horizontal(rr,par['oz']+par['lo'],par)
    Plot(rr,'window |' + fdmod.rrplot('',par))