文件名称:Q--Anisotropic-Q-
- 所属分类:
- 能源行业(电力石油煤炭)
- 资源属性:
- [Matlab] [源码]
- 上传时间:
- 2018-08-27
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- 30kb
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- 张**
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各向异性q模拟, 适应于地震资料处理反演实验(U-58 Ani Q- Anisotropic Q modeling Yaping Zhu May 2006
Confidential to the Consortium until 1 Aug 2009
Contents of this directory are Matlab packages to perform the following
tasks.
HomoPlaneAttVTI, Yaping Zhu, complex wavenumber for "homogeneous" plane
P-SV wave propagation in VTI media with VTI attenuation
Note: "Homogeneous" here means that the real and imaginary parts
of the wavevector are parallel to each other.
HomoPlaneAttORT, Yaping Zhu, complex wavenumber for "homogeneous" plane
P-wave propagation in orthorhombic (ORT) media with ORT attenuation
Note: "Homogeneous" here means that the real and imaginary parts
of the wavevector are parallel to each other.
RotCij, Yaping Zhu, Bond transformation of the Cij matrix (6x6)
EffQTI, Yaping Zhu, Effective attenuation- and velocity-anisotropy parameters
for finely-layered VTI media composed of arbitrary number of
constituents
)
Confidential to the Consortium until 1 Aug 2009
Contents of this directory are Matlab packages to perform the following
tasks.
HomoPlaneAttVTI, Yaping Zhu, complex wavenumber for "homogeneous" plane
P-SV wave propagation in VTI media with VTI attenuation
Note: "Homogeneous" here means that the real and imaginary parts
of the wavevector are parallel to each other.
HomoPlaneAttORT, Yaping Zhu, complex wavenumber for "homogeneous" plane
P-wave propagation in orthorhombic (ORT) media with ORT attenuation
Note: "Homogeneous" here means that the real and imaginary parts
of the wavevector are parallel to each other.
RotCij, Yaping Zhu, Bond transformation of the Cij matrix (6x6)
EffQTI, Yaping Zhu, Effective attenuation- and velocity-anisotropy parameters
for finely-layered VTI media composed of arbitrary number of
constituents
)
(系统自动生成,下载前可以参看下载内容)
下载文件列表
AttTI2dfSH
AttTI2dfSH\AttTI2dfSH.m
AttTI2dfSH\GetSourceWaveform.m
AttTI2dfSH\README
AttTI2dfSH\untitled3.m
EffQ
EffQ\attVTIpara2cij.m
EffQ\CalcEffParaVTI.m
EffQ\EffQTI.m
EffQ\README
EffQ\VTIcij2para.m
EffQ\VTIpara2cij.m
HomoPlaneAttORT
HomoPlaneAttORT\AttnuAniso2Qij_ORT.m
HomoPlaneAttORT\CheckElapsedTime.m
HomoPlaneAttORT\HomoPlanePAttORT.m
HomoPlaneAttORT\README
HomoPlaneAttORT\SolveChrisORT.m
HomoPlaneAttORT\VeloAniso2cij_ORT.m
HomoPlaneAttVTI
HomoPlaneAttVTI\attVTIcij2para.m
HomoPlaneAttVTI\attVTIpara2cij.m
HomoPlaneAttVTI\CheckElapsedTime.m
HomoPlaneAttVTI\HomoPlaneAttVTI.m
HomoPlaneAttVTI\PSVkkI.m
HomoPlaneAttVTI\README
README
RotCij
RotCij\BondRot66.m
RotCij\README
RotCij\testBondRot66.m
RotCij\VeloAniso2cij_ORT.m
RotCij\VoigtNotation.m
AttTI2dfSH\AttTI2dfSH.m
AttTI2dfSH\GetSourceWaveform.m
AttTI2dfSH\README
AttTI2dfSH\untitled3.m
EffQ
EffQ\attVTIpara2cij.m
EffQ\CalcEffParaVTI.m
EffQ\EffQTI.m
EffQ\README
EffQ\VTIcij2para.m
EffQ\VTIpara2cij.m
HomoPlaneAttORT
HomoPlaneAttORT\AttnuAniso2Qij_ORT.m
HomoPlaneAttORT\CheckElapsedTime.m
HomoPlaneAttORT\HomoPlanePAttORT.m
HomoPlaneAttORT\README
HomoPlaneAttORT\SolveChrisORT.m
HomoPlaneAttORT\VeloAniso2cij_ORT.m
HomoPlaneAttVTI
HomoPlaneAttVTI\attVTIcij2para.m
HomoPlaneAttVTI\attVTIpara2cij.m
HomoPlaneAttVTI\CheckElapsedTime.m
HomoPlaneAttVTI\HomoPlaneAttVTI.m
HomoPlaneAttVTI\PSVkkI.m
HomoPlaneAttVTI\README
README
RotCij
RotCij\BondRot66.m
RotCij\README
RotCij\testBondRot66.m
RotCij\VeloAniso2cij_ORT.m
RotCij\VoigtNotation.m