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sfcij2moveout (4.0)		index
user/zone/Mcij2moveout.c
\n Converting interval Cij to interval/effective moveout coefficients in 3D layered orthorhombic with possible phimuthal rotation (Sripanich and Fomel, 2016) \n

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\n Synopsis
       sfcij2moveout > a11o.rsf a12o=a12o.rsf a22o=a22o.rsf a1111o=a1111o.rsf a1112o=a1112o.rsf a1122o=a1122o.rsf a1222o=a1222o.rsf a2222o=a2222o.rsf < C11.rsf c55=C55.rsf c33=C33.rsf c66=C66.rsf c12=C12.rsf c13=C13.rsf c23=C23.rsf c22=C22.rsf c44=C44.rsf phi=Phi.rsf scalecij=1 scalequartic=n eff=n
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\n Parameters
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file a1111o= 		\tauxiliary output file name
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file a1112o= 		\tauxiliary output file name
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file a1122o= 		\tauxiliary output file name
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file a1222o= 		\tauxiliary output file name
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file a12o= 		\tauxiliary output file name
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file a2222o= 		\tauxiliary output file name
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file a22o= 		\tauxiliary output file name
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file c12= 		\tauxiliary input file name
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file c13= 		\tauxiliary input file name
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file c22= 		\tauxiliary input file name
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file c23= 		\tauxiliary input file name
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file c33= 		\tauxiliary input file name
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file c44= 		\tauxiliary input file name
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file c55= 		\tauxiliary input file name
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file c66= 		\tauxiliary input file name
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bool eff=n [y/n]		\tOutput effective parameters instead of interval
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file phi= 		\tauxiliary input file name
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float scalecij=1 		\tScaling of input Cij in case of GPa or km^2/s^2
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bool scalequartic=n [y/n]		\tScaling the output quartic coefficients y--multiplied by 2 t0^2 (t0 = two-way) to look at the property of the layer -> input for GMA
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