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if (lim_{deltarightarrow0}frac{mu}{sigma }=0), the boundary condition would be u x,t cdotnu=0 quad textit{on } partialOmega_{1}; (8) 3(ii).
(14) . if (lim_{deltarightarrow0}frac{sigma}{mu }=0), the optimal boundary condition would be u x,t cdottau=0 quad textit{on } partialOmega_{1}; (13).
if (lim_{deltarightarrow0}frac{mu}{sigma }=bethen(0,1]), the boundary condition would be u x,t)=0 quad textit{on } partialOmega_{1}.
(9) . if (lim_{deltarightarrow0}frac{mu}{sigma }=0), the boundary condition would be u x,t cdotnu=0 quad textit{on } partialOmega_{1}; (8).
if (lim_{deltarightarrow0}frac{sigma}{mu }=bethen(0,1]), the optimal boundary condition would be u x,t)=0 quad textit{on } partialOmega_{1}.
if (lim_{deltarightarrow0}frac{sigma}{mu }=0), the optimal boundary condition would be u x,t cdottau=0 quad textit{on } partialOmega_{1}; (13) 3 ii).
Similar(44)
In this case the only essential condition would be the same initial water saturation, pore structure, and boundary condition between the original and reference porous systems.
It is found that the boundary conditions would affect the modal radiation efficiencies very much in the subsonic region.
The unusual boundary conditions would ideally require new hardware.
With periodic boundary conditions, which are commonly used to mimic an infinite domain, we expected that the boundary effects would be negligible as regards the pattern characteristics.
But boundary changes would be different.
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