For an incompressible and isothermal polymer fluid, Beris and Edwards have derived the following relation for the Equation of evolution of the conformation tensor and the stress tensor [22, 30]:
Where [LAMBDA] is a fourth-order tensor, called the mobility tensor which is essentially the inverse of the relaxation time of the polymer fluids, [rho] is the fluid density, Q is anisotropic viscosity matrix that is related to viscous dissipation, L is coupling parameter between the velocity gradient field and the structural tensor field, C is second-order conformation tensor which is symmetric, and it has nine components as follow:
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where L denotes the Lie derivative, S is the Ricci
tensor and [lambda] is real constant on ik.
The next step is to calculate the alignmen
tensor using Eq.
In this section, we first introduce
tensor operations used in this paper and provide the bistatic MIMO radar signal model.
One then interprets Poisson's equation in metric language as -[[nabla].sup.2][g.sub.00] = [kappa][T.sub.00], where matter energy density is interpreted as the time-time component of the divergence free, symmetric, matter energy momentum
tensor [T.sub.ab].
To solve (1), we need to calculate an exponential function about
tensor A.
Therefore, this paper firstly uses the data completion method based on the
tensor form to complete the missing RTMS data.
defined the primitivity of nonnegative
tensors (as Definition 1), extended the theory of nonnegative matrices to nonnegative
tensors, and proved the convergence of the NQZ method which is an extension of the Collatz method and can be used to find the largest eigenvalue of any nonnegative irreducible
tensor.
Here [A.sub.PN] is an amplitude of P-wave displacement measured on north component; [G.sub.PN] (1) is the P-wave Green's function's derivative for a far-field ray approximation of north component amplitude due to the first component of moment
tensor M ; numbers (1)...