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Exact(5)
The solution of this equation is described in the Appendix.
This equation is described in detail by Nakagawa et al. [12].
The global behavior of this equation is described in Section 8 and, in this case, every solution goes to infinity.
A novel accurate and rapid numerical procedure for the solution of this equation is described in this paper.
The derivation of this equation is described in the Supporting Information.
Similar(55)
This behavior in the equation is described as stiffness.
In this case, the adjoint equation is described by dY_{t}^{v}=Z_{t}^{v},dW_{t},quad 0 leq tleq T quad quad Y_{T}^{v}=X_{T}^{v};quad quad Y_{t}^{v}=Z_{t}^{v}=0, quad T< tleq T+ delta.
Similarly, the uniaxial compressive damage equation is described in Eqs.
Analytical exProcedure for thexactstants integrationl equatiof are provided theuse for any lay-up sequence.
First, the system dynamic and kinematic equations are given, the kinematic equation is described by the (w, z) parametrization.
In Section 2, a high-accuracy linear-compact difference scheme for the GRLW equation is described.
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