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Constant coefficient differential equations.
Recently in, DGLM was developed for the constant coefficient advection-diffusion problem.
They, in fact, represent systems that are describable by linear constant coefficient differential equations.
Whereas the constant coefficient of the general characteristic polynomial is the resultant of the system.
But these properties, in particular, provide the mechanism as they did with Fourier transforms for turning linear constant coefficient differential equations into algebraic equations and, corresponding, lead to a mechanism for dealing with and solving linear constant coefficient differential equations.
We'll be using a number of these properties shortly, when we turn our attention to linear constant coefficient differential equations.
In particular, let's think of a discrete-time system that is described by a linear constant coefficient difference equation.
In the ECC presentation, we mainly discuss distributed dissipative systems described by constant coefficient linear PDE's.
Similar(3)
Inverse problem for a wave equation with a piecewise-constant coefficient was solved by Lavrent'ev [13].
In Le Rousseau's paper, the author constructed a limit weight function as he approached BV coefficient by piecewise-constant coefficient.
Dynamic as well as constant-coefficient-based subgrid-scale modeling is used within the multiscale environment.
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