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The solution is first given as a convolution of the Green function of the plate.
In the following, we present the Green function of the fractional differential equation boundary value problem.
where g α r is the Green function of the isolated lead-α.
The Green function of the differential operator (A^{x}) is constructed.
The Green function of the BVP (5.4) has the form (56). Clearly, is continuous and increasing.
Let and denote by the Green function of the problem (3.1).
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In Section 3, we will use the Poincaré matrixes and fundamental matrix solutions to give the formula of the Green functions of the periodic solution problem (1.2).
The behaviour of the global structure is predicted from the Green functions of the individual uncoupled beams, evaluated as summations over their mode shapes.
The current method also provides a perturbation series expansion and the Green functions of the wave equation in the N-dimension, all by quadratures along a single trajectory.
We show that, under some quite natural conditions, the Green functions of the Girsanov transformed process are comparable to those of the original process.
Also the Green functions of the problem are derived and their use is pointed out for tackling the problem with additional source terms or/and boundary conditions.
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