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partial differential equations


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1: 32.13 Reductions of Partial Differential Equations
§32.13 Reductions of Partial Differential Equations
2: Howard S. Cohl
Cohl has published papers in orthogonal polynomials and special functions, and is particularly interested in fundamental solutions of linear partial differential equations on Riemannian manifolds, associated Legendre functions, generalized and basic hypergeometric functions, eigenfunction expansions of fundamental solutions in separable coordinate systems for linear partial differential equations, orthogonal polynomial generating function and generalized expansions, and q -series. …
3: Peter A. Clarkson
 Kruskal, he developed the “direct method” for determining symmetry solutions of partial differential equations in New similarity reductions of the Boussinesq equation (with M. …
4: Ronald F. Boisvert
His research interests include numerical solution of partial differential equations, mathematical software, and information services that support computational science. …
5: Bonita V. Saunders
Her research interests include numerical grid generation, numerical solution of partial differential equations, and visualization of special functions. …
6: 36.15 Methods of Computation
For numerical solution of partial differential equations satisfied by the canonical integrals see Connor et al. (1983).
7: 16.14 Partial Differential Equations
§16.14 Partial Differential Equations
§16.14(i) Appell Functions
In addition to the four Appell functions there are 24 other sums of double series that cannot be expressed as a product of two F 1 2 functions, and which satisfy pairs of linear partial differential equations of the second order. …
8: 23.21 Physical Applications
§23.21(ii) Nonlinear Evolution Equations
Airault et al. (1977) applies the function to an integrable classical many-body problem, and relates the solutions to nonlinear partial differential equations. …
9: 35.7 Gaussian Hypergeometric Function of Matrix Argument
§35.7(iii) Partial Differential Equations
Subject to the conditions (a)–(c), the function f ( T ) = F 1 2 ( a , b ; c ; T ) is the unique solution of each partial differential equationSystems of partial differential equations for the F 1 0 (defined in §35.8) and F 1 1 functions of matrix argument can be obtained by applying (35.8.9) and (35.8.10) to (35.7.9). …
10: 18.39 Physical Applications
§18.39(i) Quantum Mechanics