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11 - Second order PDEs in one dependent and two independent variables

Published online by Cambridge University Press:  05 April 2013

Olle Stormark
Affiliation:
Royal Institute of Technology, Stockholm
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Summary

By Drach's classification an arbitrary PDE system can be reduced to a first or second order system in one unknown, and first order systems in one unknown are completely understood thanks to the theory in chapter 6. So the real difficulties start with second order systems in one unknown.

In this chapter we begin the study of a single PDE in one dependent and two independent variables with some generalities from [Vessiot 1924] and [Vessiot 1936]. Chapters 12-13 are then devoted to hyperbolic PDEs, and chapters 16-17 to parabolic PDEs. Finally, we study PDE systems in one dependent and three independent variables in chapter 18—thus leaving the investigation of PDE systems in one dependent and more than three independent variables in suspense.

Second order PDEs and associated vector field systems

A second order PDE in one dependent and two independent variables is equivalent to a hypersurface in the jet bundle J2(R2,R). The latter has the dimension 8, and is classically endowed with the following coordinates:

independent variables x and y,

dependent variable z,

first order jet coordinates p∂z/∂x and q∂z/∂y,

second order jet coordinates r2z/∂2x, s ↔ 2z/∂x∂y and t ↔ 2z/∂y2.

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Publisher: Cambridge University Press
Print publication year: 2000

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