12 Energy Methods, Weak Solutions and the Dirichlet Principle
The explicit formulas of the previous sections need special geometry: lines, half-spaces, balls, rectangles. For a general region, and for variable coefficients, existence must be proved by other means, and the most powerful are variational. A steady state minimises energy; so look for the minimiser of the energy, and show that it solves the equation. This is the Dirichlet principle. Riemann used it freely in complex analysis; Weierstrass showed in 1870 that the minimum need not exist; and Hilbert rescued it in 1900. The rescue required a new notion of solution, the weak solution, and new function spaces, and it led directly to the finite element method used in engineering today.
12.2 The Poincaré inequality
12.3 Weak solutions
12.4 Galerkin’s method and finite elements
12.5 Rayleigh quotients and energy decay
12.6 Variational methods in software
12.7 Practice Problems
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