The Ritz method for solving partial differential equations using number-theoretic grids
A. V. Rodionov Β· Π§Π΅Π±ΡΡΠ΅Π²ΡΠΊΠΈΠΉ ΡΠ±ΠΎΡΠ½ΠΈΠΊ Β· 2022
Consider the problem πΏπ’(βπ₯) = π(βπ₯), π’(βπ₯)ββππΊπ = π(βπ₯), where π(βπ₯), π(βπ₯) β πΈπΌ π , πΏ is a linear differential operator with constant coefficients, πΊπ is the unit cube [0; 1]π . Its solution is reduced to finding the minimum of the functional π£(π’(βπ₯)) =β«οΈ. . .πΊπ β«οΈ πΉ (βπ₯, π’, π’π₯1 , . . . , π’π₯π ) ππ₯1 ππππ‘π ππ₯π under given boundary conditions. The values of the functional π£(π’(βπ₯)) in the Ritz method are considered not on the set of all admissible functions π’(βπ₯), but on linear combinations π’(βπ₯) = π0(βπ₯) + Ξ£οΈ(π π=1) π€πππ(βπ₯), where ππ(βπ₯) are some basic functions that we will find using number-theoretic interpolation, and π0(βπ₯) is a function that satisfies the given boundary conditions, and the rest ππ(βπ₯) satisfy homogeneous boundary conditions. On these polynomials, this functional turns into a function π( βπ€) of the coefficients π€1, . . . ,π€π. These coefficients are chosen so that the function π( βπ€) reaches an extremum. Under some restrictions on the functional π£(π’(βπ₯)) and the basis functions ππ(βπ₯), we obtain an approximate solution of the boundary value problem.