The Ritz method for solving partial differential equations using number-theoretic grids

A. V. Rodionov Β· Π§Π΅Π±Ρ‹ΡˆΠ΅Π²ΡΠΊΠΈΠΉ сборник Β· 2022

Consider the problem 𝐿𝑒(βƒ—π‘₯) = 𝑓(βƒ—π‘₯), 𝑒(βƒ—π‘₯)βƒ’βƒ’πœ•πΊπ‘ = 𝑔(βƒ—π‘₯), where 𝑓(βƒ—π‘₯), 𝑔(βƒ—π‘₯) ∈ 𝐸𝛼 𝑠 , 𝐿 is a linear differential operator with constant coefficients, 𝐺𝑠 is the unit cube [0; 1]𝑠. Its solution is reduced to finding the minimum of the functional 𝑣(𝑒(βƒ—π‘₯)) =∫︁. . .πΊπ‘ βˆ«οΈ 𝐹 (βƒ—π‘₯, 𝑒, 𝑒π‘₯1 , . . . , 𝑒π‘₯𝑠 ) 𝑑π‘₯1 π‘™π‘‘π‘œπ‘‘π‘ π‘‘π‘₯𝑠 under given boundary conditions. The values of the functional 𝑣(𝑒(βƒ—π‘₯)) in the Ritz method are considered not on the set of all admissible functions 𝑒(βƒ—π‘₯), but on linear combinations 𝑒(βƒ—π‘₯) = π‘Š0(βƒ—π‘₯) + Σ︁(𝑛 π‘˜=1) π‘€π‘˜π‘Šπ‘˜(βƒ—π‘₯), where π‘Šπ‘˜(βƒ—π‘₯) are some basic functions that we will find using number-theoretic interpolation, and π‘Š0(βƒ—π‘₯) is a function that satisfies the given boundary conditions, and the rest π‘Šπ‘˜(βƒ—π‘₯) satisfy homogeneous boundary conditions. On these polynomials, this functional turns into a function πœ™( ⃗𝑀) of the coefficients 𝑀1, . . . ,𝑀𝑛. These coefficients are chosen so that the function πœ™( ⃗𝑀) reaches an extremum. Under some restrictions on the functional 𝑣(𝑒(βƒ—π‘₯)) and the basis functions π‘Šπ‘˜(βƒ—π‘₯), we obtain an approximate solution of the boundary value problem.

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