Riley hobson bence · Problem 6.23

Multiple integrals

Mathematics — Methods · multiple-integrals-volume-recurrence

Problem

(a) Let RR be a real positive number and define KmK_m by Km=∫−RR(R2−x2)mdx.K_m = \int_{-R}^{R} \left(R^2 - x^2\right)^m dx. Show, using integration by parts, that KmK_m satisfies the recurrence relation (2m+1)Km=2mR2Km−1.(2m + 1)K_m = 2mR^2 K_{m-1}. (b) For integer nn, define In=KnI_n = K_n and Jn=Kn+1/2J_n = K_{n+1/2}. Evaluate I0I_0 and J0J_0 directly and hence prove that In=22n+1(n!)2R2n+1(2n+1)!andJn=π(2n+1)!R2n+222n+1n!(n+1)!.I_n = \frac{2^{2n+1}(n!)^2 R^{2n+1}}{(2n+1)!} \qquad \text{and} \qquad J_n = \frac{\pi(2n+1)! R^{2n+2}}{2^{2n+1} n!(n+1)!}. (c) A sequence of functions Vn(R)V_n(R) is defined by V0(R)=1,V_0(R) = 1, Vn(R)=∫−RRVn−1 ⁣(R2−x2)dx,n≥1.V_n(R) = \int_{-R}^{R} V_{n-1}\!\left(\sqrt{R^2 - x^2}\right) dx, \qquad n \geq 1. Prove by induction that V2n(R)=πnR2nn!,V2n+1(R)=πn22n+1n!R2n+1(2n+1)!.V_{2n}(R) = \frac{\pi^n R^{2n}}{n!}, \qquad V_{2n+1}(R) = \frac{\pi^n 2^{2n+1} n! R^{2n+1}}{(2n+1)!}. (d) For interest, ((i)) show that V2n+2(1)<V2n(1)V_{2n+2}(1) < V_{2n}(1) and V2n+1(1)<V2n−1(1)V_{2n+1}(1) < V_{2n-1}(1) for all n≥3n \geq 3; ((ii)) hence, by explicitly writing out Vk(R)V_k(R) for 1≤k≤81 \leq k \leq 8 (say), show that the `volume' of the totally symmetric solid of unit radius is a maximum in five dimensions.
Intuitive explanation

The recurrence relation is the bridge between different powers of the polynomial. Use integration by parts strategically: differentiate the power (R2−x2)m(R^2 - x^2)^m to reduce the exponent, and integrate dxdx to create a factor of xx. This will generate a term involving Km−1K_{m-1} and a boundary term that vanishes—rearranging gives your recurrence. Once you have the relation, you can climb from base cases I0I_0 and J0J_0 (which you compute directly) to general formulas by repeatedly applying it, keeping track of the factorial and power patterns that emerge.

Intuitive explanation

The recurrence relation is the bridge between different powers of the polynomial. Use integration by parts strategically: differentiate the power (R2−x2)m(R^2 - x^2)^m to reduce the exponent, and integrate dxdx to create a factor of xx. This will generate a term involving Km−1K_{m-1} and a boundary term that vanishes—rearranging gives your recurrence. Once you have the relation, you can climb from base cases I0I_0 and J0J_0 (which you compute directly) to general formulas by repeatedly applying it, keeping track of the factorial and power patterns that emerge.

Related theory

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