Calculus · real student question

Let a(n) be the integral from x = 1/2 to x = 2 of 2^x/(1 + x^2)^n dx. Prove that a(n+1)/a(n) tends to 4/5 as n tends to infinity.

Question

Let an=1/222x(1+x2)ndx.a_n=\int_{1/2}^{2}\frac{2^{x}}{(1+x^{2})^{n}}\,dx. Prove that limnan+1an=45.\lim_{n\to\infty}\frac{a_{n+1}}{a_n}=\frac45.

Step-by-step solution

  1. Rewrite the ratio as a weighted average. Put g(x)=11+x2g(x)=\dfrac{1}{1+x^{2}}, so that an=1/222xg(x)ndxa_n=\int_{1/2}^{2}2^{x}g(x)^{n}\,dx and an+1=1/22g(x)2xg(x)ndxa_{n+1}=\int_{1/2}^{2}g(x)\cdot 2^{x}g(x)^{n}\,dx. Therefore an+1an=1/22g(x)wn(x)dx1/22wn(x)dx,wn(x)=2xg(x)n>0,\frac{a_{n+1}}{a_n}=\frac{\int_{1/2}^{2}g(x)\,w_n(x)\,dx}{\int_{1/2}^{2}w_n(x)\,dx},\qquad w_n(x)=2^{x}g(x)^{n}>0, which is exactly the average of gg against the positive weight wnw_n. An average always lies between the minimum and the maximum of gg, so the whole proof is about showing the weight concentrates where gg is largest.

  2. Locate the maximum of the base function. On x>0x>0 the function g(x)=1/(1+x2)g(x)=1/(1+x^{2}) is strictly decreasing, so on [12,2]\left[\frac12,2\right] it attains its maximum at the left endpoint: M=g ⁣(12)=11+14=45.M=g\!\left(\tfrac12\right)=\frac{1}{1+\frac14}=\frac45 . This already identifies 4/54/5 as the only candidate for the limit.

  3. Get the upper bound for free. Since g(x)Mg(x)\le M everywhere on the interval, an+1=1/22g(x)wn(x)dxM1/22wn(x)dx=Man,a_{n+1}=\int_{1/2}^{2}g(x)\,w_n(x)\,dx\le M\int_{1/2}^{2}w_n(x)\,dx=M\,a_n, so an+1an45\frac{a_{n+1}}{a_n}\le \frac45 for every nn, and hence lim supnan+1an45\limsup_{n\to\infty}\frac{a_{n+1}}{a_n}\le\frac45.

  4. Show the mass concentrates at the left endpoint. Fix ε>0\varepsilon>0. By continuity choose δ>0\delta>0 with g(x)>Mεg(x)>M-\varepsilon on [12,12+δ]\left[\frac12,\frac12+\delta\right] and with q:=g ⁣(12+δ)<Mεq:=g\!\left(\frac12+\delta\right)<M-\varepsilon. Splitting an=In+Jna_n=I_n+J_n at 12+δ\frac12+\delta and using monotonicity of gg, InC1(Mε)n,JnC2qn,C1=1/21/2+δ2xdx, C2=1/2+δ22xdx.I_n\ge C_1 (M-\varepsilon)^{n},\qquad J_n\le C_2 q^{n},\qquad C_1=\int_{1/2}^{1/2+\delta}2^{x}dx,\ C_2=\int_{1/2+\delta}^{2}2^{x}dx . Since q<Mεq<M-\varepsilon, the quotient Jn/InC2C1(qMε)n0J_n/I_n\le \frac{C_2}{C_1}\left(\frac{q}{M-\varepsilon}\right)^{n}\to 0, so the tail piece is negligible.

  5. Conclude with the lower bound. Because almost all of the weight sits on [12,12+δ]\left[\frac12,\frac12+\delta\right], where g>Mεg>M-\varepsilon, the weighted average satisfies an+1an>M2ε\frac{a_{n+1}}{a_n}>M-2\varepsilon for all large nn, so lim infnan+1anM2ε\liminf_{n\to\infty}\frac{a_{n+1}}{a_n}\ge M-2\varepsilon. As ε>0\varepsilon>0 was arbitrary, lim inf45\liminf\ge\frac45, and combined with the upper bound the limit equals 45\frac45.

  6. Check the rate numerically. Convergence is genuinely slow, since the concentration width shrinks only like 1/n1/n: numerical quadrature gives a21/a200.762a_{21}/a_{20}\approx 0.762, a41/a400.781a_{41}/a_{40}\approx 0.781 and a61/a600.787a_{61}/a_{60}\approx 0.787, all below 0.80.8 and increasing toward it, exactly as the two bounds above predict.

Answer

limnan+1an=maxx[1/2,2]11+x2=45\lim_{n\to\infty}\frac{a_{n+1}}{a_{n}}=\max_{x\in[1/2,\,2]}\frac{1}{1+x^{2}}=\frac{4}{5}

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