+15점 · 함수를 사용하여 x n \displaystyle x_{n} x n 을 함수 값들의 평균의 형태를 바꾸었는가? +15점 · 극한값을 바르게 계산하였는가? 1. f ( x ) = 1 1 + x \displaystyle f(x)=\frac{1}{1+x} f ( x ) = 1 + x 1 는 [ 0 , 1 ] \displaystyle [0,1] [ 0 , 1 ] 에서 연속함수이다. Correction. 여기서 연속성을 사용하는 구간은 [ 0 , 2 ] \displaystyle [0,2] [ 0 , 2 ] 이다. [ 0 , 1 ] \displaystyle [0,1] [ 0 , 1 ] 은 [ 0 , 2 ] \displaystyle [0,2] [ 0 , 2 ] 의 오기다. 그러나 원칙에 따라 원문 표기를 그대로 실었다.x n = 1 n ∑ k = 1 2 n 2 n 2 n + 2 k − 1 = 1 n ∑ k = 1 2 n 1 1 + 2 k − 1 2 n = 1 n ∑ k = 1 2 n f ( 2 k − 1 2 n ) \displaystyle x_{n}=\frac{1}{n}\sum_{k=1}^{2n}\frac{2n}{2n+2k-1}=\frac{1}{n}\sum_{k=1}^{2n}\frac{1}{1+\frac{2k-1}{2n}}=\frac{1}{n}\sum_{k=1}^{2n}f\left(\frac{2k-1}{2n}\right) x n = n 1 k = 1 ∑ 2 n 2 n + 2 k − 1 2 n = n 1 k = 1 ∑ 2 n 1 + 2 n 2 k − 1 1 = n 1 k = 1 ∑ 2 n f ( 2 n 2 k − 1 ) 이다.lim n → ∞ x n = lim n → ∞ 1 n ∑ k = 1 2 n f ( 2 k − 1 2 n ) = ∫ 0 2 f ( x ) d x = ∫ 0 2 1 1 + x d x = ln 3. \displaystyle \lim_{n\to\infty}x_{n}=\lim_{n\to\infty}\frac{1}{n}\sum_{k=1}^{2n}f\left(\frac{2k-1}{2n}\right)=\int_{0}^{2}f(x)\,dx=\int_{0}^{2}\frac{1}{1+x}\,dx=\ln3. n → ∞ lim x n = n → ∞ lim n 1 k = 1 ∑ 2 n f ( 2 n 2 k − 1 ) = ∫ 0 2 f ( x ) d x = ∫ 0 2 1 + x 1 d x = ln 3.
+15점 · 주어진 조건을 이용하여 위해 ∫ x 3 x f ′ ( t ) d t \displaystyle \int_{x}^{\sqrt{3}x}f^{\prime}(t)\,dt ∫ x 3 x f ′ ( t ) d t 을 적절한 형태로 바꾸었는가? Correction. “주어진 조건을 이용하여 위해”에서 “위해”는 불필요하게 들어갔다. 그러나 원칙에 따라 원문 표기를 그대로 실었다. +15점 · 극한값을 바르게 계산하였는가? 2. ∫ x 3 x f ′ ( t ) d t = [ f ′ ( t ) t ] x 3 x − ∫ x 3 x f ′ ′ ( t ) t d t = [ f ′ ( t ) t ] x 3 x − ∫ x 3 x sin t d t = [ f ′ ( t ) t ] x 3 x + [ cos t ] x 3 x = f ′ ( 3 x ) 3 x − f ′ ( x ) x + cos ( 3 x ) − cos x \displaystyle \begin{aligned}\int_{x}^{\sqrt{3}x}f^{\prime}(t)\,dt&=\Biggl[f^{\prime}(t)t\Biggr]_{x}^{\sqrt{3}x}-\int_{x}^{\sqrt{3}x}f^{\prime\prime}(t)t\,dt\\&=\Biggl[f^{\prime}(t)t\Biggr]_{x}^{\sqrt{3}x}-\int_{x}^{\sqrt{3}x}\sin t\,dt=\Biggl[f^{\prime}(t)t\Biggr]_{x}^{\sqrt{3}x}+\Biggl[\cos t\Biggr]_{x}^{\sqrt{3}x}\\&=f^{\prime}(\sqrt{3}x)\sqrt{3}x-f^{\prime}(x)x+\cos(\sqrt{3}x)-\cos x\end{aligned} ∫ x 3 x f ′ ( t ) d t = [ f ′ ( t ) t ] x 3 x − ∫ x 3 x f ′′ ( t ) t d t = [ f ′ ( t ) t ] x 3 x − ∫ x 3 x sin t d t = [ f ′ ( t ) t ] x 3 x + [ cos t ] x 3 x = f ′ ( 3 x ) 3 x − f ′ ( x ) x + cos ( 3 x ) − cos x lim x → π 3 ∫ x 3 x f ′ ( t ) d t = lim x → π 3 { f ′ ( 3 x ) 3 x − f ′ ( x ) x + cos ( 3 x ) − cos x } = lim x → π 3 f ′ ( 3 x ) lim x → π 3 3 x − lim x → π 3 f ′ ( x ) lim x → π 3 x + cos π − cos ( π 3 ) = 2 3 π − 1 − cos π 3 = 2 3 π − 0.76 \displaystyle \begin{aligned}\lim_{x\to\frac{\pi}{\sqrt{3}}}\int_{x}^{\sqrt{3}x}f^{\prime}(t)\,dt&=\lim_{x\to\frac{\pi}{\sqrt{3}}}\{f^{\prime}(\sqrt{3}x)\sqrt{3}x-f^{\prime}(x)x+\cos(\sqrt{3}x)-\cos x\}\\&=\lim_{x\to\frac{\pi}{\sqrt{3}}}f^{\prime}(\sqrt{3}x)\lim_{x\to\frac{\pi}{\sqrt{3}}}\sqrt{3}x-\lim_{x\to\frac{\pi}{\sqrt{3}}}f^{\prime}(x)\lim_{x\to\frac{\pi}{\sqrt{3}}}x+\cos\pi-\cos\left(\frac{\pi}{\sqrt{3}}\right)\\&=\frac{2}{3}\pi-1-\cos\frac{\pi}{\sqrt{3}}=\frac{2}{3}\pi-0.76\end{aligned} x → 3 π lim ∫ x 3 x f ′ ( t ) d t = x → 3 π lim { f ′ ( 3 x ) 3 x − f ′ ( x ) x + cos ( 3 x ) − cos x } = x → 3 π lim f ′ ( 3 x ) x → 3 π lim 3 x − x → 3 π lim f ′ ( x ) x → 3 π lim x + cos π − cos ( 3 π ) = 3 2 π − 1 − cos 3 π = 3 2 π − 0.76
+20점 · 코사인법칙을 활용해서 S k \displaystyle S_{k} S k 를 k \displaystyle k k 와 n \displaystyle n n 에 대한 식으로 표현했는가? +20점 · 극한값을 바르게 계산하였는가? 3. 오른쪽 그림에서 A P k ‾ 2 = 1 2 + 1 2 − 2 × 1 × 1 × cos ( π n + 1 k ) = 2 − 2 cos ( π n + 1 k ) \displaystyle \overline{\mathrm{AP}_{k}}^{2}=1^{2}+1^{2}-2\times1\times1\times\cos\left(\frac{\pi}{n+1}k\right)=2-2\cos\left(\frac{\pi}{n+1}k\right) AP k 2 = 1 2 + 1 2 − 2 × 1 × 1 × cos ( n + 1 π k ) = 2 − 2 cos ( n + 1 π k ) P k B ‾ 2 = 4 − A P k ‾ 2 = 2 + 2 cos ( π n + 1 k ) \displaystyle \overline{\mathrm{P}_{k}\mathrm{B}}^{2}=4-\overline{\mathrm{AP}_{k}}^{2}=2+2\cos\left(\frac{\pi}{n+1}k\right) P k B 2 = 4 − AP k 2 = 2 + 2 cos ( n + 1 π k ) 이고, 따라서S k 2 = ( 1 2 × A P k ‾ × P k B ‾ ) 2 = 1 4 ( 2 − 2 cos ( π n + 1 k ) ) ( 2 + 2 cos ( π n + 1 k ) ) = sin 2 ( π n + 1 k ) \displaystyle \begin{aligned}S_{k}^{2}&=\left(\frac{1}{2}\times\overline{\mathrm{AP}_{k}}\times\overline{\mathrm{P}_{k}\mathrm{B}}\right)^{2}=\frac{1}{4}\left(2-2\cos\left(\frac{\pi}{n+1}k\right)\right)\left(2+2\cos\left(\frac{\pi}{n+1}k\right)\right)\\&=\sin^{2}\left(\frac{\pi}{n+1}k\right)\end{aligned} S k 2 = ( 2 1 × AP k × P k B ) 2 = 4 1 ( 2 − 2 cos ( n + 1 π k ) ) ( 2 + 2 cos ( n + 1 π k ) ) = sin 2 ( n + 1 π k )
이므로 lim n → ∞ S 1 2 + S 2 2 + ⋯ + S n 2 n + 1 = lim n → ∞ ∑ k = 1 n sin 2 ( π n + 1 k ) 1 n + 1 = lim n + 1 → ∞ ∑ k = 1 n + 1 sin 2 ( π n + 1 k ) 1 n + 1 = lim n + 1 → ∞ 1 π ∑ k = 1 n + 1 sin 2 ( 0 + π − 0 n + 1 k ) π − 0 n + 1 = 1 π ∫ 0 π sin 2 t d t \displaystyle \begin{aligned}\lim_{n\to\infty}\frac{S_{1}^{2}+S_{2}^{2}+\cdots+S_{n}^{2}}{n+1}&=\lim_{n\to\infty}\sum_{k=1}^{n}\sin^{2}\left(\frac{\pi}{n+1}k\right)\frac{1}{n+1}=\lim_{n+1\to\infty}\sum_{k=1}^{n+1}\sin^{2}\left(\frac{\pi}{n+1}k\right)\frac{1}{n+1}\\&=\lim_{n+1\to\infty}\frac{1}{\pi}\sum_{k=1}^{n+1}\sin^{2}\left(0+\frac{\pi-0}{n+1}k\right)\frac{\pi-0}{n+1}=\frac{1}{\pi}\int_{0}^{\pi}\sin^{2}t\,dt\end{aligned} n → ∞ lim n + 1 S 1 2 + S 2 2 + ⋯ + S n 2 = n → ∞ lim k = 1 ∑ n sin 2 ( n + 1 π k ) n + 1 1 = n + 1 → ∞ lim k = 1 ∑ n + 1 sin 2 ( n + 1 π k ) n + 1 1 = n + 1 → ∞ lim π 1 k = 1 ∑ n + 1 sin 2 ( 0 + n + 1 π − 0 k ) n + 1 π − 0 = π 1 ∫ 0 π sin 2 t d t 이고, 부분적분법에 의해 ∫ sin 2 t d t = 1 2 ( t − cos t sin t ) + C \displaystyle \int\sin^{2}t\,dt=\frac{1}{2}(t-\cos t\sin t)+C ∫ sin 2 t d t = 2 1 ( t − cos t sin t ) + C 이므로, 구하는 값은 1 π ∫ 0 π sin 2 t d t = 1 2 π [ t − cos t sin t ] 0 π = 1 2 \displaystyle \frac{1}{\pi}\int_{0}^{\pi}\sin^{2}t\,dt=\frac{1}{2\pi}\Biggl[t-\cos t\sin t\Biggr]_{0}^{\pi}=\frac{1}{2} π 1 ∫ 0 π sin 2 t d t = 2 π 1 [ t − cos t sin t ] 0 π = 2 1 이다.