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埼玉大学 理工学研究科 数理電子情報系専攻 情報システム工学コース 2018年8月実施 微分積分

Author

思齐塾, 祭音Myyura

Description

  1. 以下の問に答えよ. [ Solve the following problems. ]

(a) 次の極限値を求めよ. [ Find the following limit. ]

limx0sinx21cosx\lim_{x \to 0} \frac{\sin x^2}{1 - \cos x}

(b) 以下の関数のマクローリン展開を x4x^4 の項まで求めよ. [ Find the Maclaurin expansion of the following function up to the term of x4x^4 . ]

f(x)=x2cosxf(x) = x^2 \cos x

(c) 次の不定積分を求めよ. [ Find the following indefinite integral. ]

exsinxdx\int e^x \sin x \, dx

(d) a,ba, b を定数とする。次の二重積分を求めよ. [ Let aa and bb be constants. Find the following double integral. ]

D(ax2+by2)dxdy,D:x2+y21\iint_D (ax^2 + by^2) \, dx \, dy, \quad D: x^2 + y^2 \leq 1

题目描述

  1. 回答下列问题。

(a) 求极限

limx0sinx21cosx.\lim_{x\to0}\frac{\sin x^2}{1-\cos x}.

(b) 将函数

f(x)=x2cosxf(x)=x^2\cos x

作 Maclaurin 展开,写到 x4x^4 项为止。

(c) 求不定积分

exsinxdx.\int e^x\sin x\,dx.

(d) 设 a,ba,b 为常数,计算二重积分

D(ax2+by2)dxdy,\iint_D(ax^2+by^2)\,dx\,dy,

其中

D:x2+y21.D:\quad x^2+y^2\leq1.

Kai

(a)

limx0sinx21cosx=limx0sinx21cosx1+cosx1+cosx=limx0sinx2(1+cosx)sin2x=limx0sinx2x2x2sin2x(1+cosx)=limx0sinx2x2(xsinx)2(1+cosx)=112(1+1)=2\lim_{x \to 0} \frac{\sin x^2}{1 - \cos x} = \lim_{x \to 0} \frac{\sin x^2}{1 - \cos x} \cdot \frac{1 + \cos x}{1 + \cos x} = \lim_{x \to 0} \frac{\sin x^2 (1 + \cos x)}{\sin^2 x} = \lim_{x \to 0} \frac{\sin x^2}{x^2} \cdot \frac{x^2}{\sin^2 x} \cdot (1 + \cos x) = \lim_{x \to 0} \frac{\sin x^2}{x^2} \cdot \left(\frac{x}{\sin x}\right)^2 \cdot (1 + \cos x) = 1 \cdot 1^2 \cdot (1 + 1) = 2

(b)

cosx=1x22!+x44!\cos x = 1 - \frac{x^2}{2!} + \frac{x^4}{4!} - \dots
f(x)=x2cosx=x2(1x22+x424)=x2x42+O(x6)f(x) = x^2 \cos x = x^2 \left(1 - \frac{x^2}{2} + \frac{x^4}{24} - \dots \right) = x^2 - \frac{x^4}{2} + O(x^6)

So the Maclaurin expansion up to the term of x4x^4 is

x2x42x^2 - \frac{x^4}{2}

.

(c) Let I=exsinxdxI = \int e^x \sin x \, dx . Integrating by parts, we have

I=exsinxexcosxdxI = e^x \sin x - \int e^x \cos x \, dx
I=exsinx(excosxex(sinx)dx)=exsinxexcosxexsinxdx=exsinxexcosxII = e^x \sin x - \left( e^x \cos x - \int e^x (-\sin x) \, dx \right) = e^x \sin x - e^x \cos x - \int e^x \sin x \, dx = e^x \sin x - e^x \cos x - I

Thus, 2I=exsinxexcosx+C2I = e^x \sin x - e^x \cos x + C , so I=12ex(sinxcosx)+CI = \frac{1}{2} e^x (\sin x - \cos x) + C , where C is an arbitrary constant.

(d) Using polar coordinates x=rcosθx = r \cos \theta and y=rsinθy = r \sin \theta , we have x2+y2=r2x^2 + y^2 = r^2 and dxdy=rdrdθdx \, dy = r \, dr \, d\theta . The region DD is described by 0r10 \leq r \leq 1 and 0θ2π0 \leq \theta \leq 2\pi .

D(ax2+by2)dxdy=02π01(ar2cos2θ+br2sin2θ)rdrdθ=02π01(acos2θ+bsin2θ)r3drdθ\iint_D (ax^2 + by^2) \, dx \, dy = \int_0^{2\pi} \int_0^1 (a r^2 \cos^2 \theta + b r^2 \sin^2 \theta) r \, dr \, d\theta = \int_0^{2\pi} \int_0^1 (a \cos^2 \theta + b \sin^2 \theta) r^3 \, dr \, d\theta
=02π(acos2θ+bsin2θ)[r44]01dθ=1402π(acos2θ+bsin2θ)dθ=1402π(a1+cos(2θ)2+b1cos(2θ)2)dθ= \int_0^{2\pi} (a \cos^2 \theta + b \sin^2 \theta) \left[ \frac{r^4}{4} \right]_0^1 d\theta = \frac{1}{4} \int_0^{2\pi} (a \cos^2 \theta + b \sin^2 \theta) d\theta = \frac{1}{4} \int_0^{2\pi} \left( a \frac{1 + \cos(2\theta)}{2} + b \frac{1 - \cos(2\theta)}{2} \right) d\theta
=1802π(a+acos(2θ)+bbcos(2θ))dθ=1802π((a+b)+(ab)cos(2θ))dθ=18[(a+b)θ+ab2sin(2θ)]02π= \frac{1}{8} \int_0^{2\pi} (a + a\cos(2\theta) + b - b\cos(2\theta)) d\theta = \frac{1}{8} \int_0^{2\pi} ((a+b) + (a-b)\cos(2\theta)) d\theta = \frac{1}{8} \left[ (a+b)\theta + \frac{a-b}{2} \sin(2\theta) \right]_0^{2\pi}
=18(a+b)(2π)=π4(a+b)= \frac{1}{8} (a+b) (2\pi) = \frac{\pi}{4} (a+b)