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京都大学 情報学研究科 知能情報学専攻 2024年2月実施 基礎科目 F1-2

Author

itsuitsuki, 祭音Myyura

Description

Q.1

Consider the following functions f1(x)f_1(x) and f2(x)f_2(x).

f1(x)={xsin(1x)(x0)0(x=0)f_1(x) = \begin{cases} x\sin\left(\frac{1}{x}\right) & (x \neq 0) \\ 0 & (x = 0) \end{cases}
f2(x)={x2sin(1x)(x0)0(x=0)f_2(x) = \begin{cases} x^2\sin\left(\frac{1}{x}\right) & (x \neq 0) \\ 0 & (x = 0) \end{cases}

(1) Evaluate whether f1(x)f_1(x) and f2(x)f_2(x) are differentiable, respectively.

(2) Evaluate whether their derivatives f1(x){f_1}'(x) and f2(x){f_2}'(x) are continuous at x=0x = 0, respectively.

Q.2

Evaluate the directional differentiability and continuity of the following function.

f(x,y)={xy2x2+y4(Either x0 or y0)0(Both x=0 and y=0)f(x, y) = \begin{cases} \frac{xy^2}{x^2 + y^4} & (\text{Either } x \neq 0 \text{ or } y \neq 0) \\ 0 & (\text{Both } x = 0 \text{ and } y = 0) \end{cases}

Q.3

Compute the volume in the xyzxyz-space for each of the following conditions.

(1) Under the surface z=excos(y)z = e^x \cos(y) and over the rectangle defined by D=[0,1]×[0,π2]D = [0, 1] \times \left[0, \frac{\pi}{2}\right] on the xyxy-plane.

(2) Under the surface of the paraboloid z=1x2y2z = 1 - x^2 - y^2 and over the xyxy-plane.

题目描述

  1. 定义
    f1(x)={xsin(1/x),x00,x=0,f2(x)={x2sin(1/x),x00,x=0.f_1(x)=\begin{cases}x\sin(1/x),&x\ne0\\0,&x=0,\end{cases} \qquad f_2(x)=\begin{cases}x^2\sin(1/x),&x\ne0\\0,&x=0.\end{cases}
    1. 分别判断 f1,f2f_1,f_2 是否可微;
    2. 分别判断导函数 f1,f2f_1',f_2'x=0x=0 是否连续。
  2. f(x,y)={xy2x2+y4,(x,y)(0,0),0,(x,y)=(0,0),f(x,y)=\begin{cases} \dfrac{xy^2}{x^2+y^4},&(x,y)\ne(0,0),\\ 0,&(x,y)=(0,0), \end{cases}
    判断方向可微性与连续性。
  3. 求下列 xyzxyz 空间体积:
    1. xyxy 平面矩形 D=[0,1]×[0,π/2]D=[0,1]\times[0,\pi/2] 上、曲面 z=excosyz=e^x\cos y 下方的体积;
    2. 抛物面 z=1x2y2z=1-x^2-y^2xyxy 平面之间的体积。

考点

  • 连续性、可微性与导函数连续性:用差商和振荡项分别判断零点行为,区分可微与 C1C^1
  • 多元方向导数不蕴含连续:沿直线计算原点各方向导数,再用非线性路径检验二元极限。
  • 二重积分求体积:在矩形域直接分离积分,在圆盘域用极坐标积分。

Kai

Q.1

(1)

limh0f1(h)f1(0)h=limh0hsin(1h)h=limh0sin(1h)\lim_{h\to 0}{f_1(h)-f_1(0)\over h}=\lim_{h\to 0}{h\sin(\frac1h)\over h}=\lim_{h\to 0}{\sin(\frac1h)}

does not exist. Hence f1f_1 is not differentiable.

limh0f2(h)f2(0)h=limh0h2sin(1h)h=limh0hsin(1h)=0\lim_{h\to 0}{f_2(h)-f_2(0)\over h}=\lim_{h\to 0}{h^2\sin(\frac1h)\over h}=\lim_{h\to 0}h\sin(\frac1h)=0

by Squeezing theorem. Hence f2f_2 is differentiable.

(2)

At x=0x=0, f1(x)f_1'(x) does not exist, so it is not continuous.

From (1), f2(0)=0f'_2(0)=0 and limx0f2(x)=limx0(2xsin1xcos1x)\lim_{x\to 0}f_2'(x)=\lim_{x\to 0}(2x\sin{\frac1x}-\cos{\frac1x}) does not exist, so f2f'_2 is also not continuous at x=0x=0.

Q.2

We have limh0f(h,0)f(0,0)h=0\lim_{h\to0}{f(h,0)-f(0,0)\over h}=0 and limh0f(0,h)f(0,0)h=0\lim_{h\to0}{f(0,h)-f(0,0)\over h}=0. So ff is directionally differentiable at xx and yy axes.

By

limx=y2,x0xy2x2+y4=12,\lim_{x=y^2,x\to 0}{xy^2\over x^2+y^4}=\frac12,

and

limx=0,y0xy2x2+y4=012,\lim_{x=0,y\to 0}{xy^2\over x^2+y^4}=0\ne \frac12,

limit of ff along different paths to (0,0)(0,0) is different, which means the limit does not exist. Hence ff is not continuous.

Q.3

(1)

V=010π/2excos(y)dydx=01exdx0π/2cosy=e1.\begin{aligned} V&=\int_0^1\int_0^{\pi/2}e^x\cos (y) dy dx \\ &=\int_0^1e^x dx\int_0^{\pi/2}\cos y \\ &=e-1. \end{aligned}

(2)

The partial surface to be integrated is

S={(x,y)x2+y21}.S=\{(x,y)|x^2+y^2\le 1\}.

Let x=rcosθ,y=rsinθx=r\cos \theta,y=r\sin\theta, r[0,1]r\in[0,1] and θ[0,2π)\theta\in[0,2\pi).

V=(x,y)Szdxdy=(r,θ)S(1r2)Jdrdθ=02π01(1r2)rdrdθ=2π01(rr3)dr=2π(1214)=π2.\begin{aligned} V&=\iint_{(x,y)\in S}zd xd y\\ &=\iint_{(r,\theta)\in S}(1-r^2)|J|d rd \theta \\&=\int_0^{2\pi}\int_0^1(1-r^2)rd rd \theta \\&=2\pi \int_0^1(r-r^3)d r \\&=2\pi (\frac12-\frac14)={\pi\over 2}. \end{aligned}