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) and f2(x).
f1(x)={xsin(x1)0(x=0)(x=0)
f2(x)={x2sin(x1)0(x=0)(x=0)
(1) Evaluate whether f1(x) and f2(x) are differentiable, respectively.
(2) Evaluate whether their derivatives f1′(x) and f2′(x) are continuous at x=0, respectively.
Q.2
Evaluate the directional differentiability and continuity of the following function.
f(x,y)={x2+y4xy20(Either x=0 or y=0)(Both x=0 and y=0)
Q.3
Compute the volume in the xyz-space for each of the following conditions.
(1) Under the surface z=excos(y) and over the rectangle defined by D=[0,1]×[0,2π] on the xy-plane.
(2) Under the surface of the paraboloid z=1−x2−y2 and over the xy-plane.
题目描述
- 定义
f1(x)={xsin(1/x),0,x=0x=0,f2(x)={x2sin(1/x),0,x=0x=0.
- 分别判断 f1,f2 是否可微;
- 分别判断导函数 f1′,f2′ 在 x=0 是否连续。
- 对
f(x,y)=⎩⎨⎧x2+y4xy2,0,(x,y)=(0,0),(x,y)=(0,0),
判断方向可微性与连续性。
- 求下列 xyz 空间体积:
- xy 平面矩形
D=[0,1]×[0,π/2] 上、曲面
z=excosy 下方的体积;
- 抛物面 z=1−x2−y2 与 xy 平面之间的体积。
- 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 C1。
- 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)
h→0limhf1(h)−f1(0)=h→0limhhsin(h1)=h→0limsin(h1)
does not exist. Hence f1 is not differentiable.
h→0limhf2(h)−f2(0)=h→0limhh2sin(h1)=h→0limhsin(h1)=0
by Squeezing theorem. Hence f2 is differentiable.
(2)
At x=0, f1′(x) does not exist, so it is not continuous.
From (1), f2′(0)=0 and limx→0f2′(x)=limx→0(2xsinx1−cosx1) does not exist, so f2′ is also not continuous at x=0.
Q.2
We have limh→0hf(h,0)−f(0,0)=0 and limh→0hf(0,h)−f(0,0)=0. So f is directionally differentiable at x and y axes.
By
x=y2,x→0limx2+y4xy2=21,
and
x=0,y→0limx2+y4xy2=0=21,
limit of f along different paths to (0,0) is different, which means the limit does not exist. Hence f is not continuous.
Q.3
(1)
V=∫01∫0π/2excos(y)dydx=∫01exdx∫0π/2cosy=e−1.
(2)
The partial surface to be integrated is
S={(x,y)∣x2+y2≤1}.
Let x=rcosθ,y=rsinθ, r∈[0,1] and θ∈[0,2π).
V=∬(x,y)∈Szdxdy=∬(r,θ)∈S(1−r2)∣J∣drdθ=∫02π∫01(1−r2)rdrdθ=2π∫01(r−r3)dr=2π(21−41)=2π.