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京都大学 情報学研究科 知能情報学専攻 2022年8月実施 情報学基礎 F1-2

Author

Isidore, 祭音Myyura

Description

設問1

以下の関数の xx に関する nn 階導関数を求めよ。ただし aa は実数、かつ a>0a>0a1a \neq 1 である。

  • (1) logex\log_e x
  • (2) axa^x
  • (3) x2exx^2e^x
  • (4) 1x21\frac{1}{x^2-1}

設問2

z=f(x,y)z = f(x,y), x=eucosvx = e^u \cos v, y=eusinvy = e^u \sin v とする。2zu2+2zv2\frac{\partial^2 z}{\partial u^2} + \frac{\partial^2 z}{\partial v^2}x,y,2zx2,2zy2x, y, \frac{\partial^2 z}{\partial x^2}, \frac{\partial^2 z}{\partial y^2} で表せ。

設問3

以下の積分を求めよ。計算過程を明示すること。

  • (1) ex2dx\int^{\infty}_{-\infty} e^{-x^2} dx
  • (2) 00(ax2+by2)e(ax2+by2)dxdy\int_0^{\infty} \int_0^{\infty} (ax^2 + by^2)e^{-(ax^2 + by^2)} dxdy、但し、a>0a>0 かつ b>0b>0 とし、(1) の結果を用いてよい。

题目描述

  1. 对实数 a>0a>0a1a\ne1,求下列函数关于 xxnn 阶导数:
    1. lnx\ln x
    2. axa^x
    3. x2exx^2e^x
    4. 1x21\dfrac1{x^2-1}
  2. z=f(x,y)z=f(x,y)x=eucosvx=e^u\cos vy=eusinvy=e^u\sin v。用 x,y,zxx,zyyx,y,z_{xx},z_{yy} 表示 zuu+zvvz_{uu}+z_{vv}
  3. 写出过程并计算:
    1. ex2dx\displaystyle\int_{-\infty}^{\infty}e^{-x^2}\,dx
    2. 00(ax2+by2)e(ax2+by2)dxdy\displaystyle\int_0^\infty\int_0^\infty (ax^2+by^2)e^{-(ax^2+by^2)}\,dx\,dy, 其中 a,b>0a,b>0,可使用第 1 小问结果。

考点

  • 高阶导数:归纳对数、指数、多项式乘指数及部分分式的 nn 阶公式。
  • 多元链式法则与极坐标:识别 (u,v)(u,v) 为对数极坐标,推导共形尺度下 Laplace 算子的变换。
  • Gaussian 积分与二重积分:用极坐标求 Gaussian 积分,再通过缩放和可分离积分计算带二次权的第一象限积分。

Kai

設問1

(1)

f(n)(x)=(1)n+1(n1)!xnf^{(n)}(x) = (-1)^{n+1}\frac{(n-1)!}{x^n}

(2)

f(n)(x)=ax(logea)nf^{(n)}(x) = a^x(\log_e a)^n

(3)

f(n)(x)=k=0n(nk)(x2)(k)(ex)(nk)=k=02(nk)(x2)(k)(ex)(nk)=(n0)(x2)(0)(ex)(n)+(n1)(x2)(1)(ex)(n1)+(n2)(x2)(2)(ex)(n2)=x2ex+2nxex+n(n1)ex=(x2+2nx+n(n1))ex\begin{aligned} f^{(n)}(x) &= \sum_{k=0}^{n}\binom{n}{k}(x^{2})^{(k)}(e^{x})^{(n-k)} \\ &= \sum_{k=0}^{2}\binom{n}{k}(x^{2})^{(k)}(e^{x})^{(n-k)} \\ &= \binom{n}{0}(x^{2})^{(0)}(e^{x})^{(n)}+\binom{n}{1}(x^{2})^{(1)}(e^{x})^{(n-1)}+\binom{n}{2}(x^{2})^{(2)}(e^{x})^{(n-2)}\\ &= x^{2}e^{x}+2nxe^{x}+n(n-1)e^{x} \\ &= \left(x^{2}+2nx+n(n-1)\right)e^{x} \end{aligned}

(4)

f(n)(x)=n!2(1)n{(x1)n1(x+1)n1}f^{(n)}(x) = \frac{n!}{2}(-1)^{n}\left\{(x-1)^{-n-1}-(x+1)^{-n-1}\right\}

設問2

2zu2+2zv2=(2zx2+2zy2)(x2+y2)\frac{\partial^2 z}{\partial u^2} + \frac{\partial^2 z}{\partial v^2} = (\frac{\partial^2 z}{\partial x^2} + \frac{\partial^2 z}{\partial y^2})(x^2 + y^2)

設問3

(1)

Perform the substitution x2=ux^2 = u, we have

ex2dx=20ex2dx=0u12eudu\int^{\infty}_{-\infty}e^{-x^2}\mathrm{d}x = 2\int^{\infty}_{0}e^{-x^2}\mathrm{d}x = \int^{\infty}_{0}u^{-\frac{1}{2}}e^{-u}\mathrm{d}u

By the properties of Gamma Function, the above integral equals

0u121eudu=Γ(12)=π\int^{\infty}_{0}u^{\frac{1}{2}-1}e^{-u}\mathrm{d}u = \Gamma(\frac{1}{2}) = \sqrt{\pi}

(2)

Let u=ax,v=byu=\sqrt{a}x,v=\sqrt{b}y.

00(ax2+by2)e(ax2+by2)dxdy=1ab00(u2+v2)e(u2+v2)dudv=2ab00u2e(u2+v2)dudv=2ab0u2eu2du0ev2dv=πab0u2eu2du\begin{aligned} \int_{0}^{\infty}\int_{0}^{\infty}(ax^{2}+by^{2})e^{-(ax^{2}+by^{2})}dxdy &= \frac{1}{\sqrt{ab}}\int_{0}^{\infty}\int_{0}^{\infty}(u^{2}+v^{2})e^{-(u^{2}+v^{2})}dudv\\ &= \frac{2}{\sqrt{ab}}\int_{0}^{\infty}\int_{0}^{\infty}u^{2}e^{-(u^{2}+v^{2})}dudv\\ &= \frac{2}{\sqrt{ab}}\int_{0}^{\infty}u^{2}e^{-u^{2}}du\int_{0}^{\infty}e^{-v^{2}}dv\\ &= \frac{\sqrt{\pi}}{\sqrt{ab}}\int_{0}^{\infty}u^{2}e^{-u^{2}}du \end{aligned}
0u2eu2du=0u(ueu2)du=0u(eu22)du=[ueu22]0+120eu2du=14eu2du=π4\begin{aligned} \int_{0}^{\infty}u^{2}e^{-u^{2}}du &= \int_{0}^{\infty}u\cdot (ue^{-u^{2}})du\\ &= \int_{0}^{\infty}u\cdot\left(\frac{e^{-u^{2}}}{-2}\right)^{\prime}du\\ &= \left[\frac{ue^{-u^{2}}}{-2}\right]_{0}^{\infty}+\frac{1}{2}\int_{0}^{\infty}e^{-u^{2}}du\\ &= \frac{1}{4}\int_{-\infty}^{\infty}e^{-u^{2}}du \\ &= \frac{\sqrt{\pi}}{4} \end{aligned}

Hence the result is π4ab\frac{\pi}{4\sqrt{ab}}.