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早稲田大学 創造理工学研究科 経営システム工学専攻 2023年8月実施 微积分

Author

思齐塾, 祭音Myyura

Description

次の定積分(definite integral)を計算せよ。

I=ex2dxI = \int_{-\infty}^{\infty} e^{-x^2} dx

题目描述

计算高斯反常积分

I=ex2dx.I=\int_{-\infty}^{\infty}e^{-x^2}\,dx.

Kai

To evaluate the Gaussian integral I=ex2dxI = \int_{-\infty}^{\infty} e^{-x^2} dx , we can use the trick of squaring the integral and converting to polar coordinates.

Let I=ex2dxI = \int_{-\infty}^{\infty} e^{-x^2} dx . Then, I2=(ex2dx)(ey2dy)=e(x2+y2)dxdyI^2 = \left(\int_{-\infty}^{\infty} e^{-x^2} dx\right) \left(\int_{-\infty}^{\infty} e^{-y^2} dy\right) = \int_{-\infty}^{\infty} \int_{-\infty}^{\infty} e^{-(x^2+y^2)} dx dy .

Now, we convert to polar coordinates: x=rcosθx = r\cos\theta , y=rsinθy = r\sin\theta , and x2+y2=r2x^2 + y^2 = r^2 . Also, dxdy=rdrdθdx dy = r dr d\theta . The limits of integration become 0r<0 \leq r < \infty and 0θ2π0 \leq \theta \leq 2\pi . So, I2=02π0er2rdrdθI^2 = \int_{0}^{2\pi} \int_{0}^{\infty} e^{-r^2} r dr d\theta .

We can evaluate the inner integral by using the substitution u=r2u = r^2 , so du=2rdrdu = 2r dr , and rdr=12dur dr = \frac{1}{2} du . The limits of integration for uu are 00 to \infty . Thus, 0er2rdr=0eu12du=120eudu=12[eu]0=12[0(1)]=12\int_{0}^{\infty} e^{-r^2} r dr = \int_{0}^{\infty} e^{-u} \frac{1}{2} du = \frac{1}{2} \int_{0}^{\infty} e^{-u} du = \frac{1}{2} [-e^{-u}]_{0}^{\infty} = \frac{1}{2} [0 - (-1)] = \frac{1}{2} .

Therefore, I2=02π12dθ=1202πdθ=12[θ]02π=12(2π0)=πI^2 = \int_{0}^{2\pi} \frac{1}{2} d\theta = \frac{1}{2} \int_{0}^{2\pi} d\theta = \frac{1}{2} [\theta]_{0}^{2\pi} = \frac{1}{2} (2\pi - 0) = \pi .

Since I2=πI^2 = \pi , we have I=πI = \sqrt{\pi} .

Therefore, the value of the definite integral is π\sqrt{\pi} .

I=ex2dx=πI = \int_{-\infty}^{\infty} e^{-x^2} dx = \sqrt{\pi}