前置知识: 高等数学

定积分与应用典型例题

12 minIntermediate2026/6/14

定积分与应用15道典型例题:定积分计算、变限积分、反常积分、几何与物理应用等核心题型。

1. 定积分基本计算

例1:求 ∫0π/2sin⁡xsin⁡x+cos⁡xdx\int_0^{\pi/2} \frac{\sin x}{\sin x + \cos x} dx

解:利用公式 ∫0π/2f(sin⁡x)dx=∫0π/2f(cos⁡x)dx\int_0^{\pi/2} f(\sin x) dx = \int_0^{\pi/2} f(\cos x) dx

设 I=∫0π/2sin⁡xsin⁡x+cos⁡xdxI = \int_0^{\pi/2} \frac{\sin x}{\sin x + \cos x} dx,J=∫0π/2cos⁡xsin⁡x+cos⁡xdxJ = \int_0^{\pi/2} \frac{\cos x}{\sin x + \cos x} dx

由对称性 I=JI = J,又 I+J=∫0π/2dx=π2I + J = \int_0^{\pi/2} dx = \frac{\pi}{2}

故 I=π4I = \frac{\pi}{4}


例2:求 ∫01ln⁡(1+x)1+x2dx\int_0^1 \frac{\ln(1+x)}{1+x^2} dx

解:令 x=tan⁡tx = \tan t,dx=sec⁡2t dtdx = \sec^2 t\, dt

∫0π/4ln⁡(1+tan⁡t)1+tan⁡2t⋅sec⁡2t dt=∫0π/4ln⁡(1+tan⁡t) dt\int_0^{\pi/4} \frac{\ln(1+\tan t)}{1+\tan^2 t} \cdot \sec^2 t\, dt = \int_0^{\pi/4} \ln(1+\tan t)\, dt

利用 1+tan⁡t=sin⁡t+cos⁡tcos⁡t=2cos⁡(π4−t)cos⁡t1+\tan t = \frac{\sin t + \cos t}{\cos t} = \frac{\sqrt{2}\cos(\frac{\pi}{4}-t)}{\cos t}

∫0π/4ln⁡2cos⁡(π4−t)cos⁡t dt=π4ln⁡2+∫0π/4ln⁡cos⁡(π4−t)dt−∫0π/4ln⁡cos⁡t dt\int_0^{\pi/4} \ln\frac{\sqrt{2}\cos(\frac{\pi}{4}-t)}{\cos t}\, dt = \frac{\pi}{4}\ln\sqrt{2} + \int_0^{\pi/4}\ln\cos\left(\frac{\pi}{4}-t\right)dt - \int_0^{\pi/4}\ln\cos t\, dt

后两项相等(变量替换 u=π4−tu = \frac{\pi}{4}-t),故:

∫01ln⁡(1+x)1+x2dx=π8ln⁡2\int_0^1 \frac{\ln(1+x)}{1+x^2} dx = \frac{\pi}{8}\ln 2

2. 变限积分求导

例3:求 ddx∫0x(x−t)f(t) dt\frac{d}{dx}\int_0^x (x-t)f(t)\, dt

解:

∫0x(x−t)f(t) dt=x∫0xf(t) dt−∫0xtf(t) dt\int_0^x (x-t)f(t)\, dt = x\int_0^x f(t)\, dt - \int_0^x tf(t)\, dt

ddx=∫0xf(t) dt+xf(x)−xf(x)=∫0xf(t) dt\frac{d}{dx} = \int_0^x f(t)\, dt + xf(x) - xf(x) = \int_0^x f(t)\, dt


例4:求 ddx∫x2exsin⁡t2 dt\frac{d}{dx}\int_{x^2}^{e^x} \sin t^2\, dt

解:设 F(u)=∫0usin⁡t2 dtF(u) = \int_0^u \sin t^2\, dt

ddx∫x2exsin⁡t2 dt=F′(ex)⋅ex−F′(x2)⋅2x=exsin⁡(e2x)−2xsin⁡(x4)\frac{d}{dx}\int_{x^2}^{e^x} \sin t^2\, dt = F'(e^x) \cdot e^x - F'(x^2) \cdot 2x = e^x \sin(e^{2x}) - 2x\sin(x^4)

3. 定积分的对称性

例5:求 ∫−11x3cos⁡x1+x4dx\int_{-1}^{1} \frac{x^3 \cos x}{1+x^4} dx

解:被积函数 f(x)=x3cos⁡x1+x4f(x) = \frac{x^3 \cos x}{1+x^4} 是奇函数(f(−x)=−f(x)f(-x) = -f(x)),积分区间关于原点对称。

∫−11x3cos⁡x1+x4dx=0\int_{-1}^{1} \frac{x^3 \cos x}{1+x^4} dx = 0


例6:求 ∫−π/2π/2(x3+sin⁡2x)cos⁡2x dx\int_{-\pi/2}^{\pi/2} (x^3 + \sin^2 x)\cos^2 x\, dx

解:x3cos⁡2xx^3\cos^2 x 是奇函数,积分为 0。

∫−π/2π/2sin⁡2xcos⁡2x dx=2∫0π/2sin⁡22x4 dx=12∫0π/21−cos⁡4x2 dx=π8\int_{-\pi/2}^{\pi/2} \sin^2 x \cos^2 x\, dx = 2\int_0^{\pi/2} \frac{\sin^2 2x}{4}\, dx = \frac{1}{2}\int_0^{\pi/2} \frac{1-\cos 4x}{2}\, dx = \frac{\pi}{8}

4. 华里士公式

例7:求 ∫0π/2sin⁡4xcos⁡2x dx\int_0^{\pi/2} \sin^4 x \cos^2 x\, dx

解:

∫0π/2sin⁡4xcos⁡2x dx=∫0π/2sin⁡4x(1−sin⁡2x) dx=I4−I6\int_0^{\pi/2} \sin^4 x \cos^2 x\, dx = \int_0^{\pi/2} \sin^4 x(1-\sin^2 x)\, dx = I_4 - I_6

由华里士公式:I4=34⋅12⋅π2=3π16I_4 = \frac{3}{4} \cdot \frac{1}{2} \cdot \frac{\pi}{2} = \frac{3\pi}{16},I6=56⋅34⋅12⋅π2=5π32I_6 = \frac{5}{6} \cdot \frac{3}{4} \cdot \frac{1}{2} \cdot \frac{\pi}{2} = \frac{5\pi}{32}

∫0π/2sin⁡4xcos⁡2x dx=3π16−5π32=π32\int_0^{\pi/2} \sin^4 x \cos^2 x\, dx = \frac{3\pi}{16} - \frac{5\pi}{32} = \frac{\pi}{32}

5. 反常积分

例8:判断 ∫0+∞x(1+x2)2dx\int_0^{+\infty} \frac{x}{(1+x^2)^2} dx 的收敛性并求值。

解:

∫0+∞x(1+x2)2dx=12∫0+∞d(1+x2)(1+x2)2=12[−11+x2]0+∞=12(0−(−1))=12\int_0^{+\infty} \frac{x}{(1+x^2)^2} dx = \frac{1}{2}\int_0^{+\infty} \frac{d(1+x^2)}{(1+x^2)^2} = \frac{1}{2}\left[-\frac{1}{1+x^2}\right]_0^{+\infty} = \frac{1}{2}(0-(-1)) = \frac{1}{2}


例9:求 ∫01ln⁡x dx\int_0^1 \ln x\, dx

解:

∫01ln⁡x dx=lim⁡ε→0+∫ε1ln⁡x dx=lim⁡ε→0+[xln⁡x−x]ε1\int_0^1 \ln x\, dx = \lim_{\varepsilon \to 0^+} \int_\varepsilon^1 \ln x\, dx = \lim_{\varepsilon \to 0^+} [x\ln x - x]_\varepsilon^1

=lim⁡ε→0+(−1−εln⁡ε+ε)=−1= \lim_{\varepsilon \to 0^+} (-1 - \varepsilon\ln\varepsilon + \varepsilon) = -1

(因为 lim⁡ε→0+εln⁡ε=0\lim_{\varepsilon \to 0^+} \varepsilon\ln\varepsilon = 0)

6. 定积分证明题

例10:证明:∫0af(x)dx=∫0af(a−x)dx\int_0^a f(x) dx = \int_0^a f(a-x) dx

证明:令 t=a−xt = a - x:

∫0af(a−x)dx=−∫a0f(t)dt=∫0af(t)dt=∫0af(x)dx\int_0^a f(a-x) dx = -\int_a^0 f(t) dt = \int_0^a f(t) dt = \int_0^a f(x) dx


例11:设 f(x)f(x) 在 [0,1][0,1] 连续,证明:∫01f(x)dx=∫01f(1−x)dx\int_0^1 f(x) dx = \int_0^1 f(1-x) dx,并利用此证明 ∫0π/2sin⁡xsin⁡x+cos⁡xdx=π4\int_0^{\pi/2} \frac{\sin x}{\sin x + \cos x} dx = \frac{\pi}{4}。

证明:令 t=1−xt = 1-x 即得。

I=∫0π/2sin⁡xsin⁡x+cos⁡xdxI = \int_0^{\pi/2} \frac{\sin x}{\sin x + \cos x} dx

I=∫0π/2sin⁡(π2−x)sin⁡(π2−x)+cos⁡(π2−x)dx=∫0π/2cos⁡xcos⁡x+sin⁡xdxI = \int_0^{\pi/2} \frac{\sin(\frac{\pi}{2}-x)}{\sin(\frac{\pi}{2}-x)+\cos(\frac{\pi}{2}-x)} dx = \int_0^{\pi/2} \frac{\cos x}{\cos x + \sin x} dx

2I=∫0π/2dx=π2⇒I=π42I = \int_0^{\pi/2} dx = \frac{\pi}{2} \Rightarrow I = \frac{\pi}{4}

7. 几何应用

例12:求由 y=x2y = x^2 和 y=2xy = 2x 所围图形的面积。

解:联立 x2=2xx^2 = 2x 得交点 x=0x = 0 和 x=2x = 2。

A=∫02(2x−x2)dx=[x2−x33]02=4−83=43A = \int_0^2 (2x - x^2) dx = \left[x^2 - \frac{x^3}{3}\right]_0^2 = 4 - \frac{8}{3} = \frac{4}{3}


例13:求 y=xy = \sqrt{x} 绕 xx 轴旋转(0≤x≤40 \leq x \leq 4)所得旋转体体积。

解:

V=π∫04(x)2dx=π∫04x dx=π⋅x22∣04=8πV = \pi \int_0^4 (\sqrt{x})^2 dx = \pi \int_0^4 x\, dx = \pi \cdot \frac{x^2}{2}\Big|_0^4 = 8\pi

8. 物理应用

例14:一弹簧的力 F(x)=kxF(x) = kx(k>0k > 0),将弹簧从自然长度拉伸 aa 到 2a2a,求所做的功。

解:

W=∫a2akx dx=k2[x2]a2a=k2(4a2−a2)=3ka22W = \int_a^{2a} kx\, dx = \frac{k}{2}[x^2]_a^{2a} = \frac{k}{2}(4a^2 - a^2) = \frac{3ka^2}{2}


例15:求半圆 x2+y2≤R2x^2 + y^2 \leq R^2(y≥0y \geq 0)绕 xx 轴旋转所得球的表面积。

解:y=R2−x2y = \sqrt{R^2 - x^2},y′=−xR2−x2y' = \frac{-x}{\sqrt{R^2-x^2}}

S=2π∫−RRy1+y′2 dx=2π∫−RRR2−x2⋅RR2−x2 dx=2π∫−RRR dx=4πR2S = 2\pi \int_{-R}^{R} y\sqrt{1+y'^2}\, dx = 2\pi \int_{-R}^{R} \sqrt{R^2-x^2} \cdot \frac{R}{\sqrt{R^2-x^2}}\, dx = 2\pi \int_{-R}^{R} R\, dx = 4\pi R^2