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心得

随想

∬Rf(x,y) dx dy=∬Sf(aRcos⁡(θ),bRsin⁡(θ))∣∂(x,y)∂(R,θ)∣ dR dθ=∬Sf(aRcos⁡(θ),bRsin⁡(θ))∣∣∂x∂R∂x∂θ∂y∂R∂y∂θ∣∣ dR dθ=∬Sf(aRcos⁡(θ),bRsin⁡(θ))∣∣acos⁡(θ)−aRsin⁡(θ)bsin⁡(θ)bRcos⁡(θ)∣∣ dR dθ=∬Sf(aRcos⁡(θ),bRsin⁡(θ))∣(acos⁡(θ))(bRcos⁡(θ))−(−aRsin⁡(θ))(bsin⁡(θ))∣ dR dθ=∬Sf(aRcos⁡(θ),bRsin⁡(θ))∣abRcos⁡2(θ)+abRsin⁡2(θ)∣ dR dθ=∬Sf(aRcos⁡(θ),bRsin⁡(θ))∣abR(cos⁡2(θ)+sin⁡2(θ))∣ dR dθ=∬Sf(aRcos⁡(θ),bRsin⁡(θ))abR dR dθ(假设 a,b,R≥0)\begin{aligned} \iint_R f(x,y)\,\mathrm{d} x\,\mathrm{d} y &= \iint_S f(aR\cos(\theta),bR\sin(\theta))\left|\frac{\partial(x,y)}{\partial(R,\theta)}\right|\,\mathrm{d} R\,\mathrm{d} \theta \\ &= \iint_S f(aR\cos(\theta),bR\sin(\theta))\left| \begin{vmatrix} \frac{\partial x}{\partial R} & \frac{\partial x}{\partial \theta} \\ \frac{\partial y}{\partial R} & \frac{\partial y}{\partial \theta} \end{vmatrix} \right|\,\mathrm{d} R\,\mathrm{d} \theta \\ &= \iint_S f(aR\cos(\theta),bR\sin(\theta))\left| \begin{vmatrix} a\cos(\theta) & -aR\sin(\theta) \\ b\sin(\theta) & bR\cos(\theta) \end{vmatrix} \right|\,\mathrm{d} R\,\mathrm{d} \theta \\ &= \iint_S f(aR\cos(\theta),bR\sin(\theta))\left| (a\cos(\theta))(bR\cos(\theta)) - (-aR\sin(\theta))(b\sin(\theta)) \right|\,\mathrm{d} R\,\mathrm{d} \theta \\ &= \iint_S f(aR\cos(\theta),bR\sin(\theta))\left| abR\cos^2(\theta) + abR\sin^2(\theta) \right|\,\mathrm{d} R\,\mathrm{d} \theta \\ &= \iint_S f(aR\cos(\theta),bR\sin(\theta))\left| abR(\cos^2(\theta) + \sin^2(\theta)) \right|\,\mathrm{d} R\,\mathrm{d} \theta \\ &= \iint_S f(aR\cos(\theta),bR\sin(\theta)) abR \, \mathrm{d} R\,\mathrm{d} \theta \quad (\text{假设 } a,b,R \ge 0) \end{aligned}

这里可以理解为坐标轴改变,即假设以(θ,R\theta,R)为新坐标轴,原先的x,yx,y就变成了∂x,∂y\partial x,\partial y的新坐标,新的面积即为他们的叉乘(即二阶行列式)


当函数f(x)f(x)满足∀a≤x≤b,f(x)=f(a+b−x)\forall a\leq x \leq b,f(x)=f(a+b-x)(即积分区间内函数对称)时,有

∫abxf(x) dx=∫ab(a+b−x)f(x) dx=a+b2∫abf(x) dxe.g.∫0πxsin⁡(x) dx=π2∫0πsin⁡(x) dx\begin{aligned} \int_a^b xf(x)\,\mathrm{d} x &=\int_a^b(a+b-x)f(x)\,\mathrm{d} x\\ &=\frac{a+b}{2}\int_a^b f(x)\,\mathrm{d} x \\ \text{e.g.} \quad \int_{0}^{\pi} x\sin(x)\,\mathrm{d} x &=\frac{\pi}{2}\int_{0}^\pi \sin(x)\,\mathrm{d} x \end{aligned}