本章主要介绍了多维随机变量及其分布的相关计算。
目录
- 习题三
- 28.设X , Y X,YX,Y是相互独立的随机变量,它们都服从正态分布N ( 0 , σ 2 ) N(0,\sigma^2)N(0,σ2)。试验证随机变量Z = X 2 + Y 2 Z=\sqrt{X^2+Y^2}Z=X2+Y2的概率密度为f Z ( z ) = { z σ 2 e − z 2 / ( 2 σ 2 ) , z ⩾ 0 , 0 , 其他 . f_Z(z)=\begin{cases}\cfrac{z}{\sigma^2}e^{-z^2/(2\sigma^2)},&z\geqslant0,\\0,&\text{其他}.\end{cases}fZ(z)=⎩⎨⎧σ2ze−z2/(2σ2),0,z⩾0,其他.我们称Z ZZ服从参数为σ ( σ > 0 ) \sigma(\sigma>0)σ(σ>0)的`瑞利分布`。
- 34.设X , Y X,YX,Y是相互独立的随机变量,X ∼ π ( λ 1 ) , Y ∼ π ( λ 2 ) X\sim\pi(\lambda_1),Y\sim\pi(\lambda_2)X∼π(λ1),Y∼π(λ2)。证明Z = X + Y ∼ π ( λ 1 + λ 2 ) . Z=X+Y\sim\pi(\lambda_1+\lambda_2).Z=X+Y∼π(λ1+λ2).
- 写在最后
习题三
28.设X , Y X,YX,Y是相互独立的随机变量,它们都服从正态分布N ( 0 , σ 2 ) N(0,\sigma^2)N(0,σ2)。试验证随机变量Z = X 2 + Y 2 Z=\sqrt{X^2+Y^2}Z=X2+Y2的概率密度为f Z ( z ) = { z σ 2 e − z 2 / ( 2 σ 2 ) , z ⩾ 0 , 0 , 其他 . f_Z(z)=\begin{cases}\cfrac{z}{\sigma^2}e^{-z^2/(2\sigma^2)},&z\geqslant0,\\0,&\text{其他}.\end{cases}fZ(z)=⎩⎨⎧σ2ze−z2/(2σ2),0,z⩾0,其他.我们称Z ZZ服从参数为σ ( σ > 0 ) \sigma(\sigma>0)σ(σ>0)的瑞利分布。
证 由于Z = X 2 + Y 2 ⩾ 0 Z=\sqrt{X^2+Y^2}\geqslant0Z=X2+Y2⩾0,知当z < 0 z<0z<0时,F Z ( z ) = 0 F_Z(z)=0FZ(z)=0。当z ⩾ 0 z\geqslant0z⩾0时有
F Z ( z ) = p { Z ⩽ z } = P { X 2 + Y 2 ⩽ z } = P { X 2 + Y 2 ⩽ z 2 } = ∬ x 2 + y 2 ⩽ z 2 f ( x , y ) d x d y = ∬ x 2 + y 2 ⩽ z 2 1 2 π σ 2 e − ( x 2 + y 2 ) / ( 2 σ 2 ) d x d y = 用极坐标 ∫ 0 2 π d θ ∫ 0 z 1 2 π σ 2 e − r 2 / ( 2 σ 2 ) d r = 2 π ⋅ 1 2 π [ − e − r 2 / ( 2 σ 2 ) ] ∣ 0 z = 1 − e − z 2 / ( 2 σ 2 ) . \begin{aligned} F_Z(z)&=p\{Z\leqslant z\}=P\{\sqrt{X^2+Y^2}\leqslant z\}\\ &=P\{X^2+Y^2\leqslant z^2\}=\displaystyle\iint\limits_{x^2+y^2\leqslant z^2}f(x,y)\mathrm{d}x\mathrm{d}y\\ &=\displaystyle\iint\limits_{x^2+y^2\leqslant z^2}\cfrac{1}{2\pi\sigma^2}e^{-(x^2+y^2)/(2\sigma^2)}\mathrm{d}x\mathrm{d}y\\\\ &\xlongequal{\text{用极坐标}}\displaystyle\int^{2\pi}_0\mathrm{d}\theta\displaystyle\int^z_0\cfrac{1}{2\pi\sigma^2}e^{-r^2/(2\sigma^2)}\mathrm{d}r\\ &=2\pi\cdot\cfrac{1}{2\pi}[-e^{-r^2/(2\sigma^2)}]\biggm\vert^z_0=1-e^{-z^2/(2\sigma^2)}. \end{aligned}FZ(z)=p{Z⩽z}=P{X2+Y2⩽z}=P{X2+Y2⩽z2}=x2+y2⩽z2∬f(x,y)dxdy=x2+y2⩽z2∬2πσ21e−(x2+y2)/(2σ2)dxdy用极坐标∫02πdθ∫0z2πσ21e−r2/(2σ2)dr=2π⋅2π1[−e−r2/(2σ2)]∣∣∣∣0z=1−e−z2/(2σ2).
将F Z ( z ) F_Z(z)FZ(z)关于z zz求导数,得Z ZZ的概率密度为f Z ( z ) = { z σ 2 e − z 2 / ( 2 σ 2 ) , z ⩾ 0 , 0 , 其他 . f_Z(z)=\begin{cases}\cfrac{z}{\sigma^2}e^{-z^2/(2\sigma^2)},&z\geqslant0,\\0,&\text{其他}.\end{cases}fZ(z)=⎩⎨⎧σ2ze−z2/(2σ2),0,z⩾0,其他.
(这道题主要利用了极坐标求解)
34.设X , Y X,YX,Y是相互独立的随机变量,X ∼ π ( λ 1 ) , Y ∼ π ( λ 2 ) X\sim\pi(\lambda_1),Y\sim\pi(\lambda_2)X∼π(λ1),Y∼π(λ2)。证明Z = X + Y ∼ π ( λ 1 + λ 2 ) . Z=X+Y\sim\pi(\lambda_1+\lambda_2).Z=X+Y∼π(λ1+λ2).
证 因X ∼ π ( λ 1 ) , Y ∼ π ( λ 2 ) X\sim\pi(\lambda_1),Y\sim\pi(\lambda_2)X∼π(λ1),Y∼π(λ2),故
p ( k ) = P { X = k } = λ 1 k e − λ 1 k ! , k = 0 , 1 , 2 , ⋯ , q ( k ) = P { X = k } = λ 2 k e − λ 2 k ! , k = 0 , 1 , 2 , ⋯ . p(k)=P\{X=k\}=\cfrac{\lambda_1^{k}e^{-\lambda_1}}{k!},\qquad k=0,1,2,\cdots,\\ q(k)=P\{X=k\}=\cfrac{\lambda_2^{k}e^{-\lambda_2}}{k!},\qquad k=0,1,2,\cdots.p(k)=P{X=k}=k!λ1ke−λ1,k=0,1,2,⋯,q(k)=P{X=k}=k!λ2ke−λ2,k=0,1,2,⋯.
而Z = X + Y Z=X+YZ=X+Y可能取的值为0 , 1 , 2 , ⋯ , 0,1,2,\cdots,0,1,2,⋯,,且X , Y X,YX,Y相互独立。由此可得
P { Z = i } = ∑ k = 0 i λ 1 k λ 2 i − k k ! ( i − k ) ! e − ( λ 1 + λ 2 ) = e − ( λ 1 + λ 2 ) i ! ∑ k = 0 i i ! k ! ( i − k ) ! λ 1 k λ 2 i − k = e − ( λ 1 + λ 2 ) i ! ∑ k = 0 i ( i k ) λ 1 k λ 2 i − k = e − ( λ 1 + λ 2 ) i ! ( λ 1 + λ 2 ) i = ( λ 1 + λ 2 ) i e − ( λ 1 + λ 2 ) i ! , i = 0 , 1 , 2 , ⋯ . \begin{aligned} P\{Z=i\}&=\sum^i\limits_{k=0}\cfrac{\lambda_1^k\lambda_2^{i-k}}{k!(i-k)!}e^{-(\lambda_1+\lambda_2)}\\ &=\cfrac{e^{-(\lambda_1+\lambda_2)}}{i!}\sum^i\limits_{k=0}\cfrac{i!}{k!(i-k)!}\lambda_1^k\lambda_2^{i-k}\\ &=\cfrac{e^{-(\lambda_1+\lambda_2)}}{i!}\sum^i\limits_{k=0}\begin{pmatrix}i\\k\end{pmatrix}\lambda_1^k\lambda_2^{i-k}=\cfrac{e^{-(\lambda_1+\lambda_2)}}{i!}(\lambda_1+\lambda_2)^i\\ &=\cfrac{(\lambda_1+\lambda_2)^ie^{-(\lambda_1+\lambda_2)}}{i!},\qquad i=0,1,2,\cdots. \end{aligned}P{Z=i}=k=0∑ik!(i−k)!λ1kλ2i−ke−(λ1+λ2)=i!e−(λ1+λ2)k=0∑ik!(i−k)!i!λ1kλ2i−k=i!e−(λ1+λ2)k=0∑i(ik)λ1kλ2i−k=i!e−(λ1+λ2)(λ1+λ2)i=i!(λ1+λ2)ie−(λ1+λ2),i=0,1,2,⋯.
即Z ∼ π ( λ 1 + λ 2 ) Z\sim\pi(\lambda_1+\lambda_2)Z∼π(λ1+λ2)。(这道题主要利用了二项式的展开求解)
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