应用统计学课件 33页

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  • 2022-08-13 发布

应用统计学课件

  • 33页
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;%F&!2.(X1,···,Xn)(;X= f(x),F(x)cXFI!:F:=i)RnFI!:F:c∞n−2fRn(x)=n(n−1)[F(x+u)−F(u)]f(x+u)f(u)du,x>0,−∞∞n−1FRn(x)=n[F(x+u)−F(u)]f(u)du,x>0.−∞3.Z&EXF:F(x),]17\n00,c(X(n)−an)/bngquirFG(x),AG(x)i,F.L=Zi+F i,F i+FAiF?I!i,F(UAopq(Gumbel)F)−xG1(x)=exp(−e),−∞0;G2(x)=⎪⎪⎪⎪⎪⎩0,x≤0,9k>0?III!i,F(UAsFq(Weibull)F)⎧⎪⎪⎪⎪⎪⎨1,x>0;G3(x)=⎪⎪⎪⎪k⎪⎩exp(−(−x)),x≤0,9k>0?sZiF−1/ξG(x;θ)=exp[−{1+ξ(x−μ)/σ}+]θ=(μ,σ,ξ)Dσ>0,μ,ξ∈R,\]ps,{s}+=max{s,0}.AGEV(μ,σ,ξ)Rt5Æevd,evir,ismev,evdbayes,extremes2/ i?19\nhDF3F(x;θ)5?XF θ=? 4A@),AΘ,A{F(x;θ):θ∈Θ}XF:3?(1)22HF3{N(μ,σ):θ∈Θ},9Θ={(μ,σ):−∞<μ<∞,σ2>0}(2)0}(4).F3{R(a,b):−∞0}?GammaF31.Z&EX;I!:λαα−1−λxf(x:α,λ)=xe,x>0,Γ(α)AXN$FGammaF AGa(α,λ),9α>0P/λ>0k!{Ga(α,λ):α>0,λ>0}AGammaF3?2.iXtit−α(1)g4:ϕ(t)=Ee=(1−)λαα(2)E(X)=D(X)=λλ2(3)hα=1fGa(1,λ)8λ1F?20\nn122Ga(,)An(!χF Aχ(n)2221n−1−x(n)22F χFI!:f(x,n)=nnxe,x>22Γ()20(!1FE(4)=dX1∼Ga(α1,λ),X2∼Ga(α2,λ),\X1X2EGFX1+X2∼Ga(α1+α2,λ)21FExp(λ)χ(n)FGammaFguvxU;=d?1X∼Ga(α,λ),9α>0,λ>0Dn(X1,···,Xn)(;= k =i=1XiFI!:f-GammaF;=d\XiF)nF i=1Xi∼Ga(nα,λ)λ2X∼Ga(α,λ),Y=kX,0qY∼Ga(α,k),k>0 O\kX¯Ff-X∼Ga(α1,λ)BI!:λαα−1−λxf(x:α,λ)=xe,x>0,Γ(α)21\n-Y=kX,X=Y/k,X=1/k,-bλαyyα−1−λ1f(y:α,λ)=()ekΓ(α)kk(λ)αkα−1−λ=yek,Γ(α)λ∼Ga(α,)kX¯=1nni=1xi∼Ga(nα,nλ)22113X∼N(0,σ),Y=X∼Ga(,).22σ2fhy>0fYF:2√√FY(y)=P{Y≤y}=P{X≤y}=P{−y≤X≤y}√√=FX(y)−FX(−y),9FI!:√√111−y−fY(y)=[fX(y)+fX(−y)]√=√y2e2σ2,2y2πσ1√11-Γ(2)=π,-lY∼Ga(2,2σ2).23.χFyZ/`(1)2222&Xi∼N(0,1)iid,Y=X1+X2+···+Xn∼χ(n)(2)2nxi−μ22&X∼N(μ,σ),Σi=1(σ)∼χ(n)0,b>0<?{Be(a,b):a>0,b>0}ABetaF3.2.aab(1)E(X)=,D(X)=a+b(a+b)2(a+b+1)(2)ha=b=1fBe(1,1)F8(0,1)O.FR(0,1)3.22&X1∼χ(n1),X2∼χ(n2),\X1,X2EGFX1/n1(1)F=∼F(n1,n2),9F(n1,n2)5?(!X2/n2n1,n2FF?X1n1n2(2)∼Be(,)X1+X2224.zCXn1n2(1)&X∼F(n1,n2),∼Be(,)9C=1+CX22n1/n2,twx?(2)22&X1∼χ(n1),X2∼χ(n2),\X1,X2EGFY1=X1+X2Y2=X1/X2EGF?YtF1.2ZEX∼N(0,1),Y∼χ(n),\X,Y23\nXEGFAET=Y/nN$Fn(!tF AT∼t(n).2.t(n)FI!:n+1Γ()22x−n+1t(x;n)=n√(1+)2,−∞2fE(T)=0,D(T)=n−2(2)2∼F(1,n).&X∼t(n),Xnn1(3)&X∼t(n),Y=∼Be(,).n+X2221x2−(4)limn→∞t(x;n)=√e22πtFirF(HFh1!F31.ZF={f(x;θ):θ∈Θ}F3& =(X1,···,Xn)I!:(<F^)f(x1,···,xn;θ)=5?.kf(x1,···,xn;θ)=a(θ)exp{Qj(θ)Tj(x1,···,xn)}h(x1,···,xn)j=1O\Mu{x:f(x1,···,xn;θ)>0}*`θ,AlF31!F3CA1324\n1:0q0}*1!F3-Mu{x:f(x;θ)>0}=(−θ,θ)`)θ.23XN$HFN(μ,σ),=@)nn{y@)R.Ax=(x1,···,xn),%&=(X1,···,Xn)FI!1n12√n2f(x;μ,σ)=()exp{−2(xi−μ)}2πσi=12σ2n2√1nnμnμxi=()exp{−+x¯−}2σ2σ22σ22πσi=11nμ2nμ1n√n2=()exp{−2σ2}exp{σ2x¯−2xi},2πσ2σi=15zc1nμ2nμ2√n2a(μ,σ)=()exp{−2},Q1(μ,σ)=2,2πσ2σσ21n2Q2(μ,σ)=−2,T1(x)=¯x,T2(x)=xi,h(x)=12σi=125\n22-lHF3{N(μ,σ):−∞<μ<∞,σ>0}1!F3?hH;vH;1.Z&AX4FI!:11−1f(x)=n1exp{−(x−a)B(x−a)}(2π)2|B|22−19B6|B|9^`?BB|R6AAXN$FvHF,CAX∼Nn(a,B).2.g4:AX∼Nn(a,B),9g4:1ϕ(t)=exp{iat−tBt}29t=(t1,···,tn)3.pn/){/)6X=(X1,···,Xn),Y=(Y1,···,Ym)AZ=(Zij)r×s R6AE(X)=(E(X1),···,E(Xn)),E(Z)=(E(Zij))r×s,26\nD(X)=E(X−E(X))(X−E(X))⎛⎞D(X1)Cov(X1,X2)···Cov(X1,Xn)⎜⎟⎜⎟⎜⎟⎜⎟⎜⎜Cov(X2,X1)D(X2)···Cov(X2,Xn)⎟⎟⎜⎟=⎜⎟,⎜⎜.........⎟⎟⎜...⎟⎜⎟⎜⎟⎝⎠Cov(Xn,X1)Cov(Xn,X2)···D(Xn)9D(Xi)Xi/) Cov(Xi,Xj)XiXj{/)?Cov(X,Y)=(Cov(Y,X))=E(X−E(X))(Y−E(Y))⎛⎞⎜Cov(X1,Y1)···Cov(X1,Ym)⎟⎜⎟⎜⎟=⎜⎜.........⎟⎟,⎜⎟⎜⎟⎜⎟⎝⎠Cov(Xn,Y1)···Cov(Xn,Ym)4.ρ=√Cov(Xi,Xj)ijD(XAXiXj)KE10i)D(Xj)CAE10?LFnnxin−xiP{X=x,···,X=x;p}=pi=1(1−p)i=11nnnxi=(1−p)n(p)i=1,1−pnT(x1,···,xn)=xi,h(x1,···,xn)=1,i=1npTg(T(x1,···,xn),p)=(1−p)()1−pP{X=x1,···,Xn=xn;p}=h(x1,···,xn)·g(T(x1,···,xn),p),n-+f=)T(X1,···,Xn)=Xipwi=1?4X∼N(μ,1),−∞<μ<+∞)0qXμw31\n0X1,···,Xn4FI!nnf(x;θ)=(√1)nexp{−1(x−μ)2}iii=12π2i=1nn222b(xi−μ)=(xi−x)+n(x−μ)i=1i=1n1n1212`=(√)exp{−(xi−x)}exp{−n(x−μ)}2π2i=12n12h(x1,···,xn)=exp{−(xi−x)}2i=1g(T(x,···,x),μ)=(√1)nexp{−1n(x−μ)2}1n2π2-+f=)Xμw?3.&FnθAD2.FAT(X1,···,Xn)1θ4w225.X∼N(μ,σ),θ=(μ,σ))A0n22(X,Xi)(μ,σ)4w?i=10(X1,···,Xn)(;= 94I!:nL(x1,···,xn;θ)=f(xi;θ)i=1n112=√nexp{−2(xi−μ)}(2πσ)2σi=1n2112nμnμ=√nexp{−2σ2xi+σ2x−2σ2}.(2πσ)i=132\nh(x1,···,xn)=1,n2√112nμnμg(T(x1,···,xn),θ)=nexp{−2σ2xi+σ2x−2σ2}(2πσ)i=1n2-+f=)T(X1,···,Xn)=(X,Xi)θ=i=12)(μ,σ4w?T(X1,···,Xn)θ4w*?n2Tiθiw?-l*?qX,Xici=12μ,σw?33

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