フェルマーの最終定理の証明 (645ﾚｽ)
上下前次1-新
抽出解除 必死ﾁｪｯｶｰ(本家) (べ) 自ID ﾚｽ栞 あぼーん

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ﾘﾛｰﾄﾞ規制です｡10分ほどで解除するので､他のﾌﾞﾗｳｻﾞへ避難してください｡

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591: 08/07(木)04:29 ID:jDc0ZGtb(1/9) AAS
∫_α^β??(x-α)^m (β-x)^n ? dx=m!n!/(m+n+1)! (β-α)^(m+n+1)
t=(β-α)x+α dt=(β-α)dx dx=dt/(β-α)
x:0→1 t:α→β
x=(t-α)/(β-α) 1-x=(β-α-(t-α))/(β-α)=(β-t)/(β-α)
∫_0^1?x^m (1-x)^n dx
=∫_α^β??((t-α)/(β-α))^m ((β-t)/(β-α))^n ? dt/(β-α)=∫_α^β?((t-α)^m (β-t)^m)/(β-α)^(m+n+1) dt
=1/(β-α)^(m+n+1) ∫_α^β??(t-α)^m (β-t)^m ? dt=m!n!/(m+n+1)!
∴∫_α^β??(x-α)^m (β-x)^n ? dx=m!n!/(m+n+1)! (β-α)^(m+n+1)

m=1,n=1⇒∫_α^β?(x-α)(x-β) dx=-∫_α^β?(x-α)(β-x) dx
=-1/6 (β-α)^3
m=2,n=1⇒∫_α^β?(x-α)(x-β) dx=-∫_α^β??(x-α)^2 (β-x) ? dx
=-1/12 (β-α)^4
m=2,n=2⇒∫_α^β??(x-α)^2 (x-β)^2 ? dx=∫_α^β??(x-α)^2 (β-x)^2 ? dx
=(2?2)/(5?4?3?2?1) (β-α)^5=1/30 (β-α)^5

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592: 08/07(木)04:30 ID:jDc0ZGtb(2/9) AAS
M(θ)=E[e^θX ]=∫_(-∞)^∞??e^θx f(x)dx?
M(θ)=E[e^θX ]=1/(√2π σ) ∫_(-∞)^∞??e^θx e^(-(x-μ)^2/(2σ^2 )) ? dx=1/(√2π σ) ∫_(-∞)^∞?e^(θx-(x-μ)^2/(2σ^2 )) dx
θx-(x-μ)^2/(2σ^2 )=1/(2σ^2 ) (2σ^2 θx-(x-μ)^2 )=-1/(2σ^2 ) (? (x-μ)?^2-2σ^2 θx )
=-1/(2σ^2 ) (? x?^2+μ^2-2μx-2σ^2 θx )
=-1/(2σ^2 ) (? x?^2-2(μ+σ^2 θ)x+μ^2 )
=-1/(2σ^2 ) ((x-(μ+σ^2 θ))^2-(μ+σ^2 θ)^2+μ^2 )
=-1/(2σ^2 ) ((x-(μ+σ^2 θ))^2-(μ^2+2μσ^2 θ+σ^4 θ^2 )+μ^2 )
=-1/(2σ^2 ) ((x-(μ+σ^2 θ))^2-(2μσ^2 θ+σ^4 θ^2 ) )
=-(x-(μ+σ^2 θ))^2/(2σ^2 )+μθ+(σ^2 θ^2)/2
M(θ)=1/(√2π σ) ∫_(-∞)^∞?e^(θx-(x-μ)^2/(2σ^2 )) dx
=1/(√2π σ) ∫_(-∞)^∞?e^((-(x-(μ+σ^2 θ))^2/(2σ^2 )+μθ+(σ^2 θ^2)/2) ) dx
=1/(√2π σ) e^(μθ+(σ^2 θ^2)/2) ∫_(-∞)^∞?e^((-(x-(μ+σ^2 θ))^2/(2σ^2 )) ) dx
t=(x-(μ+σ^2 θ))/(√2 σ) x=√2 σt+μ+σ^2 θ dx=√2 σdt
(x-(μ+σ^2 θ))^2/(2σ^2 )=((x-(μ+σ^2 θ))/(√2 σ))^2=t^2
-∞<x?∞ ⇒-∞<t?∞

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593: 08/07(木)04:30 ID:jDc0ZGtb(3/9) AAS
y''+6y'+10y=2sin(x).
D^2+6D+10=0. D=-3±i
(D^2+6D+10)y=2sin(x)
(D-(-3+i))(D-(-3-i))y=i(e^(-ix)-e^ix)
y=1/(D-(-3+i))∙1/(D-(-3-i)) i(e^(-ix)-e^ix)
a=-3+i, b = -3-i, f(x)=i(e^(-ix)-e^ix)
と置くと
y=1/(D-a)∙1/(D-b) f(x)=1/(D-b)∙1/(D-a) f(x)
=1/(D-b) e^ax 1/D e^(-ax) f(x)=1/(D-b) e^ax ∫▒〖e^(-ax) f(x)〗 dx
=e^bx 1/D e^(-bx) e^ax ∫▒〖e^(-ax) f(x)〗 dx
=e^bx 1/D e^(a-b)x ∫▒〖e^(-ax) f(x)〗 dx
=e^bx ∫▒(e^(a-b)x ∫▒〖e^(-ax) f(x)〗 dx) dx
=e^(-(3+i)x) ∫▒(e^2ix ∫▒〖e^((3-i)x) i(e^(-ix)-e^ix)〗 dx) dx
=e^(-(3+i)x) ∫▒(〖ie〗^2ix ∫▒〖e^((3-2i)x)-e^3x 〗 dx) dx
=e^(-(3+i)x) i∫▒e^2ix (e^((3-2i)x)/(3-2i)-e^3x/3+A)dx
=e^(-(3+i)x) i∫▒〖e^3x/(3-2i)-e^((3+2i)x)/3+A〗 e^2ix dx
=e^(-(3+i)x) (〖ie〗^3x/(3(3-2i))-〖ie〗^((3+2i)x)/(3(3+2i))+A (i2e^2ix)/2i+B)
=e^(-ix) e^(-3x) ((ie^3x)/(3(3-2i))-(〖ie〗^2ix e^3x)/(3(3+2i))+Ae^2ix+B)
=e^(-ix) (i/(3(3-2i))-〖ie〗^2ix/(3(3+2i))+Ae^((2i-3)x)+Be^(-3x) )
=(ie^(-ix))/(3(3-2i))-(ie^ix)/(3(3+2i))+Ae^((i-3)x)+Be^(-(3+i)x)
=i (3+2i)/3∙(cosx-isinx)/13-i (3-2i)/3∙(cosx+isinx)/13+e^(-3x) (Ae^ix+Be^(-ix))
=i (4icosx-6isinx)/39+e^(-3x) (Acosx+iAsinx+Bcosx-iBsinx)
=(-4cosx+6sinx)/39+e^(-3x) ((A+B)cosx+i(A-B)sinx)
=2sinx/13-4cosx/39+e^(-3x) (C_1 cosx+C_2 sinx)

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603: 08/07(木)11:23 ID:jDc0ZGtb(4/9) AAS
∫_0^∞?(sin(x))/x dx
∂/∂s (e^(-sx) (sin(x))/x)=-xe^(-sx) (sin(x))/x=-e^(-sx) sin(x)

F(s)=∫_0^∞??e^(-sx) (sin(x))/x? dx (s?0)

dF(s)/ds=d/ds ∫_0^∞??e^(-sx) sin?(x)/x? dx
=∫_0^∞??∂/ds e^(-sx) sin?(x)/x? dx
=∫_0^∞??-xe^(-sx) sin?(x)/x? dx=-∫_0^∞??e^(-sx) sin?(x) ? dx
=-∫_0^∞??-1/s (e^(-sx) )^' sin(x)? dx
=∫_0^∞??1/s (e^(-sx) )^' sin(x)? dx
=[1/s e^(-sx) sin(x)]_0^∞-1/s ∫_0^∞??e^(-sx) cos(x)? dx
=0-1/s ∫_0^∞??e^(-sx) cos(x)? dx=-1/s ∫_0^∞???-1/s (e^(-sx) )?^' cos(x)? dx
=1/s^2 ∫_0^∞??(e^(-sx) )^' cos(x)? dx
=[1/s^2 e^(-sx) cos(x)]_0^∞-1/s^2 ∫_0^∞??-e^(-sx) sin(x)? dx
=-1/s^2 +1/s^2 ∫_0^∞??e^(-sx) sin(x)? dx
=-1/s^2 -1/s^2 dF(s)/ds (dF(s)/ds=-∫_0^∞??e^(-sx) sin?(x) ? dx)

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604: 08/07(木)11:23 ID:jDc0ZGtb(5/9) AAS
E(t)=Ri(t)+1/C ∫?i(t) dt
i(t)=dq(t)/dt ∫?dq(t)/dt dt=q(t)
E(t)=R dq(t)/dt+q(t)/C
L[Rq^' ]=RsQ(s)-Rq(0)=RsQ(s)
L[q(t)/C]=Q(s)/C L[E]=E/s
E/s=RsQ(s)+Q(s)/C=Q(s)(Rs+1/C)
Q(s)= E/s 1/(Rs+1/C)=E/s(Rs+1/C) =(E/R)/s(s+1/CR) =E/R 1/s(s+1/CR)
1/s(s+1/CR) =A/s+B/(s+1/CR) 1=A(s+1/CR)+Bs
s=0⇒A/CR=1 A=CR
s=-1/CR⇒-B 1/CR=1 B=-CR
Q(s)=E/R (A/s+B/(s+1/CR))=E/R (CR/s-CR/(s+1/CR))=CE/s-CE/(s+1/CR)
L^(-1) [CE/s-CE/(s+1/CR)]=CE(L^(-1) [1/s-1/(s+1/CR)])=CE(1-e^(-1/CR t) )

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605: 08/07(木)11:26 ID:jDc0ZGtb(6/9) AA×

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606: 08/07(木)11:29 ID:jDc0ZGtb(7/9) AA×

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610: 08/07(木)21:57 ID:jDc0ZGtb(8/9) AAS
x ?+ax ?+bx=0 ???
λ^2+aλ+b=0
λ=α, β ⇒ x= C_1 e^αt+C_2 e^βt
λ=α (重解) ⇒ x= C_1 e^αt+C_2 te^βt
λ=α±βi ⇒ x= e^αt (C_1 cos?(βt)+C_2 cos?(βt))
λ^2-μ=0
0^2-4(-μ)=4μ
(?@)μ>0のときλ=±√μなので
X= C_1 e^(√μ x)+C_2 e^(-√μ x)
X^'= C_1 √μ e^(√μ x)-C_2 √μ e^(-√μ x)
境界条件 u_x (0,t)=u_x (1,t)=0より
u_x (0,t)=X^' (0)= C_1 √μ e^0-C_2 √μ e^0=(C_1-C_2 ) √μ=0
μ>0なので
C_1-C_2=0 C_1=C_2
u_x (1,t)=X^' (1)= C_1 √μ e^√μ-C_2 √μ e^(-√μ)=(C_1 e^√μ-C_2 e^(-√μ) ) √μ=0
C_1=C_2なので
(C_1 e^√μ-C_1 e^(-√μ) ) √μ= C_1 (e^√μ-e^(-√μ) ) √μ=0
μ>0、e^√μ-e^(-√μ)≠0なのでC_1=C_2=0
（※e^√μ=e^(-√μ)となるのはμ=0のときだけ）
X(x)=0 ∴u(x,t)=X(x)T(t)=0
(?A)μ=0のとき重解なので
X= C_1 e^0x+C_2 xe^0x=C_1+C_2 x
境界条件 u_x (0,t)=u_x (1,t)=0より
X^' (0)=X^' (1)= C_2=0
X=C_1

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611: 08/07(木)21:58 ID:jDc0ZGtb(9/9) AAS
E(t)=Ri(t)+1/C ∫?i(t) dt
i(t)=dq(t)/dt ∫?dq(t)/dt dt=q(t)
E(t)=R dq(t)/dt+q(t)/C
L[Rq^' ]=RsQ(s)-Rq(0)=RsQ(s)
L[q(t)/C]=Q(s)/C L[E]=E/s
E/s=RsQ(s)+Q(s)/C=Q(s)(Rs+1/C)
Q(s)= E/s 1/(Rs+1/C)=E/s(Rs+1/C) =(E/R)/s(s+1/CR) =E/R 1/s(s+1/CR)
1/s(s+1/CR) =A/s+B/(s+1/CR) 1=A(s+1/CR)+Bs
s=0⇒A/CR=1 A=CR
s=-1/CR⇒-B 1/CR=1 B=-CR
Q(s)=E/R (A/s+B/(s+1/CR))=E/R (CR/s-CR/(s+1/CR))=CE/s-CE/(s+1/CR)
L^(-1) [CE/s-CE/(s+1/CR)]=CE(L^(-1) [1/s-1/(s+1/CR)])=CE(1-e^(-1/CR t) )

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