u = X ( x ) ∗ T ( t ) T ′ β T = X ′ X = c o n s t = − λ X ′ ′ + λ X = 0 X ( x ) = C 1 cos ( λ x ) + C 2 sin ( λ x ) X ( 0 ) = C 1 ∗ 1 + C 2 ∗ 0 = C 1 = 0 = > X ( x ) = sin ( λ x ) X ( L ) = sin ( λ L ) = 0 λ L = π ∗ k = > λ = ( π ∗ k L ) 2 X ( x ) = sin ( λ x ) , T ( t ) = C ∗ e − β λ t , λ = ( π ∗ k L ) 2 = > W e k n o w t h a t : u = X ( x ) ∗ T ( t ) , s o u ( x , t ) = ∑ k = 0 C ∗ e − β λ t ∗ sin ( λ x ) , w h e r e C = 2 L ∫ 0 L f ( x ) ∗ sin ( λ x ) d x , i s c o e f f i c i e n t o f a F o u r i e r s e r i e s λ = ( π ∗ k L ) 2 u=X(x)*T(t)\\
\dfrac{T'}{\beta T}=\dfrac{X'}{X}=const=-\lambda\\
X''+\lambda X=0\\
X(x)=C_1\cos(\sqrt{\lambda}x)+C_2\sin(\sqrt{\lambda}x)\\
X(0)=C_1*1+C_2*0=C_1=0=>X(x)=\sin(\sqrt{\lambda}x)\\
X(L)=\sin(\sqrt{\lambda}L)=0\\
\sqrt{\lambda}L=\pi *k=>\lambda=(\dfrac{\pi *k}{L})^2\\
X(x)=\sin(\sqrt{\lambda}x),\\
T(t)=C*e^{-\beta\lambda t},
\lambda=(\dfrac{\pi *k}{L})^2=>\\
We \space know \space that \space:u=X(x)*T(t), \space so\\
u(x,t)=\underset{k=0}{\sum}C*e^{-\beta\lambda t}*\sin(\sqrt{\lambda}x),\\
where\\
C=\dfrac{2}{L}\overset{L}{\underset{0}{\int}}f(x)*\sin(\sqrt{\lambda}x)dx,is \space coefficient \space of \space a \space Fourier \space series\\
\lambda=(\dfrac{\pi *k}{L})^2 u = X ( x ) ∗ T ( t ) βT T ′ = X X ′ = co n s t = − λ X ′′ + λ X = 0 X ( x ) = C 1 cos ( λ x ) + C 2 sin ( λ x ) X ( 0 ) = C 1 ∗ 1 + C 2 ∗ 0 = C 1 = 0 => X ( x ) = sin ( λ x ) X ( L ) = sin ( λ L ) = 0 λ L = π ∗ k => λ = ( L π ∗ k ) 2 X ( x ) = sin ( λ x ) , T ( t ) = C ∗ e − β λ t , λ = ( L π ∗ k ) 2 => W e kn o w t ha t : u = X ( x ) ∗ T ( t ) , so u ( x , t ) = k = 0 ∑ C ∗ e − β λ t ∗ sin ( λ x ) , w h ere C = L 2 0 ∫ L f ( x ) ∗ sin ( λ x ) d x , i s coe ff i c i e n t o f a F o u r i er ser i es λ = ( L π ∗ k ) 2
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