Exam 14: Integral Transform Method

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Consider the problem of a vibrating string, tightly-stretched between x=0x = 0 and x=1x = 1 , with a fixed initial position, f(x)f ( x ) , and zero initial velocity. The mathematical problem for the deflection, u(x,t)u ( x , t ) , is ( with u(0,t)=0,u(1,t)=0)( \text { with } u ( 0 , t ) = 0 , u ( 1 , t ) = 0 )

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The value of lim⁡x→∞erfc⁡(x)\lim _ { x \rightarrow \infty } \operatorname { erfc } ( x ) is

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In the previous problem, apply the Laplace transform. The resulting equation for U(x,s)=L{u(x,t)}U ( x , s ) = \mathcal { L } \{ u ( x , t ) \} is

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The Fourier integral representation of a function f is given by

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In the previous problem, the solution for U(α,t)U ( \alpha , t ) is

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The value of L{eterf⁡(t)}\mathcal { L } \left\{ \mathrm { e } ^ { t } \operatorname { erf } ( \sqrt { t } ) \right\} is

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In the previous two problems, the integral converges for x<0x < 0 to the function

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The solution of the integral equation ∫0−∞f(x)cos⁡(ax)dx=F(α)\int _ { 0 } ^ { - \infty } f ( x ) \cos ( a x ) d x = F ( \alpha ) is

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In the previous problem, apply the Laplace transform. The resulting equation for U(x,s)=L{u(x,t)}U ( x , s ) = \mathcal { L } \{ u ( x , t ) \} is

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The Fourier cosine integral of f(x)=e−x,x≥0f ( x ) = e ^ { - x } , x \geq 0 is

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The complex form of the Fourier integral of a function f is

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The value of L{erf⁡(t)}\mathcal { L } \{ \operatorname { erf } ( \sqrt { t } ) \} is

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In the three previous problems, the solution for u(x,t)u ( x , t ) is

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In the previous three problems, the solution for u(x,t)u ( x , t ) is

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In the previous problem, if F(α)=e−α, then f(x)F ( \alpha ) = e ^ { - \alpha } \text {, then } f ( x ) is

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Consider the problem of finding the temperature in a semi-infinite rod with zero initial temperature and a fixed constant temperature, u0u _ { 0 } , at x=0x = 0 . The mathematical model for this problem is

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In the previous problem, the integral converges at x=0x = 0 to the value

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The value of lim⁡x→∞erf⁡(x)\lim _ { x \rightarrow \infty } \operatorname { erf } ( x ) is

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In the previous problem, apply a Fourier sine transform in x. The new problem for the transform U(a,t)U ( a , t ) is

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Consider the temperature, u(x,t)u ( x , t ) , in an infinite rod (−∞<x<∞)( - \infty < x < \infty ) , with an initial temperature of f(x)=e−∣x∣f ( x ) = e ^ { - | x | } . The mathematical model for this is

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