Question #67205

Show that the function
i) 3 u(x, t) = A(x + ct)³ is a solution of the one-dimensional wave equation
ii) u( x, t) =exp(-ut) sin x , is a solution of the one-dimensional heat equation

Expert's answer

Answer on Question #67205 – Math – Differential Equations

Question

Show that the function

i) u(x,t)=A(x+ct)3u(x, t) = A(x + ct)^3 is a solution of the one-dimensional wave equation

ii) u(x,t)=exp(ut)sinxu(x, t) = \exp(-ut)\sin x is a solution of the one-dimensional heat equation

Solution

i)

One-dimensional wave equation is


2u(x,t)t2=c22u(x,t)x2\frac{\partial^2 u(x, t)}{\partial t^2} = c^2 \frac{\partial^2 u(x, t)}{\partial x^2}


To show that the function


u(x,t)=A(x+ct)3u(x, t) = A(x + ct)^3


is a solution of the one-dimensional wave equation we first find 2u(x,t)t2\frac{\partial^2 u(x,t)}{\partial t^2} and 2u(x,t)x2\frac{\partial^2 u(x,t)}{\partial x^2} for the given function:


u(x,t)t=t[A(x+ct)3]=3Ac(x+ct)2\frac{\partial u(x, t)}{\partial t} = \frac{\partial}{\partial t} [A(x + ct)^3] = 3Ac(x + ct)^22u(x,t)t2=t[3Ac(x+ct)2]=6Ac2(x+ct)\frac{\partial^2 u(x, t)}{\partial t^2} = \frac{\partial}{\partial t} [3Ac(x + ct)^2] = 6Ac^2(x + ct)u(x,t)x=x[A(x+ct)3]=3A(x+ct)2\frac{\partial u(x, t)}{\partial x} = \frac{\partial}{\partial x} [A(x + ct)^3] = 3A(x + ct)^22u(x,t)x2=x[3A(x+ct)2]=6A(x+ct)\frac{\partial^2 u(x, t)}{\partial x^2} = \frac{\partial}{\partial x} [3A(x + ct)^2] = 6A(x + ct)


Substituting the obtained values into the one-dimensional wave equation one gets the identity


6Ac2(x+ct)=c26A(x+ct)6Ac^2(x + ct) = c^2 6A(x + ct)


Thus, the function u(x,t)=A(x+ct)3u(x,t) = A(x + ct)^3 is a solution of the one-dimensional wave equation.

ii)

One-dimensional heat equation is


u(x,t)t=u2u(x,t)x2,\frac {\partial u (x , t)}{\partial t} = u \frac {\partial^ {2} u (x , t)}{\partial x ^ {2}},


where u(x,t)u(x,t) is the function, uu is the constant.

To show that given function is a solution of the one-dimensional heat equation we first find u(x,t)t\frac{\partial u(x,t)}{\partial t} and 2u(x,t)x2\frac{\partial^2 u(x,t)}{\partial x^2} for the given function


u(x,t)t=t[exp(ut)sinx]=uexp(ut)sinx\frac {\partial u (x , t)}{\partial t} = \frac {\partial}{\partial t} [ \exp (- u t) \sin x ] = - u \exp (- u t) \sin xu(x,t)x=x[exp(ut)sinx]=exp(ut)cosx\frac {\partial u (x , t)}{\partial x} = \frac {\partial}{\partial x} [ \exp (- u t) \sin x ] = \exp (- u t) \cos x2u(x,t)x2=x[exp(ut)cosx]=exp(ut)sinx\frac {\partial^ {2} u (x , t)}{\partial x ^ {2}} = \frac {\partial}{\partial x} [ \exp (- u t) \cos x ] = - \exp (- u t) \sin x


Substituting the obtained values into the one-dimensional heat equation one gets the identity


uexp(ut)sinx=uexp(ut)sinx- u \exp (- u t) \sin x = - u \exp (- u t) \sin x


Thus, the function u(x,t)=exp(ut)sinxu(x,t) = \exp(-ut)\sin x is a solution of the one-dimensional heat equation.

Answer:

i) u(x,t)=A(x+ct)3u(x, t) = A(x + ct)^3 is a solution of the one-dimensional wave equation;

ii) u(x,t)=exp(ut)sinxu(x, t) = \exp(-ut)\sin x is a solution of the one-dimensional heat equation.

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