Question #169937

A thin, homogenous bar of length L has insulated ends and initial temperature f(x) = x. Determine the temperature distribution u(x,t) in the bar.


1
Expert's answer
2021-03-08T18:10:47-0500

We know one dimensional equation for a rod is given as,


δuδt=c2δ2uδx2\dfrac{\delta u}{\delta t} = c^2\dfrac{\delta^2 u}{\delta x^2}


It's solution can be given as u(x,t)=(C1cos(px)+C2sin(px))ec2p2tu(x,t) = (C_1cos(px) + C_2sin(px))e^{-c^2p^2t}


At x = 0 ,u(x,t)=0=u(0,t)=C1ec2p2tu(x,t) = 0 = u(0,t) = C_1e^{-c^2p^2t}


Hence, C1=0C_1 = 0


u(x,t)=C2sin(px)ec2p2tu(x,t) = C_2sin(px)e^{-c^2p^2t}


Using condition u(a,t) = 0


Hence, C2sin(px)ec2p2t=0C_2sin(px)e^{-c^2p^2t} = 0


But actually it is not equal to zero to get the desired solution


then, sin(px)=0sin(px) = 0


pa=nπpa = n\pi


Hence, p=nπap = \dfrac{n\pi}{a}

Putting the value of p in above equation, we get


u(x,t)=C2sinnπxaen2π2kta2u(x,t) = C_2sin{\dfrac{n\pi x}{a}}e^-\dfrac{n^2\pi^2kt}{a^2}


where, n = 0,1,2,3.....


u(x,t)=1bnsinnπxaen2π2kta2u(x,t) = \sum_{1}^{\infin}b_nsin{\dfrac{n\pi x}{a}}e^-{\dfrac{n^2\pi^2kt}{a^2}} .......(A)


It is given that u(x,0) = f(x)


So, f(x)=1bnsinnπxaf(x) = \sum_{1}^{\infin}b_nsin{\dfrac{n\pi x}{a}}


then bn=2a0af(x)sinnπxadxb_n = \dfrac{2}{a}\int _{0}^{a}f(x)sin{\dfrac{n\pi x}{a}}dx (Using Fourier Sine Series)


Putting this value of bnb_n in equation (A) we get the desired equation.


u(x,t)=12a0af(x)sinnπxadx(sinnπxaen2π2kta2)u(x,t) = \sum_{1}^{\infin} \dfrac{2}{a}\int _{0}^{a}f(x)sin{\dfrac{n\pi x}{a}}dx (sin{\dfrac{n\pi x}{a}}e^-{\dfrac{n^2\pi^2kt}{a^2}})






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