Solving Boundary Conditions for One-Dimensional Heat Flow Equation

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Homework Help Overview

The discussion revolves around the boundary conditions for the one-dimensional heat flow equation governing the temperature distribution in a bar. The original poster describes their progress in solving the equation but expresses difficulty in interpreting the boundary conditions related to an insulated end and the initial temperature setup.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to apply separation of variables to solve the heat equation but struggles with the implications of the boundary conditions. They question how to handle the insulated end and the initial conditions, particularly regarding the temperature at x=L.

Discussion Status

Some participants provide insights regarding the behavior of the temperature at the insulated end, noting that it will eventually reach the maximum temperature of 100 degrees at infinity. This suggests a productive direction in understanding the long-term behavior of the system.

Contextual Notes

The original poster mentions that the bar is perfectly insulated at one end and that the initial temperature is uniformly 0 degrees Celsius, raising questions about the physical implications of these conditions on the temperature evolution over time.

Tomsk
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I have done most of a question except for the most important part, putting in the boundary conditions, I can't really interpret them.

The question is:

The temperature T of a one dimensional bar whose sides are perfectly insulated obeys the heat flow equation

\frac{\partial T}{\partial t} = \kappa\frac{\partial^2 T}{\partial x^2}

where kappa is a positive constant.

I managed to solve this, with -c^2 as a separation constant, and I got:

T(x,t) = X(x)F(t) = (A_{1} \cos{\frac{cx}{\sqrt{\kappa}}} + A_{2} \sin{\frac{cx}{\sqrt{\kappa}}})e^{-c^2 t}

But then the question says,

The bar extends from x=0 to x=L and is perfectly insulated at x=L. At t<0 the temperature is 0 degC throughout the bar and at t=0 the uninsulated end is placed in contact with a heat bath at 100 degC. Show that the temperature of the bar at subsequent times is given by:

\frac{T}{100} = 1 - \sum_{n=0}^{\infty} \frac{4}{(2n + 1)\pi} \sin{\left(\frac{(2n+1)\pi x}{2L}\right)} exp{\left(-\kappa\left(\frac{(2n+1)\pi}{2L}\right)^{2} t \right)}

And I can't figure out how to get this. I got T(0,t) = 100, therefore A1 e^(-c^2 t) = 100, but that doesn't tell me much. I know I need to sum over c or n at some point, but am I right in thinking you can't sum over c yet because it's a real arbitrary constant, rather than an integer n? That would probably give you the 1 though from n=0. But the problem is with the insulated end x=L, surely if it's insulated it won't lose heat, so the temperature would just go up?
 
Last edited:
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The maximum temperature at any point is 100 degrees. The temperature at the insulated end will only reach this limit at t = infinity. So you have T(L,inf) = 100.
 
Thanks very much, that looks like it'll sort it. It's funny how its always such a little thing missing... Maybe it's just me.
 
Thanks very much, that looks like it'll sort it. It's funny how its always such a little thing missing... Maybe it's just me.
 
Thanks very much, that looks like it'll sort it. It's funny how its always such a little thing missing... Maybe it's just me.
 

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