Finding the Steady Solution for a PDE Problem

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SUMMARY

The discussion focuses on finding the steady solution for the partial differential equation (PDE) governing heat conduction in a slender homogeneous conducting bar. The PDE is defined as u_t = α²u_xx - u, with boundary conditions u_x(0,t) = 0 and u_x(1,t) = q. The user successfully identifies the time-independent solution by setting u_t to zero, resulting in a differential equation with the general solution y = c_1e^(x/α) + c_2e^(-x/α). The user emphasizes the importance of applying boundary conditions to derive specific constants.

PREREQUISITES
  • Understanding of partial differential equations (PDEs)
  • Knowledge of boundary value problems
  • Familiarity with heat conduction principles
  • Basic differential equations and their solutions
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  • Study the method of separation of variables for solving PDEs
  • Learn about boundary conditions and their applications in heat transfer problems
  • Explore the concept of steady-state solutions in thermal systems
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Students and professionals in engineering, particularly those specializing in thermal dynamics, applied mathematics, and physics, will benefit from this discussion on solving PDEs related to heat conduction.

HalfManHalfAmazing
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I'm wondering if anyone can just run through how this is done. I have the solution so that's now the problem. I just need someone to provide me with the method of finding the steady solution (I can find the transient no problem).

A slender homogeneous conducting bar of uniform cross section lies along the x-axis with ends at x = 0 and x = 1. The lateral surface of the bar radiates heat into the surroundings at temperature zero. The left end is insulated and heat is added through the right end. The initial temperature distributions is u(x,0) = f(x).

Okay so the PDE we have here is:

u_t = \alpha^2u_{xx} - u
u_x(0,t) = 0
u_x(1,t) = q
u(x,0) = f(x)

And to find the steady solution I do the usual tricks. I know how to get it I just want someone to explain a bit. Thanks.
 
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Okay well I went ahead and did it myself. I figure I'll explain myself in case anyone wishes:

I start by finding the time indepenent solution - where u_t vanishes. I find that I have an DE similar to basic differential equations with solution - y = c_1e^{\frac{x}{\alpha}}+c_2e^{-\frac{x}{\alpha}}

I want to plug in some boundary conditions and for that I need to differentiate and then plug in.
 
Glad you were able to figure it out! :biggrin:
 

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