Finding u(x) for the 1-D Heat Equation

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SUMMARY

The discussion focuses on solving the 1-D heat equation under steady-state conditions, specifically with the equation u_t = ku_xx + F(x), where F(x) = sin(x) and k = 2. The user seeks to find the function u(x) given boundary conditions u(0) = u'(0) and u(L) = 1. The solution involves finding both a particular solution and a homogeneous solution, with the general solution expressed as u(x) = c1cos(x) + c2sin(x), where c2 = c1. The final step requires determining the constant c1 to satisfy the boundary condition u(L) = 1.

PREREQUISITES
  • Understanding of the 1-D heat equation and its steady-state form
  • Knowledge of partial differential equations (PDEs) and boundary value problems
  • Familiarity with trigonometric functions and their properties
  • Experience with solving ordinary differential equations (ODEs)
NEXT STEPS
  • Study methods for solving boundary value problems in PDEs
  • Learn about particular and homogeneous solutions in the context of ODEs
  • Explore the use of Fourier series for solving heat equations
  • Investigate the application of the method of separation of variables in PDEs
USEFUL FOR

Mathematicians, physics students, and engineers working on heat transfer problems or studying differential equations, particularly those interested in boundary value problems and steady-state solutions.

clope023
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Homework Statement



If there is heat radiation in a rod of length L, then the 1-D heat equation might take the form:

u_t = ku_xx + F(x,t)

exercise deals with the steady state condition => temperature u and F are independent of time t and that u_t = 0.

u_t = partial derivative with respect to t
u_xx = 2nd partial derivative with respect to x

Problem: find u(x) if F(x) = sinx, k = 2, u(0) = u'(0), u(L) = 1

Homework Equations




e^(itheta) = cos(theta) + isin(theta)
e^(-itheta) = cos(theta) - isin(theta)
e^(itheta) + e^(-itheta) = 2cos(theta)
e^(itheta) - e^(-itheta) = 2isin(theta)

The Attempt at a Solution



u_t = ku_xx + F(x,t)
u_t = ku_xx + F(x)G(t)
2u_xx + sin(x)G(t) = 0
characteristic equation: m^2+1=0, m^2 = -1, m = +-i
general soltn: u(x) = c1cos(x) + c2sin(x)
u(0) = c1cos(0) + c2sin(0)
u'(x) = -c1sin(x) + c2cos(x)
u'(0) = -c1sin(0) + c2cos(0)
=> c2 = c1
u(x) = c1cos(x) + c1sin(x)
u(L) = c1cos(L) + c1sin(L) = 1

from here I'm actually a little lost, I'm not sure what to do with u(L) = 1 portion; do I perhaps need to find a particular solution? any help would be appreciated.
 
Physics news on Phys.org
If everything is time independent then it's really just an ODE with boundary conditions, right? Yes, find a particular solution. Then find a homogeneous solution and adjust the constants to fit the boundary conditions.
 

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