Heat diffusion equation solutions for semi-infinite slab

Click For Summary
SUMMARY

The discussion focuses on solving the heat diffusion equation for a semi-infinite slab, specifically addressing the application of boundary conditions that lead to complex numbers in the solution. The user struggled with the mathematical approach, trying various functions including exponentials and hyperbolic functions. A suggested solution involves substituting the cosine function with a complex exponential form, specifically using q(0)R(e^iwt) to simplify the boundary condition application. This method is referenced from the textbook "Transport Phenomena" by Bird, Stewart, and Lightfoot.

PREREQUISITES
  • Understanding of the heat diffusion equation
  • Familiarity with boundary conditions in differential equations
  • Knowledge of complex numbers and their physical interpretations
  • Experience with mathematical functions such as exponentials and hyperbolic functions
NEXT STEPS
  • Study the heat diffusion equation in detail, focusing on boundary conditions
  • Learn about complex analysis and its applications in physical problems
  • Explore the use of Fourier series in solving differential equations
  • Read "Transport Phenomena" by Bird, Stewart, and Lightfoot for practical examples
USEFUL FOR

Students and professionals in engineering, particularly those studying heat transfer, as well as anyone involved in solving differential equations related to physical phenomena.

Hipp0
Messages
11
Reaction score
0

Homework Statement



http://img42.imageshack.us/img42/1082/clipboard01lx.jpg

Homework Equations



(see solution)

The Attempt at a Solution



I literary just spent 5 hours trying to apply those boundary conditions, trying exponentials, sines, cosines, hyperbolic function etc... I always get complex numbers in the final solution :( but it's not physical to get complex numbers there :(
Note: Aw and Bw are just constants (w is an index).

http://img189.imageshack.us/img189/4475/94889151.jpg
Any ideas where I went wrong? General solution seems fine, maybe I'm misunderstanding the boundary conditions? And in my final answer I tried expanding \sqrt{i}=\frac{1}{\sqrt{2}}+\frac{1}{\sqrt{2}}i and then using cos(A+B) formula and writing the result using hyperbolic sines and cosines, but it's still complex :(
Thanks
 
Last edited by a moderator:
Physics news on Phys.org
Hello,

Perhaps a substitution for cos(wt) (allow w = omega)

So now you have q = q(0) cos(wt) at the boundary, where q(0) is the amplitude of the heat flux and omega is the circular frequency.

Substitute q(0)R(e^iwt) where R = the real part for the original equation of q(0) = cos(wt).

I worked this problem out as it is given in Transport Phenomena by Bird Stewart and Lightfoot and they suggested this substitution. (Actually it is given as an example, but quite a few steps are missing.)

If you have already done that and I have overlooked it in your somewhat hard to follow layout above, I apologize.

I will have to dig my notes out on this one later this evening to really provide you with some help.

Thanks
Matt
 
Last edited:

Similar threads

Replies
13
Views
3K
Replies
2
Views
2K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 7 ·
Replies
7
Views
3K
Replies
0
Views
1K
Replies
7
Views
2K
  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 2 ·
Replies
2
Views
3K