Find equilibrium profile T(x) Between Two Rods

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Homework Help Overview

The discussion revolves around finding the equilibrium temperature profile T(x) between two rods in contact, focusing on the application of Laplace's equation under steady-state conditions. The problem involves boundary conditions and the physical properties of the rods, such as their thermal conductivities and dimensions.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the separation of the rod into halves and the application of boundary conditions. There are questions regarding the second boundary condition and the interpretation of the heat flow equation. Some participants seek clarification on the physical setup, including the positions of the boundary conditions and the dimensions of the rods.

Discussion Status

The discussion is ongoing, with participants exploring various interpretations of the problem and seeking clarification on specific aspects. Some guidance has been provided regarding the heat flow equation and its implications, but no consensus has been reached on the second boundary condition or the overall approach.

Contextual Notes

Participants note that both rods have the same diameter and that each rod is of length L/2. There is a lack of a diagram to illustrate the setup, which may contribute to confusion regarding the boundary conditions.

happyparticle
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Homework Statement
Find equilibrium profile T(x) Between Two Rods in contact.
##x = 0 , T= T_1##
##x = L, T=T_2##
For the first rod: ##\kappa = \kappa_1##
The second rod: ##\kappa = \kappa_2##
Relevant Equations
##\frac{\partial T}{\partial t} = \kappa \frac{\partial^2 T}{\partial x^2}##
Knowing that we are in equilibrium ##\frac{\partial}{\partial t} = 0##.

We now have a Laplace's equation ##\kappa \frac{\partial^2 T}{\partial x^2} = 0##

I separated the rod in 2 halves.

The solution of this equation is ##\kappa_1 \frac{\partial2 T}{\partial x2} = C_1##

Integrating both side we get ##\kappa_1 T = C_1 x + C_2##

The first boundary condition: ##x = 0 , T = T_1##

We now have
##\kappa_1 T = C_1 x + \kappa_1 T_1##

I'm stuck here. I can't find what is the second condition and I have the same problem with the second half of the rod.

Any help will be appreciated. I'm really stuck.

Thank you
 
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happyparticle said:
Homework Statement: Find equilibrium profile T(x) Between Two Rods in contact.
##x = 0 , T= T_1##
##x = L, T=T_2##
For the first rod: ##\kappa = \kappa_1##
The second rod: ##\kappa = \kappa_2##
Relevant Equations: ##\frac{\partial T}{\partial t} = \kappa \frac{\partial^2 T}{\partial x^2}##

Knowing that we are in equilibrium ##\frac{\partial}{\partial t} = 0##.

We now have a Laplace's equation ##\kappa \frac{\partial^2 T}{\partial x^2} = 0##

I separated the rod in 2 halves.

The solution of this equation is ##\kappa_1 \frac{\partial2 T}{\partial x2} = C_1##

Integrating both side we get ##\kappa_1 T = C_1 x + C_2##

The first boundary condition: ##x = 0 , T = T_1##

We now have
##\kappa_1 T = C_1 x + \kappa_1 T_1##

I'm stuck here. I can't find what is the second condition and I have the same problem with the second half of the rod.

Any help will be appreciated. I'm really stuck.

Thank you
How about showing a diagram that has the end conditions. Is the ##x = 0## at the meeting point, or one of the ends, or what?
 
What are the lengths of the two rods? Are their diameters the same?
 
erobz said:
How about showing a diagram that has the end conditions. Is the ##x = 0## at the meeting point, or one of the ends, or what?
##x = 0 , T = T_1## is one of the ends. I don't have any diagram.

Chestermiller said:
What are the lengths of the two rods? Are their diameters the same?
Their diameters are the same and the length of each rod is L/2.
 
happyparticle said:
##x = 0 , T = T_1## is one of the ends. I don't have any diagram.Their diameters are the same and the length of each rod is L/2.
$$Q=k_{left}A\frac{(T_1-T_m)}{L/2}=k_{right}A\frac{(T_m-T_2)}{L/2}$$where Q is the total rate of heat flow along the rod, A is the cross sectional area, and ##T_m## is the temperature at the junction between the two materials.
 
Just to be sure, does it means that the total rate of heat flow just before the junction on the right is equal to the total rate of heat flow just after the second rod. I try to figure out what that equation means. If so, is it always the case?

Secondly, Does it means that my constant ##C_1 = Q ## ?

Thank you
 
happyparticle said:
Just to be sure, does it means that the total rate of heat flow just before the junction on the right is equal to the total rate of heat flow just after the second rod. I try to figure out what that equation means. If so, is it always the case?
Sure. The heat has nowhere else to go.
happyparticle said:
Secondly, Does it means that my constant ##C_1 = Q ## ?

Thank you
Here, Q is a constant.
 
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