Find equilibrium profile T(x) Between Two Rods

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The discussion focuses on finding the equilibrium temperature profile T(x) between two rods in contact, governed by Laplace's equation under equilibrium conditions. The user has successfully separated the rods into halves and derived the initial equation, but is unsure about the second boundary condition needed for the solution. Clarification is sought regarding the setup, particularly the positions of boundary conditions and the physical properties of the rods, which are confirmed to have the same diameter and length of L/2. The conversation also addresses the heat flow equation, confirming that the heat flow before and after the junction is equal, and that the constant C_1 represents the total rate of heat flow Q.
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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