Analyzing 2D Fin Temperature with Separation of Variables

In summary: For Y(y), we have Y''+λ^2Y=0, which also has a general solution of Y(y)=c3sin(λy)+c4cos(λy).Now, we can apply the boundary conditions to solve for the constants in the general solution. At x=0, we have X(0)=Tb, which means that c2=Tb. At x=L, we have X'(L)=0, which means that c1λcosh(λL)-c2λsinh(λL)=0. We can combine this with the previous condition to get c1λsinh(λL)+
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Homework Statement


We have a 2D fin that has length L (x-axis), and thickness t, (y-axis). The left side has a fixed temperature, the right side is insulated, and the top and bottom surfaces are subject to convection. Find an analytical solution for the temperature at steady state.

Homework Equations


Boundary Conditions:
[itex](0,y) \quad T=T_b[/itex]
[itex]\displaystyle (L,y) \quad \frac{\partial{T}}{\partial{x}}=0[/itex]
[itex]\displaystyle (x,t/2) \quad k\frac{\partial{T}}{\partial{y}}+h(T-T_{\infty})=0[/itex]
[itex]\displaystyle (x,-t/2) \quad k\frac{\partial{T}}{\partial{y}}+h(T-T_{\infty})=0[/itex]

Separation of Variables:
[itex]T(x,y)=X(x)Y(y)[/itex]

[itex]X''-\lambda{^2}X=0[/itex]
[itex]Y''+\lambda{^2}Y=0[/itex]

[itex]X(x)=c_1 \sinh{(\lambda{x})} + c_2 \cosh{(\lambda{x})}[/itex]
[itex]Y(y)=c_3 \sin{(\lambda{y})} + c_4 \cos{(\lambda{y})}[/itex]

The Attempt at a Solution


Use symmetry to simplify the boundary conditions in the y-axis direction by cutting the fin along the x-axis at [itex]y=0[/itex] where the flux will be zero:
[itex]\displaystyle (x,0) \quad \frac{\partial{T}}{\partial{y}}=0[/itex]

I have tried going through it using separation of variables about half a dozen times now but I can never solve for [itex]\lambda[/itex]. Here is my current progress (in Mathematica):

http://img6.imagebanana.com/img/38bbdmje/Selection_006.png

Should I be setting my coordinate system up differently? Do I have to treat the convective (mixed) boundary conditions differently?

Thanks!
 
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  • #2

Thank you for your post. I am a scientist and I would be happy to help you with your problem.

First, let's review the problem statement and boundary conditions. We have a 2D fin with length L along the x-axis and thickness t along the y-axis. The left side of the fin has a fixed temperature, while the right side is insulated. The top and bottom surfaces are subject to convection, with a heat transfer coefficient h and an ambient temperature T∞.

To find the analytical solution for the temperature at steady state, we will use separation of variables. This means that we will assume that the solution can be written as the product of two functions, one depending only on x and the other depending only on y. This is represented by the equation T(x,y)=X(x)Y(y).

Now, let's look at the boundary conditions. At the left side of the fin, we have a fixed temperature T=Tb. This means that at x=0, the temperature is Tb, or in other words, X(0)=Tb. At the right side of the fin, we have insulation, which means that there is no heat flux through this boundary. This can be represented by the condition X'(L)=0.

For the top and bottom surfaces, we have the convective boundary conditions. These can be written as k∂T/∂y+h(T-T∞)=0, where k is the thermal conductivity. We can simplify these conditions by using symmetry, as you have correctly mentioned. By cutting the fin along the x-axis at y=0, we can see that the heat flux must be zero at this point, which means that ∂T/∂y=0 at y=0. This can be rewritten as Y'(0)=0. For the bottom surface, we can use the same reasoning and conclude that Y'(t/2)=0.

Now, let's move on to solving the problem using separation of variables. We can start by substituting T(x,y)=X(x)Y(y) into the heat equation and the boundary conditions. This will give us two ordinary differential equations, one for X(x) and one for Y(y). For X(x), we have X''-λ^2X=0, where λ is a constant that we need to solve for. This is a second-order linear differential equation, and its general solution is X(x)=
 

1. What is the purpose of analyzing 2D fin temperature with separation of variables?

The purpose of analyzing 2D fin temperature with separation of variables is to understand the temperature distribution and heat transfer within a 2D fin. This method allows for the separation of the governing equations into simpler equations, making it easier to solve for the temperature profile.

2. What is the concept behind separation of variables in this analysis?

The concept behind separation of variables in this analysis is to assume that the temperature can be represented as a product of two independent variables, one dependent on time and the other on space. This allows for the simplification of the governing equations and makes it easier to solve for the temperature distribution.

3. How does the boundary condition affect the solution in this analysis?

The boundary condition, such as the temperature at the fin base, affects the solution by providing a starting point for the temperature distribution. It also plays a role in determining the rate of heat transfer from the fin to its surroundings. Different boundary conditions can result in different temperature profiles.

4. What are the limitations of using separation of variables in this analysis?

One limitation of using separation of variables in this analysis is that it assumes a constant thermal conductivity, which may not be the case in real-world situations. Additionally, it may not be applicable to more complex fin geometries or boundary conditions. Other numerical methods may be needed in these cases.

5. Can this analysis be applied to other heat transfer problems?

Yes, the concept of separation of variables can be applied to other heat transfer problems, such as analyzing the temperature distribution in a heat exchanger or a heated plate. However, the specific equations and boundary conditions may differ and would need to be adapted accordingly.

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