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A wall is made from an inhomogeneous (nonuniform) material for which the thermal conductivity varies through the thickness according to \(k=a x+b\), where \(a\) and \(b\) are constants. The heat flux is known to be constant. Determine expressions for the temperature gradient and the temperature distribution when the surface at \(x=0\) is at temperature \(T_{1}\).

Short Answer

Expert verified
The temperature gradient and temperature distribution expressions for an inhomogeneous material with a constant heat flux and thermal conductivity varying according to \(k = ax + b\) are: Temperature gradient: \(\frac{dT}{dx} = - \frac{q}{ax + b}\) Temperature distribution: \(T = - \frac{q}{a} \ln{(ax + b)} + T_1 + \frac{q}{a} \ln{(b)}\)

Step by step solution

01

Identify the governing equation

We'll start with the heat conduction equation, which is given by the Fourier's law: \(q = -k \frac{dT}{dx}\) where q is heat flux, k is the thermal conductivity, and \(dT/dx\) is the temperature gradient. Since the thermal conductivity is given as a function of x, we can write: \(k = ax + b\) The heat flux is constant, so we can rewrite the heat conduction equation as: \(q = - (ax + b) \frac{dT}{dx}\)
02

Solve for the temperature gradient

Now, we'll solve for the temperature gradient, \(dT/dx\). Rearrange the equation to isolate the temperature gradient: \(\frac{dT}{dx} = - \frac{q}{ax + b}\)
03

Integrate to find the temperature distribution

To find the temperature distribution, we'll now integrate both sides of the equation with respect to x: \(\int dT = -q \int \frac{dx}{ax + b}\) First, we can solve the right-hand side integral using substitution. Let \(u = ax + b\) \(du = adx\) \(dx = \frac{du}{a}\) The integral becomes: \(-q \int \frac{du}{au}\) Now, let's integrate: \(\int dT = - \frac{q}{a} \int \frac{du}{u}\) Integrate both sides to find T as a function of x: \(T = - \frac{q}{a} \ln{(|u|)} + C\) where C is the constant of integration. Now we can substitute u back and get the temperature distribution formula: \(T = - \frac{q}{a} \ln{(ax + b)} + C\)
04

Apply the boundary condition

We're given the boundary condition that when x = 0, the temperature T = \(T_1\). We can use this information to find C: \(T_1 = - \frac{q}{a} \ln{(a(0) + b)} + C\) \(T_1 = - \frac{q}{a} \ln{(b)} + C\) Rearrange to find the value of the constant C: \(C = T_1 + \frac{q}{a} \ln{(b)}\)
05

Write the final expressions

Now, we have the expressions for the temperature gradient and the temperature distribution: Temperature gradient: \(\frac{dT}{dx} = - \frac{q}{ax + b}\) Temperature distribution: \(T = - \frac{q}{a} \ln{(ax + b)} + T_1 + \frac{q}{a} \ln{(b)}\) And these are the expressions for the temperature gradient and temperature distribution for the given inhomogeneous material with a constant heat flux.

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