Introduction to finite elements/Steady state heat conduction
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Steady state heat conduction[edit | edit source]
If the problem does not depend on time and the material is isotropic, we get the boundary value problem for steady state heat conduction.
Poisson's equation[edit | edit source]
If the material is homogeneous the density, heat capacity, and the thermal conductivity are constant. Define the thermal diffusivity as
Then, the boundary value problem becomes
where is the Laplacian
Laplace's equation[edit | edit source]
Finally, if there is no internal source of heat, the value of is zero, and we get Laplace's equation.
The Analogous Membrane Problem[edit | edit source]
The thin elastic membrane problem is another similar problem. See Figure 1 for the geometry of the membrane.
The membrane is thin and elastic. It is initially planar and occupies the 2D domain . It is fixed along part of its boundary . A transverse force per unit area is applied. The final shape at equilibrium is nonplanar. The final displacement of a point on the membrane is . There is no dependence on time.
The goal is to find the displacement at equilibrium.
It turns out that the equations for this problem are the same as those for the heat conduction problem - with the following changes:
- The time derivatives vanish.
- The balance of energy is replaced by the balance of forces.
- The constitutive equation is replaced by a relation that states that the vertical force depends on the displacement gradient ().
If the membrane if inhomogeneous, the boundary value problem is:
For a homogeneous membrane, we get
Note that the membrane problem can be formulated in terms of a problem of minimization of potential energy.