Consider
a thin rod of length L. Fourier's law,
relating heat flux q'' and temperature T is then q(x;T)=-kdT/dx, where 0<=x<=L is the position along rod, t is time, and k is the thermal conductivity. Using this
expression, and applying conservation of energy to a small element of the rod
between x and x+ \delta x yields the heat equation
where: alpha=k/cc is the thermal diffusivity, in which \rho is the mass density and cc is the specific heat capacity; Ta is the ambient temperature; and c is the heat transfer coefficient
between the rod and the ambient air. The last term in Eq. (1) represents the distributed heat flux due to
the temperature difference between the rod and air. In general, the parameters \alpha and c can depend on position, and Ta can depend on position and time.
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