Fourier's Law Of Heat Conduction
In a one dimensional differential form, Fourier's Law is as follows:
1) q = Q/A = -kdT/dx.
The symbol q is the heat flux, which is the heat per unit area, and it is a vector. Q is the heat rate. dT/dx is the thermal gradient in the direction of the flow. The minus sign is to show that the flow of heat is from hotter to colder. If the temperature decreases with x, q will be positive and will flow in the direction of x. If the temperature increases with x, q will be negative, and will flow opposite to the direction of x. In the International System of Units SI, q is watts per meter squared (w/m2).
The constant k is the thermal conductivity, and is used to show that not all materials heat up or retain heat equally well. In SI units, k is W/m*K, where W is watts, m is meters, and K is kelvin. It may also be J/m *s*K, where J is joules and s is seconds. In the English system, it is Btu/h*ft*oF, or British thermal units per horsepower*foot*Fahrenheit.
The thermal conductivity is larger for conductors than insulators. Silver is an excellent conductor at 428 W/m * k, and so is copper with its value of 401 W/m * k. Air and wool are insulators and are poor conductors; they are 0.026 and 0.043 W/m*k, respectively.
The heat transfer or conduction rate is a scalar and is
2) Q = -kA ΔT/L,
where L is the length of the slab. ΔT is the temperature difference between two different surfaces.
Equations 1 and 2 show that heat can be considered to be a flow. The flow of heat depends upon the thickness of the material, the area, and the conductivity, all of which combine to retard or resist this flow.