Heat Transfer — Conduction
In steady state, thermal energy flows from hot to cold through a material; Fourier's law quantifies the rate as proportional to area and temperature gradient.
Concept
Fourier's law (1-D steady state):
where is thermal conductivity (W/m·K). For a uniform slab of thickness :
By analogy with electrical resistance, thermal resistance is . Series resistances add; parallel conductances add.
Derivation
Two slabs in series, thicknesses and conductivities . In steady state, the same heat current passes through both:
Eliminating :
so the effective conductivity for equal-area slabs:
For parallel slabs of equal length and different areas, the effective is area-weighted.
JEE Worked Example
Problem: A compound wall is made of two layers: 10 cm thick brick ( W/mK) and 5 cm thick wood ( W/mK). Outside is at °C, inside at °C. Find the heat current per m² and the interface temperature.
Solution:
Interface from inside: °C (wood between inside and brick).
Traps
- Fourier's law assumes steady state; transient problems need the heat equation.
- For radial conduction in a cylinder, — not linear.
- In series, the highest-resistance layer drops most of the temperature.
- Don't confuse conductivity (intensive) with conductance (extensive).
- For composite rods with different areas, area cancellation does not apply directly.
Key Takeaways
- in 1-D steady state.
- ; series adds, parallel like resistors.
- The largest thermal-resistance layer controls heat flow.
- Use radial form for cylindrical and spherical geometries.