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PSU & GATE Mechanical Engineering Master Course

Lesson 6.2: Steady & Unsteady State Conduction

Conduction is the transfer of heat through a material due to a temperature gradient. GATE and PSU exams often test heat flux, temperature distribution, and conduction equations.


🔹 1. Introduction

  • Definition: Heat transfer through stationary medium without fluid motion.

  • Applications: Heat sinks, furnace walls, thermal insulation, electronic devices

  • Key Concepts:

    1. Thermal conductivity (k): Ability of material to conduct heat

    2. Temperature gradient: Drives heat transfer

    3. Steady vs Unsteady: Depends on whether temperature changes with time


🔹 2. Steady State Conduction

  • Definition: Temperature at any point does not change with time

∂T∂t=0\frac{\partial T}{\partial t} = 0

  • Governing Equation (1D):

qx=−kdTdxq_x = -k \frac{dT}{dx}

  • Through Plane Wall:

q=kA(T1−T2)Lq = \frac{k A (T_1 – T_2)}{L}

Where:
A = cross-sectional area, L = thickness, T₁/T₂ = temperatures

  • Through Cylindrical Wall:

q=2πkL(Ti−To)ln⁡(ro/ri)q = \frac{2 \pi k L (T_i – T_o)}{\ln(r_o/r_i)}

  • Through Spherical Wall:

q=4πk(Ti−To)(1/ri−1/ro)q = \frac{4 \pi k (T_i – T_o)}{(1/r_i – 1/r_o)}

  • Example: Heat transfer through wall 0.05 m thick, k = 50 W/m·K, A = 1 m², ΔT = 100 K → q = ?

q=kAΔTL=50∗1∗100/0.05=100kWq = k A \frac{\Delta T}{L} = 50*1*100/0.05 = 100 kW


🔹 3. Unsteady (Transient) Conduction

  • Definition: Temperature changes with time

∂T∂t≠0\frac{\partial T}{\partial t} \neq 0

  • Lumped Capacitance Method: Used when Biot number Bi < 0.1

T−T∞Ti−T∞=e−hAtρcV\frac{T-T_\infty}{T_i – T_\infty} = e^{- \frac{h A t}{\rho c V}}

Where:
h = convective coefficient, ρ = density, c = specific heat, V = volume

  • 1D Heat Equation:

∂T∂t=α∂2T∂x2,α=kρc\frac{\partial T}{\partial t} = \alpha \frac{\partial^2 T}{\partial x^2}, \quad \alpha = \frac{k}{\rho c}

  • Applications: Cooling of rods, transient heating, thermal energy storage


🔹 4. Solved Examples (PYQ Style)

  1. Heat flux through plane wall in steady state

  2. Temperature variation in lumped system (Bi < 0.1)

  3. Transient conduction in slab using 1D heat equation


🔹 5. Practice Exercises

  1. Calculate q for plane, cylindrical, and spherical walls

  2. Determine temperature variation in lumped capacitance system

  3. Solve 1D transient conduction problems

  4. Compute Biot number and validate lumped capacitance assumption


🔹 6. Summary

  • Steady State: Temperature constant with time, q = kΔT/L

  • Unsteady State: Temperature varies with time, use lumped capacitance or 1D heat equation

  • Applications: Thermal insulation, electronic cooling, transient heating

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