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
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Definition: Heat transfer through stationary medium without fluid motion.
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Applications: Heat sinks, furnace walls, thermal insulation, electronic devices
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Key Concepts:
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Thermal conductivity (k): Ability of material to conduct heat
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Temperature gradient: Drives heat transfer
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Steady vs Unsteady: Depends on whether temperature changes with time
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🔹 2. Steady State Conduction
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Definition: Temperature at any point does not change with time
∂T∂t=0\frac{\partial T}{\partial t} = 0
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Governing Equation (1D):
qx=−kdTdxq_x = -k \frac{dT}{dx}
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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
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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)}
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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)}
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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
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Definition: Temperature changes with time
∂T∂t≠0\frac{\partial T}{\partial t} \neq 0
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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
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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}
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Applications: Cooling of rods, transient heating, thermal energy storage
🔹 4. Solved Examples (PYQ Style)
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Heat flux through plane wall in steady state
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Temperature variation in lumped system (Bi < 0.1)
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Transient conduction in slab using 1D heat equation
🔹 5. Practice Exercises
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Calculate q for plane, cylindrical, and spherical walls
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Determine temperature variation in lumped capacitance system
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Solve 1D transient conduction problems
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Compute Biot number and validate lumped capacitance assumption
🔹 6. Summary
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Steady State: Temperature constant with time, q = kΔT/L
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Unsteady State: Temperature varies with time, use lumped capacitance or 1D heat equation
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Applications: Thermal insulation, electronic cooling, transient heating
