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Principles of Waves, Fluids and Thermodynamics

Heat Transfer: Conduction, Convection, Radiation

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Touch a metal bench and a wooden one on the same cold morning: same temperature, wildly different feel. Your skin measures heat flow, not temperature — and conduction, convection and radiation are the three highways that flow can take. Engineering a thermos is just blocking all three at once.

There are three mechanisms of heat transfer.

Conduction — Heat flows through a material by molecular collisions:

dQdt=kAdTdx(Fourier’s law)\frac{dQ}{dt} = -kA\frac{dT}{dx} \qquad\text{(Fourier's law)}

where kk is thermal conductivity (W/(m K)).

Thermal resistance for a slab of thickness LL:

Rth=LkA,dQdt=ΔTRthR_{\text{th}} = \frac{L}{kA}, \qquad \frac{dQ}{dt} = \frac{\Delta T}{R_{\text{th}}}

Convection — Heat carried by fluid motion:

dQdt=hA(TsT)\frac{dQ}{dt} = hA(T_s - T_\infty)

where hh is the convective heat transfer coefficient.

Radiation — All objects emit thermal radiation:

P=εσAT4(Stefan-Boltzmann law)P = \varepsilon\sigma A T^4 \qquad\text{(Stefan-Boltzmann law)}

ConstantValue
σ\sigma (Stefan-Boltzmann)5.67×1085.67\times 10^{-8} W/(m2^{2} K4^{4})
ε\varepsilon (emissivity)00 (perfect reflector) to 11 (blackbody)

Wien's displacement law — Peak wavelength of blackbody radiation:

λmaxT=2.898×103  m K\lambda_{\max} T = 2.898\times 10^{-3}\;\text{m K}

Physics link: The Sun (T5778T \approx 5778 K) peaks at λ500\lambda \approx 500 nm (visible light). The Earth (T288T \approx 288 K) peaks at λ10  μ\lambda \approx 10\;\mum (infrared).
Common pitfall: "Cold" is not a thing that flows into you. There is only heat flowing out. Every heat-transfer analysis tracks energy moving from hot to cold; reversing the bookkeeping direction is the fastest way to sign errors.
Placeholder: Heat Transfer: Conduction, Convection, Radiation

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Principles of Waves, Fluids and Thermodynamics