Lumped Capacitance Time Constant
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ρVc is the heat a body stores per kelvin — its thermal capacitance — and hA is the conductance draining it. Their ratio is a time constant in exactly the sense an electrical engineer means, and the analogy is complete: the body is a capacitor, the surface film is a resistor, and the temperature decays exponentially. In one τ the gap to ambient closes by 63%, in three τ by 95%, in five τ by over 99%.
Worked example: an aluminium block, ρ = 2700 kg/m³, V = 100 cm³, c = 900 J/(kg·K), cooling in air at h = 30 W/(m²·K) over A = 0.02 m². τ = 2700 × 0.0001 × 900/(30 × 0.02) = 243/0.6 = 405 s, so it is essentially at room temperature in about twenty minutes. This is the number that sizes thermocouple response — a fine bead responds in milliseconds, a 6 mm thermowell in a stagnant pocket can lag a minute, and a control loop tuned without knowing which one you have will hunt forever. Trap: τ assumes the lumped regime, so check Bi < 0.1 before trusting it, and remember h is not constant during a violent transient — free convection off a hot block starts strong and weakens as the block cools.
- = Thermal time constant
- = Density
- = Body volume
- = Specific heat
- = Film coefficient
- = Surface area
- Thermal time constant — Lumped Capacitance Cooling Curve, Fourier Number
- Density — Fourier Number, Density
- Body volume — Boyle's Law, Charles's Law
- Specific heat — Stream Duty from Mass Flow (Q = ṁcΔT), Fourier Number
- Film coefficient — Fin Parameter mL (Straight Fin), Fin Heat Transfer Rate
- Surface area — Newton's Law of Cooling (Q = hAΔT), Net Radiation Exchange Between Surfaces