Newton Cooling and Radiative Cooling Dynamics
For a lumped body of heat capacity C, C dT/dt = -P_loss(T); Newton cooling gives P_loss=hA(T-T_s), while pure radiation gives P_loss=e sigma A(T^4-T_s^4).
Why this shows up in the exam
Comparing cooling rates of bodies · Solar-heating steady temperature · Time ratios in radiative cooling
Learn the idea
Cooling rate equals net heat-loss power divided by the body's heat capacity. Temperature does not fall because of temperature alone: the body loses power to its environment, and its thermal inertia converts that power into a rate of temperature change.
🧠 Memory hook: Loss power sets the fall; heat capacity sets the delay.
Get this one clearly and it pays off every single time it shows up in the paper. 🎯
Formulas & facts to keep ready
- C dT/dt = -P_loss(T) — lumped energy balance for cooling
- T-T_s = (T_i-T_s)e^(-t/tau) — Newton-cooling solution for constant coefficients
- tau = C/(hA) — Newton-cooling time constant
- C dT/dt = -e sigma A(T⁴-T_s⁴) — radiative cooling equation
How to approach it
- 1Write the body's total heat capacity
- 2Write the correct net loss law
- 3Form or integrate dT/dt and check the sign and limiting behavior
Common slip-ups that cost marks
- •Comparing power without dividing by heat capacity
- •Linearizing radiation over a large temperature range
- •Ignoring the surroundings temperature
🌟 That's the whole idea — you've got this. Try the practice set below; every question you attempt makes it stick a little harder.
Original chapter practice
Original questions for this chapter, not past-paper questions or an exact mapping to this individual concept.
A wire 1 m long and cross-sectional area 2 mm^2 extends by 1 mm under a 200 N load. Find Young modulus.
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