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Physics · Ch 8 — Heat and Thermodynamics

Newton's Law of Cooling

8.2.8

Newton's Law of Cooling

Newton's law of cooling states that the rate at which a hot object loses heat is proportional to how much hotter it currently is than its surroundings: dQdt∝−(T−Ts)\dfrac{dQ}{dt}\propto-(T-T_s), where TsT_s is the surrounding temperature (the negative sign shows the rate of loss itself decreases as the object cools). Combining this with dQ=ms dTdQ=ms\,dT and integrating gives the exponential solution T=Ts+b2e−amstT=T_s+b_2e^{-\frac{a}{ms}t}, which matches the graph in Figure 8.12: cooling is fastest right at the start (largest temperature excess) and progressively slows as the object approaches room temperature, tracing a curve rather than a straight line. Example 8.8 applies this practically: knowing a hot-water sample takes 3 minutes to cool from 92°C to 84°C at a 27°C room temperature lets you predict the time it takes to cool through a diffe …

Figure 8.12Cooling of hot water with time

What this figure shows. A graph of temperature (°C, y-axis, marked from 10 up to 100) against time (seconds, x-axis, marked out to 300 seconds) for a sample of hot water cooling in a room. The curve starts steep near the top of the graph (rapid initial cooling, when the water is much hotter than the surrounding air at temperature Ts, marked with a horizontal dashed line) and progressively flattens out as it approaches the surrounding temperature Ts, never quite reaching it within the plotted range. This shape is the graphical signature of Newton's law of cooling: the rate of cooling is fastest when the temperature difference from the surroundings is large …