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Mathematics · Ch 10 — Ordinary Differential Equations

Newton's Law of cooling/warming

10.8.3

Newton's Law of cooling/warming

Pour a 150∘150^\circ cup of coffee onto a table in an 80∘C80^\circ\mathrm C room, and it cools until it reaches room temperature; take a 35∘35^\circ glass of water from the fridge into the same room, and it warms up until it reaches room temperature. Both observations are captured by a single law.

Newton's Law of Cooling/Warming. The rate at which a body's temperature changes is proportional to the difference between the body's temperature and the temperature of the surrounding medium (the ambient temperature). If T(t)T(t) is the body's temperature at time tt and TmT_m is the (constant) ambient temperature,

dTdt∝(T−Tm)or equivalentlydTdt=k(T−Tm),\dfrac{dT}{dt}\propto (T-T_m)\quad\text{or equivalently}\quad\dfrac{dT}{dt}=k(T-T_m),

where kk is the constant of proportionality. In either case — cooling or warming, with TmT_m held constant — it stands to reason that k<0k<0: the temperature gap always shrinks towards zero over time.

Solution. Separating variables, dTT−Tm=k dt\dfrac{dT}{T-T_m}=k\,dt, and integrating gives

T−Tm=Cekt.T-T_m=Ce^{kt}.

The constant CC is fixed by the temperature at t=0t=0 (usually the first reading), and kk is fixed from a second reading at some later time; once both constants are known, T(t)T(t) can be evaluated at any time, or the equation can be inverted to find the time at which a target temperature is reached. …