# Temperature of Body under Newton's Law of Cooling

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## Contents

## Theorem

Let $B$ be a body in an environment whose ambient temperature is $H_a$.

Let $H$ be the temperature of $B$ at time $t$.

Let $H_0$ be the temperature of $B$ at time $t = 0$.

Then:

- $H = H_a - \paren {H_0 - H_a} e^{-k t}$

where $k$ is some positive constant.

## Proof

- The rate at which a hot body loses heat is proportional to the difference in temperature between it and its surroundings.

We have the differential equation:

- $\dfrac {\d H} {\d t} \propto - \paren {H - H_a}$

That is:

- $\dfrac {\d H} {\d t} = - k \paren {H - H_a}$

where $k$ is some positive constant.

This is an instance of the Decay Equation, and so has a solution:

- $H = H_a + \paren {H_0 - H_a} e^{-k t}$

$\blacksquare$

## Source of Name

This entry was named for Isaac Newton.

He applied this law to make an estimate of the temperature of a red-hot iron ball. Although this approximation was somewhat crude, it was better than anything else up till then.

## Sources

- 1972: George F. Simmons:
*Differential Equations*... (previous) ... (next): $\S 1.4$: Growth, Decay and Chemical Reactions: Problem $5$ - 1977: Gary Chartrand:
*Introductory Graph Theory*... (previous) ... (next): $\S 1.2$: Mathematical Models: Example $\S 1.2$ (but beware - the expression given is incorrect)