The electric motor of a heat pump transfers energy as heat from the outdoors, which is at $-10^{\circ} \mathrm{C}$, to a room that is at $17^{\circ} \mathrm{C}$. If the heat pump were a Carnot heat pump (a Carnot engine working in reverse), how much energy would be transferred as heat to the room for each joule of electric energy consumed?
a configuration of the system. The number of microstates in a configuration is the multiplicity $W$ of the configuration.
For a system of $N$ molecules that may be distributed between the two halves of a box, the multiplicity is given by
$$
W=\frac{N !}{n_{1} ! n_{2} !},
$$
in which $n_1$ is the number of molecules in one half of the box and $n_2$ is the number in the other half. A basic assumption of statistical mechanics is that all the microstates are equally probable. Thus, configurations with a large multiplicity occur most often.
The multiplicity $W$ of a configuration of a system and the entropy $S$ of the system in that configuration are related by Boltzmann's entropy equation:
$$
S=k \ln W,
$$
where $k=1.38 \times 10^{-23} \mathrm{~J} / \mathrm{K}$ is the Boltzmann constant.