The true weight of an object can be measured in a vacuum, where buoyant forces are absent. A measurement in air, however, is disturbed by buoyant forces. An object of volume $V$ is weighed in air on an equal-arm balance with the use of counterweights of density $\rho$. Representing the density of air as $\rho_{\text {air }}$ and the balance reading as $F_{g}^{\prime}$, show that the true weight $F_{g}$ is $F_{g}=F_{g}^{\prime}+\left(V-\frac{F_{g}^{\prime}}{\rho g}\right) \rho_{\mathrm{air}} g$