$A$ piece of granite floats at the interface of mercury and water contained in a beaker as shown in the figure. If the densities of granite,water,and mercury are $\rho, \rho_1$,and $\rho_2$ respectively,the ratio of the volume of granite in water to the volume of granite in mercury is:

  • A
    $\frac{\rho_2-\rho}{\rho-\rho_1}$
  • B
    $\frac{\rho_2+\rho}{\rho_1+\rho}$
  • C
    $\frac{\rho_1 \rho_2}{\rho}$
  • D
    $\frac{\rho_1}{\rho_2}$

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What is buoyancy?

$A$ gas in equilibrium has uniform density and pressure throughout its volume. This is strictly true only if there are no external influences. $A$ gas column under gravity,for example,does not have uniform density (and pressure). As you might expect,its density decreases with height. The precise dependence is given by the so-called law of atmospheres:
$n_{2}=n_{1} \exp \left[-m g\left(h_{2}-h_{1}\right) / k_{B} T\right]$
where $n_{2}, n_{1}$ refer to number density at heights $h_{2}$ and $h_{1}$ respectively. Use this relation to derive the equation for sedimentation equilibrium of a suspension in a liquid column:
$n_{2}=n_{1} \exp \left[-m g N_{A}\left(\rho-\rho^{\prime}\right)\left(h_{2}-h_{1}\right) /(\rho R T)\right]$
where $\rho$ is the density of the suspended particle,and $\rho^{\prime}$ that of the surrounding medium. [$N_{A}$ is Avogadro's number,and $R$ the universal gas constant.]

State the law of floatation.

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