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Question: In a cylindrical glass container a solid silica cylinder is placed vertically at its bottom and rema...

In a cylindrical glass container a solid silica cylinder is placed vertically at its bottom and remaining space is filled with mercury up to the top level of the silica cylinder as shown in the figure . Assume that the volume of silica remains unchanged due to variation in temperature, the coefficient of cubical expansion of mercury is γ\gamma and the coefficient of linear expansion of glass is α\alpha. If the top surface of silica and mercury level remains at the same level with the variation in temperature then the ratio of volume of mercury and volume of silica is equal to

Explanation

Solution

Kinetic energy is the free motion input to a mass to make the identical momentum change or the momentum change that releases the identical amount of free passage of mass onto another mass. Momentum is the result of the product of the mass of the body and its velocity. We will change wavelengths in terms of kinetic energy and mass; then we will get the ratio of wavelengths by putting the mass of electron and proton.

Complete step-by-step solution:
Given that the system of cylindrical glass container, with say volume vgv_g initially contains silica of volume vsv_s and liquid mercury of volume vmv_m.
Then, we have
vg=vs+vmv_g=v_s+v_m
When the system is heated, and the temperature is increased by and let the increase in volume of the glass cylinder be marked as ΔVg\Delta V_g and if ΔVm\Delta V_m and ΔVs\Delta V_s be the increase in volume of the mercury and silica, then
ΔVg=ΔVm+ΔVs\Delta V_g=\Delta V_m+\Delta V_s
Given that ΔVs=0\Delta V_s=0
Then we have, ΔVg=ΔVm\Delta V_g=\Delta V_m,
From thermal expansion, we know that ΔV=V×α×ΔT\Delta V=V\times \alpha \times \Delta T, where α\alpha is the coefficient of thermal expansion and VV is the initial volume.
Also given that the coefficient of cubical expansion of mercury is γ\gamma and the coefficient of linear expansion of glass is α\alpha and αv=3αl\alpha_v=3\alpha_l, whereαv\alpha_v and αl\alpha_l are the coefficient of volume expansion and the coefficient of linear expansion respectively.
Substituting, we have
    ΔT×3α×vg=ΔT×γ×vm\implies \Delta T\times 3\alpha \times v_g=\Delta T\times \gamma \times v_m
    3α×vg=γ×vm\implies 3\alpha \times v_g=\gamma\times v _m
    3α(vs+vm)=γ×vm\implies 3\alpha(v_s+v_m)=\gamma \times v_m
    3α(vsvm+1)=γ\implies 3\alpha\left(\dfrac{v_s}{v_m}+1\right)=\gamma
    (vsvm+1)=γ3α\implies \left(\dfrac{v_s}{v_m}+1\right)=\dfrac{\gamma }{3\alpha}
    vsvm=γ3α1\implies \dfrac{v_s}{v_m}=\dfrac{\gamma }{3\alpha}-1
Thus the ratio of volume of mercury and volume of silica is equal to vsvm=γ3α1\dfrac{v_s}{v_m}=\dfrac{\gamma }{3\alpha}-1

Note: Thermal expansion can change the shape, area, volume and/or the density of the given substance. And αl\alpha_l which is the coefficient of linear expansion. However, other expansions can also be written with respect to αl\alpha_l as αv=3αl\alpha_v=3\alpha_l and αa=2αl\alpha_a=2\alpha_l are the coefficient of volume expansion and coefficient of area expansion respectively mainly for isotropic solids.