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Question: A one litre flask contains some mercury. It is found that at different temperatures the volume of ai...

A one litre flask contains some mercury. It is found that at different temperatures the volume of air inside the flask remains the same. The volume of mercury taken in the flask is : (Coefficient of linear expansion of glass is 9×106oC19 \times {10^{ - 6}}{}^o{C^{ - 1}} and coefficient of volume expansion of HgHg is 1.80×104oC11.80 \times {10^4}{}^o{C^{ - 1}} )
(A) 150ml150ml
(B) 750ml750ml
(C) 1000ml1000ml
(D) 700ml700ml

Explanation

Solution

Hint : Use the formula for volume expansion of solid to find the volume of mercury taken in the flask. THE formula for volume expansion is given by, ΔV=VγΔθ\Delta V = V\gamma \Delta \theta , where ΔV\Delta V is the change in volume VV is the initial volume γ\gamma is the volume expansion coefficient and Δθ\Delta \theta is the temperature change of the material in which the volume expansion of the material happens.

Complete Step By Step Answer:
We know that the volume expansion of a material is given by, ΔV=VγΔθ\Delta V = V\gamma \Delta \theta , where ΔV\Delta V is the change in volume VV is the initial volume γ\gamma is the volume expansion coefficient and Δθ\Delta \theta is the temperature change of the material in which the volume expansion of the material happens.
So, for glass we can write, (ΔV)g=VγgΔθ{\left( {\Delta V} \right)_g} = V{\gamma _g}\Delta \theta . Now, we have given the coefficient of linear expansion of glass αg{\alpha _g} . We know that the volume expansion coefficient is related to linear expansion coefficient as γ=3α\gamma = 3\alpha . Hence, we can write, (ΔV)g=VγgΔθ=V(3αg)Δθ{\left( {\Delta V} \right)_g} = V{\gamma _g}\Delta \theta = V(3{\alpha _g})\Delta \theta .
For mercury the change of volume of mercury can also be written similarly. So, (ΔV)m=VmγmΔθ{\left( {\Delta V} \right)_m} = {V_m}{\gamma _m}\Delta \theta .
Now, since volume of the air does not change due to the change of temperature, hence the change of volume of flask must be equal to the change of volume of mercury hence we can write,
(ΔV)g=(ΔV)m{\left( {\Delta V} \right)_g} = {\left( {\Delta V} \right)_m}
Or, 3αgV=γmVm3{\alpha _g}V = {\gamma _m}{V_m}
Putting the values, coefficient of linear expansion of flask αg=9×106oC1{\alpha _g} = 9 \times {10^{ - 6}}{}^o{C^{ - 1}} , coefficient of volume expansion of mercury γm=1.80×104oC1{\gamma _m} = 1.80 \times {10^4}{}^o{C^{ - 1}} and the volume of flask V=1lV = 1l we get,
3×9×106×1=1.80×104Vm3 \times 9 \times {10^{ - 6}} \times 1 = 1.80 \times {10^4}{V_m}
On simplifying we get ,
Vm=27×1061.80×104{V_m} = \dfrac{{27 \times {{10}^{ - 6}}}}{{1.80 \times {{10}^4}}}
Or, Vm=0.15{V_m} = 0.15
Hence, volume of mercury taken in flask is 0.15l0.15l or 0.15×1000=150ml0.15 \times 1000 = 150ml
Hence, option (A ) is correct.

Note :
\bullet The temperature change for both the flask and mercury is the same.
\bullet When the volume of air changes then we can find the change in volume of the air using Charles’s law of ideal gas and then find the volume of the mercury in the flask.
\bullet The coefficient of areal expansion is related to linear expansion as β=2α\beta = 2\alpha where β\beta is the coefficient of areal expansion.