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Question: A pycnometer weighs 40 gm when empty and 1040 gm when filled with mercury at \[0^\circ {\text{C}}\]....

A pycnometer weighs 40 gm when empty and 1040 gm when filled with mercury at 0C0^\circ {\text{C}}. On heating to 100C100^\circ {\text{C}}, 10 gm of mercury overflows. If the coefficient of real expansion of mercury is 0.0002/C0.0002/^\circ {\text{C}}, the coefficient of cubical expansion of glass is:
A. 0.00001/C0.00001/^\circ {\text{C}}
B. 0.0003/C0.0003/^\circ {\text{C}}
C. 0.0002/C0.0002/^\circ {\text{C}}
D. 0.0001/C0.0001/^\circ {\text{C}}

Explanation

Solution

Calculate the apparent expansion coefficient of the mercury using the expression for the volume expansion with respect to the temperature. The real expansion coefficient of the mercury is the sum of cubical expansion of the glass and the apparent expansion of the mercury. Then solve for the coefficient of cubical expansion of the glass.

Formula used:
γreal=γglass+γapp{\gamma _{real}} = {\gamma _{glass}} + {\gamma _{app}}
Here, γreal{\gamma _{real}} is the real expansion coefficient, γglass{\gamma _{glass}} is the cubical expansion coefficient of glass and γapp{\gamma _{app}} is the apparent coefficient of expansion.

Complete step by step answer:
We have given that the initial mass of the mercury is 1000 gm and when it is heated to 100C100^\circ {\text{C}}, 10 gm of mass overflows. We have the relation,
γapp=Mass overflowsInitial mass×ΔT{\gamma _{app}} = \dfrac{{{\text{Mass overflows}}}}{{{\text{Initial mass}} \times \Delta T}}
Here,γapp{\gamma _{app}} is the apparent coefficient of expansion of mercury and ΔT\Delta T is the change in the temperature.

Substituting the values, we get,
γapp=101000×100{\gamma _{app}} = \dfrac{{{\text{10}}}}{{1000 \times 100}}
γapp=0.0001/C\Rightarrow {\gamma _{app}} = 0.0001/^\circ {\text{C}}
We know that the real expansion of the mercury is the sum of cubical expansion of the glass and the apparent expansion of the mercury. Therefore,
γreal=γglass+γapp{\gamma _{real}} = {\gamma _{glass}} + {\gamma _{app}}
γglass=γrealγapp\Rightarrow {\gamma _{glass}} = {\gamma _{real}} - {\gamma _{app}}

Substituting 0.0002/C0.0002/^\circ {\text{C}} for γreal{\gamma _{real}} and 0.0001/C0.0001/^\circ {\text{C}} for γapp{\gamma _{app}} in the above equation, we get,
γglass=0.00020.0001{\gamma _{glass}} = 0.0002 - 0.0001
γglass=0.0001/C\therefore {\gamma _{glass}} = 0.0001/^\circ {\text{C}}
Therefore, the cubical expansion of the glass is 0.0001/C0.0001/^\circ {\text{C}}.

So, the correct answer is option D.

Note: Always remember when we heat the substance placed in the glass; both glass and the substance undergo volume expansion. To determine the apparent expansion coefficient of the mercury, we have used the expression for the volume expansion, ΔV=γViΔT\Delta V = \gamma {V_i}\Delta T, where, ΔV\Delta V is the change in the volume which can be treated as change in the weight, γ\gamma is the coefficient of volume expansion and ΔT\Delta T is the change in the temperature.