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Question: An open glass tube is immersed in mercury in such a way that a length of \(8cm\) tends about the mol...

An open glass tube is immersed in mercury in such a way that a length of 8cm8cm tends about the molecular level. The open end of the tube is closed and sealed and the tube is raised vertically up by an additional 48cm48cm. What will be the length of the air column about mercury in the tube now? (Atmospheric pressure= 76cm76cm of Hg)
(A). 38cm38cm
(B). 6cm6cm
(C). 16cm16cm
(D). 22cm22cm

Explanation

Solution

Give, the tube is first raised by 8cm8cm and then raised by 48cm48cm. In the first condition, the pressure will be due to the air column only but in the second condition, the pressure will be due to mercury as well as air column. Using the ideal gas law equation and formula for pressure in a fluid and equating the pressures at equilibrium point, we can calculate the length of the air column.
Formulas used:
PV=nRTPV=nRT
P=ρghP=\rho gh

Complete answer:

The ideal gas equation is given by-
PV=nRTPV=nRT - (1)
Here, PP is the pressure
VV is the volume
nn is the number of moles
RR is the gas constant
TT is the temperature
By isothermal process condition, the temperature of both bodies at a given number of moles is same, therefore,
T1=T2{{T}_{1}}={{T}_{2}}
From eq (1), we have
P1V1nR=P2V2nR\dfrac{{{P}_{1}}{{V}_{1}}}{nR}=\dfrac{{{P}_{2}}{{V}_{2}}}{nR}
P1V1=P2V2\Rightarrow {{P}_{1}}{{V}_{1}}={{P}_{2}}{{V}_{2}} - (2)
Let P0{{P}_{0}} be the pressure of tube-1 and PP be the pressure of tube-2. We know that volume can be written as a product of area and length. Substituting given values in eq (2), we get,
P08A=PxA{{P}_{0}}8A=PxA
P=8P0x\Rightarrow P=\dfrac{8{{P}_{0}}}{x} - (3)
We know that pressure in a fluid is given as-
P=ρghP=\rho gh - (4)
Here, ρ\rho is the density of the fluid
gg is acceleration due to gravity
hh is the height in the fluid
Using the above equation, we get,
P0=ρmg(76){{P}_{0}}={{\rho }_{m}}g(76) - (5)
Using eq (3), eq (4), eq (5) equating pressures at point A and B, we get,
ρmg(76)=8P0x+ρmg(54x) ρmg(76)=8ρmg(76)x+ρmg(54x) 76=8×76x+(54x) 22+x=608x x2+22x608=0 x2+38x16x608=0 (x+38)(x16)=0 x=16cm \begin{aligned} & {{\rho }_{m}}g(76)=\dfrac{8{{P}_{0}}}{x}+{{\rho }_{m}}g(54-x) \\\ & \Rightarrow {{\rho }_{m}}g(76)=\dfrac{8{{\rho }_{m}}g(76)}{x}+{{\rho }_{m}}g(54-x) \\\ & \Rightarrow 76=\dfrac{8\times 76}{x}+(54-x) \\\ & \Rightarrow 22+x=\dfrac{608}{x} \\\ & \Rightarrow {{x}^{2}}+22x-608=0 \\\ & \Rightarrow {{x}^{2}}+38x-16x-608=0 \\\ & \Rightarrow (x+38)(x-16)=0 \\\ & \therefore x=16cm \\\ \end{aligned}
Therefore, the length of the air column about mercury in the tube is 16cm16cm.

Hence, the correct option is (C).

Note:
Using the thermodynamic equation is more efficient than using the ideal gas equation in this question. Isothermal process is the process in which temperature remains constant, since bodies are kept at room temperature, we can apply isothermal condition here. The pressures at point A and B are equal because in both tubes equilibrium is established at these points.