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Question: A U-tube of base length ‘\[l\]’ is filled with the same volume of two liquids of densities \[\rho \]...

A U-tube of base length ‘ll’ is filled with the same volume of two liquids of densities ρ\rho and 2ρ2\rho is moving with an acceleration ‘aa’ on the horizontal plane. If the height difference between the two surfaces (open to atmosphere) becomes zero then the height hh is given by

A. a2gl\dfrac{a}{{2g}}l
B. 3a2gl\dfrac{{3a}}{{2g}}l
C. agl\dfrac{a}{g}l
D. 2a3gl\dfrac{{2a}}{{3g}}l

Explanation

Solution

Use the formula of pressure-depth relation. This formula gives the relation between the atmospheric pressure, density of liquid, acceleration of liquid and depth.

Formula used:
The pressure PP at a depth hh is given by
P=P0+ρghP = {P_0} + \rho gh …… (1)
Here, P0{P_0} is the atmospheric pressure, ρ\rho is the density and gg is the acceleration due to gravity.

Complete step by step answer:
A U-tube of base length ‘ll’ is filled with the same volume of two liquids of densities ρ\rho and 2ρ2\rho which are moving with an acceleration ‘aa’ on the horizontal plane.
Redraw the diagram of the U-tube.

The liquid with the density 2ρ2\rho must be moving slowly as compared to the liquid with the density ρ\rho .
The liquids have the acceleration aa only in the horizontal plane and not in the vertical plane.
Using equation (1), determine the pressure PA{P_A} at point A considering the right column of the U-tube.
PA=P0+ρgh{P_A} = {P_0} + \rho gh
Using equation (1), determine the pressure PB{P_B} at point B from point A considering the right column of the U-tube.
PB=PA+ρal2{P_B} = {P_A} + \rho a\dfrac{l}{2}
Substitute P0+ρgh{P_0} + \rho gh for PA{P_A} in the above equation.
PB=P0+ρgh+ρal2{P_B} = {P_0} + \rho gh + \rho a\dfrac{l}{2}
Using equation (1), determine the pressure PC{P_C} at point C from point B considering the right column of the U-tube.
PC=PB+2ρal2{P_C} = {P_B} + 2\rho a\dfrac{l}{2}
Substitute P0+ρgh+ρal2{P_0} + \rho gh + \rho a\dfrac{l}{2} for PB{P_B} in the above equation.
PC=P0+ρgh+ρal2+2ρal2{P_C} = {P_0} + \rho gh + \rho a\dfrac{l}{2} + 2\rho a\dfrac{l}{2}
PC=P0+ρgh+32ρal{P_C} = {P_0} + \rho gh + \dfrac{3}{2}\rho al …… (2)
Using equation (1), determine the pressure PC{P_C} at point C considering the left column of the U-tube.
PC=P0+2ρgh{P_C} = {P_0} + 2\rho gh …… (3)
The height difference between the two surfaces of two liquids open to the atmosphere becomes zero. Hence, the pressure at point C from both right and left liquid columns are the same.
Equate equation (2) and (3).
P0+ρgh+32ρal=P0+2ρgh{P_0} + \rho gh + \dfrac{3}{2}\rho al = {P_0} + 2\rho gh
32ρal=ρgh\Rightarrow \dfrac{3}{2}\rho al = \rho gh
Rearrange the above equation for height hh.
h=32ρalρgh = \dfrac{{\dfrac{3}{2}\rho al}}{{\rho g}}
h=3a2gl\Rightarrow h = \dfrac{{3a}}{{2g}}l
Therefore, the height hh is 3a2gl\dfrac{{3a}}{{2g}}l.

So, the correct answer is “Option B”.

Note:
The pressure-depth relation is not the same for the pressure at the height h.
The height difference between the two surfaces (open to atmosphere) becomes zero.
The average density of a substance or object is defined as its mass per unit volume.