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Question: Two liquids of densities \(d_1\)​ and \(d_2\)​ are flowing in identical capillary tubes under the sa...

Two liquids of densities d1d_1​ and d2d_2​ are flowing in identical capillary tubes under the same pressure difference. If t1t_1​ and t2t_2​ are time taken for the flow of equal quantities (mass) of liquids, then the ratio of coefficient of viscosity of liquids must be:
(A) d1t1d2t2\dfrac{{{d_1}{t_1}}}{{{d_2}{t_2}}}
(B) t1t2\dfrac{{{t_1}}}{{{t_2}}}
(C) d2t2d1t1\dfrac{{{d_2}{t_2}}}{{{d_1}{t_1}}}
(D) d1t1d2t2\sqrt {\dfrac{{{d_1}{t_1}}}{{{d_2}{t_2}}}}

Explanation

Solution

The Poiseuille’s law provides information about the rate of the flow of liquid in a capillary tube when there is pressure difference at both the ends of the tube. And the rate of flow gives the amount of the fluid passed in unit times from a cross-section.

Complete step by step answer:
Given,
It is given that both the capillary tubes are in the same pressure difference, let it is ΔP\Delta P .
The density of the first liquid is d1{d_1} , and the density of the second liquid is d2{d_2} .
It is given that the time taken by the first and second liquid is t1{t_1}and t2{t_2} respectively for the flow of the same mass mm.
The expression for the rate of flow of the liquid across the end of a capillary tube is given as follows,
Q=πr4ΔP8μLQ = \dfrac{{\pi {r^4}\Delta P}}{{8\mu L}}
Here, μ\mu is the viscosity of the liquid and rr is the radius of the capillary tube and LL is the length of the tube.
Now, we write the expression for the rate of flow of the liquid for first tube,
Q1=πr14ΔP8μ1L1  ...............(1){Q_1} = \dfrac{{\pi r_1^4\Delta P}}{{8{\mu _1}{L_1}}}\;...............{\rm{(1)}}
Now, we write the expression for the rate of flow of the liquid for second tube,
Q2=πr24ΔP8μ2L2  ...............(2){Q_2} = \dfrac{{\pi r_2^4\Delta P}}{{8{\mu _2}{L_2}}}\;...............{\rm{(2)}}
It is given that the tubes are identical, so the value of rr and LL will be the same for both the tube, and we can write,
r1=r2{r_1} = {r_2} and L1=L2{L_1} = {L_2}
Divide the equation (1) by the equation (2).
Q1Q2=πr14ΔP8μ1L1πr24ΔP8μ2L2 Q1Q2=μ2μ1  ..................(3) \Rightarrow\dfrac{{{Q_1}}}{{{Q_2}}} = \dfrac{{\dfrac{{\pi r_1^4\Delta P}}{{8{\mu _1}{L_1}}}}}{{\dfrac{{\pi r_2^4\Delta P}}{{8{\mu _2}{L_2}}}}}\\\ \Rightarrow\dfrac{{{Q_1}}}{{{Q_2}}} = \dfrac{{{\mu _2}}}{{{\mu _1}}}\;..................{\rm{(3)}}
Also, we know that the expression for the discharge is,
Q=Vt Q=md×t Q = \dfrac{V}{t}\\\ \Rightarrow Q = \dfrac{m}{{d \times t}}
Here, VV is the volume of the liquid, mm is the mass of the liquid, dd is the density of the liquid and tt is the time.
Now, substitute the value of discharge for both the liquid in the equation (3).
md1×t1md2×t2=μ2μ1 μ1μ2=md2×t2md1×t1 μ1μ2=d1×t1d2×t2 \Rightarrow\dfrac{{\dfrac{m}{{{d_1} \times {t_1}}}}}{{\dfrac{m}{{{d_2} \times {t_2}}}}} = \dfrac{{{\mu _2}}}{{{\mu _1}}}\\\ \Rightarrow\dfrac{{{\mu _1}}}{{{\mu _2}}} = \dfrac{{\dfrac{m}{{{d_2} \times {t_2}}}}}{{\dfrac{m}{{{d_1} \times {t_1}}}}}\\\ \therefore\dfrac{{{\mu _1}}}{{{\mu _2}}} = \dfrac{{{d_1} \times {t_1}}}{{{d_2} \times {t_2}}}
Therefore, ratio of the viscosity will be d1t1d2t2\dfrac{{{d_1}{t_1}}}{{{d_2}{t_2}}} and the correct answer is option (A).

Note: The viscosity of a fluid provides information about the resistance of the fluid against the motion, so the fluid having low viscosity can move quickly on a surface, but the fluid that has a high value of viscosity, moves slower.