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Viscosity MCQ - Practice Questions with Answers

Edited By admin | Updated on Sep 25, 2023 25:23 PM | #NEET

Quick Facts

  • Viscosity is considered one of the most asked concept.

  • 18 Questions around this concept.

Solve by difficulty

A beaker contains a fluid of density \rho kg/m3, specific heat S J/kg 0C and viscosity \eta. The beaker is filled up to height h. To estimate the rate of heat transfer per unit area (Q /A) by convection when a beaker is put on a hot plate, a student proposes that it should depend on \eta,

\left ( \frac{S\Delta \Theta }{h} \right ) \: and\: \left ( \frac{1}{\rho g} \right )when \Delta \Theta   (in_{}^{0}\textrm{C}) is the difference in the temperature between the bottom and top of the fluid. In that situation the correct option for (Q /A) is:

 

A spherical steel ball released at the top of a long column of glycerine of length L falls through a distance \mathrm{L / 2} with accelerated motion and the remaining distance \mathrm{ L / 2} with a uniform velocity. If \mathrm{ t_1} and \mathrm{ t_2} denote the times taken to cover the first and second half and W1 and W2 the work done against gravity in the two halves, then

There is a 1 \mathrm{~mm} thick layer of water between a plate of area 100 \mathrm{~cm}^{2} and another very big plate. The coefficient of viscosity of water is 0.01 poise. Then the force required to move the smaller plate with a velocity of 10 \mathrm{~cm} / \mathrm{sec} with respect to the larger plate is:

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 A thin horizontal disc of radius \mathrm{R} is located within a cylindrical cavity filled with oil whose viscosity is\mathrm{ ' \eta '.} The distance between the disc and horizontal planes of cavity is \mathrm{ ' h '. }The power developed by the viscous forces acting on the disc when it rotates with angular velocity \mathrm{ \omega} (The end effects are to be neglected)

Concepts Covered - 1

Viscosity
  • Viscosity-

 Ideal fluids are non-viscous. But for real fluids, there is a viscous force between the adjacent layers of fluids which are in contact.

In case of a steady flow of a fluid when a layer of fluid slips or tends to slip on adjacent layers in contact, the tangential force/viscous force acting between two adjacent layers try to stop the relative motion between them.

So The property of a fluid due to which it opposes the relative motion between its different layers is called viscosity. 

Viscosity is also known as fluid friction or internal friction.

  • Velocity gradient -

It is defined as the ratio of change in velocity to change in height.

I.e Velocity \ gradient=\frac{chane \ in \ velocity}{change \ in \ height}

For the above figure

Layer AB is at rest

While Layer CD is having velocity v and is at a distance x from layer AB

Similarly, Layer MN is having velocity (v+dv) and is at a distance (x+dx)  from layer AB

Then Velocity gradient is given as Velocity \ gradient= \frac{dv}{dx}

Means Velocity gradient denotes the rate of change of velocity with distance x. 

 

  • Viscous Force-

In case of a steady flow of fluid, the force between the fluid layers opposing the relative motion is called viscous force.

  1. Viscous force directly proportional  to the area

I.e F\alpha A

Where A is the area 

  1. Viscous force directly proportional  to the Velocity gradient

I.e F\alpha \frac{dv}{dx}

So we can write 

F\alpha \frac{Adv}{dx}= F=-\eta A \frac{dv}{dx}

Where A -Area

F -Viscous force

\eta =Co-efficient \ of \ viscosity

v -Velocity\: of \: liquid

x\ -\ Distance\ from\ refrence\ point 

And here Negative sign shows viscous force acts opposite to flow of liquid

  • Coefficient of viscosity-

From the equation F=-\eta A \frac{dv}{dx}

If \ A=1 \ and \ \frac{dv}{dx}=1\\ then \ \ \eta =F

So the coefficient of viscosity is defined as the viscous force acting per unit area between two layers moving with unit velocity gradient.

  1. Coefficient of viscosity shows the nature of liquids.

  2. Unit of viscosity is dyne -s -cm^{-2}\: or\: Poise in CGS system

And  Newton \:- S - m^{-2}\ or\ Poiseuille \: or \: decapoise in the SI system

And 1 decapoise = 10 Poise

  1. The dimension of viscosity is ML^{-1}T^{-1}

  2. The cause of viscosity in liquids is cohesive forces among molecule whereas, in gases, it is due to the diffusion of molecules.

  3. The viscosity of the liquid is much greater (about 100 times more) than that of gases.

  4. With an increase in pressure, the viscosity of liquids (except water) increases while For gases viscosity is practically independent of pressure. And the viscosity of water decreases with increase in pressure.

  5. The viscosity of gases increases with the increase of temperature, because on increasing temperature the rate of diffusion increases.

  6. The viscosity of liquid decreases with the increase of temperature, because the cohesive force between the liquid molecules decreases with the increase of temperature

 

  • Poiseuille’s Formula

For the stream-line flow of liquid in capillary/narrow tube, If a pressure difference (P) is maintained across the two ends of a capillary tube of length 'l ' and radius r as shown in figure

Then according to Poiseuille’s Formula

V= the volume of liquid coming out of the tube per second is

  1. Directly proportional to the pressure difference (P).

  2. Directly proportional to the fourth power of radius (r) of the capillary tube

  3. Inversely proportional to the coefficient of viscosity (\eta) of the liquid.

  4. Inversely proportional to the length (l) of the capillary tube.

And with the help of Dimension formula we get

V=\frac{KPr^4}{\eta l}

Where K  is the constant of proportionality

And experimentally it is found that K=\frac{\pi }{8}

So Poiseuille’s Formula is given as 

V=\frac{\pi Pr^4}{8\eta l}

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Viscosity

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Viscosity

Physics Part II Textbook for Class XI

Page No. : 262

Line : 47

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