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Mechanical Properties of Fluids Test - 22

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Mechanical Properties of Fluids Test - 22
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  • Question 1
    1 / -0
    A piston of cross-sectional area $$100 cm^2$$ is used in a hydraulic press to exert a force of $$10^7$$ dyne on the water. The cross-sectional area of the other piston which supports an object having a mass of 2000 kg is :
    Solution
    As we know ,  1 dyne = $$10 ^{-5}$$ N  so $$ 10 ^{7} $$ dyne = 100 N 
    hence , for Hydraulic press we have  
    $$\dfrac{100N}{100 cm^{2}}$$ = $$\dfrac{2000g}{A}$$  $$\Rightarrow$$ Area = $$2\times 10 ^{4} cm^{2}$$
    So option C is correct.
  • Question 2
    1 / -0
    A solid sphere falls with a terminal velocity of 10 m/s in air. If it is allowed to fall in vacuum:
    Solution
    Terminal velocity is reached in air since there is viscous force while moving through air( viscous force is  balanced by the weight )
    In vacuum, terminal velocity is not achieved since velocity of the sphere will keep on increasing with time.
  • Question 3
    1 / -0
    A uniformly tapering vessel shown in figure, is filled with liquid of density  $$900 kg/m^3$$. The force that acts on the base of the vessel due to liquid is :

    Solution
    This cylinder so formed has volume exactly half the total volume,
    $$\therefore$$ force due to liquid
    $$= 2\times A \times 8gh$$
    $$= 2\times 10^{-3} \times 9.8\times 900\times 0.4$$
    $$= 7.056\ N = 7.2\ N$$ (Taking $$g = 10\ m/s^{2})$$.

  • Question 4
    1 / -0
    A girl stands on a box having 60 cm length, 40 cm breadth and 20 cm width in three ways. The pressure exerted by the box will be:
    Solution
    The force exerted by the box on base=Weight of object=$$W$$
    The pressure that it exerts on the base$$=\dfrac{W}{A}$$
    where $$A$$ is the area of the base.
    Hence the pressure is maximum for smallest area of the base, which is when formed by breadth and width.
  • Question 5
    1 / -0
    Equal volumes of two immiscible liquids of densities $$\rho$$ and $$2\rho$$ are filled in a vessel as shown in figure. Two small holes are punched at depth $$\frac{h}{2}$$ and $$\dfrac{3h}{2}$$ from the surface of lighter liquid. If $$v_1$$ and $$v_2$$ are the velocities of a flux at these two holes, then $$v_1/v_2$$ is:

    Solution
    Here, two small holes are punchesd at depth $$\frac{h}{2}$$ and $$\frac{3h}{2}$$ from the surface of lighter liquid. Hence, the height of first hole from the surface of lighter liquid is
    $$h_1 = \dfrac{h}{2}$$
    and the height of second hole from the first hole is(i.e. from surface of remaining liquid)
    $$h_2 = \dfrac{3h}{2} - \dfrac{h}{2} = h$$
    Now, we have the velocity of flux from first hole is
    $$v_1 = \sqrt 2h_1g$$
    $$v_1 = \sqrt 2(\frac{h}{2})g$$
    $$v_1 = \sqrt hg$$
    Also, the velocity of flux from second hole is
    $$v_2 = \sqrt 2h_2g$$
    $$v_2 = \sqrt 2hg$$
    Therefore,
    $$\dfrac{v_1}{v_2} = \dfrac{\sqrt hg}{\sqrt 2hg}$$
    $$\dfrac{v_1}{v_2} = \dfrac{1}{\sqrt 2}$$
  • Question 6
    1 / -0
    With the increase in the area of contact of an object, the pressure:
    (Note : Thrust remains same)
    Solution
    Since,
    $$P = \frac{F}{A}$$
    Thus pressure is inversely proportional to area,
    $$i.e. \,\,P \propto \frac{1}{A}$$
    With the increase in the area of contact of an object the pressure decreases because pressure is inversely proportional to area of contact.
  • Question 7
    1 / -0
    Figure shows water filled in a symmetrical container. Four pistons of equal area $$A$$ are used at the four openings to keep the water in equilibrium. Now an additional force $$F$$ is applied at each piston. The increase in the pressure at the centre of the container due to this addition is

    Solution
    The four pistons are initially in equilibrium. As additional force $$F$$ is applied to each piston, the pressure in the fluid at each point must be increased by $$F.A$$ so that each piston retains state of equilibrium.
    Thus, the increment in the pressure at each point is
    $$\Delta P=\dfrac {F}{A}$$ (by Pascal's law)
    So, the pressure increment at the centre is  $$ 4\dfrac {F}{A}$$

  • Question 8
    1 / -0
    A Cylindrical vessel of cross-sectional area $$1000cm^{2}$$, is fitted with a frictionless piston of mass 10 kg, and filled with water completely. A small hole of cross-sectional area $$10mm^{2}$$ is opened at a point 50 cm deep from the lower surface of the piston. The velocity of effluent from the hole will be
    Solution
    Given that
    $$A = 1000 cm^3$$
    $$m = 10 Kg =10000 g$$
    $$A_h = 10 mm^2 = 0.1 m^2$$
    $$(H-h) = 50 cm$$
    Here, the force on piston is
    $$F = mg$$
    Hence, Increase in pressure on the liquid in the wider tube is
    $$P = \frac{F}{A} = \frac{mg}{A}$$
    Let, H is the level of water to which piston will move, thus
    $$P = H\rho g$$
    $$H = \frac{P}{\rho g}$$
    $$H = \frac{mg}{A\rho g} = \frac{m}{A\rho}$$  
    $$H = \frac{10000}{1000}$$.......($$\because \rho = 1$$)
    $$\therefore H = 10 cm$$ from surface of tube.
    Since, (H-h) = 50cm, h = 60cm = 0.6 m
    The velocity of effluent from the hole is
    $$v = \sqrt h\rho g$$
    $$v = (\sqrt 2gh) $$ 
    $$v = \sqrt (2)(9.8)(0.6) = 3.4 ms^{-1}$$ 
  • Question 9
    1 / -0
    Match column I with column II :
    List IList II
    Magnus energyPascal's Law
    Loss of EnergyArchimedes' principle
    Pressure is same at same level in a liquidViscous force
    Hydraulic MachinesLifting of asbestos roofs
    Solution
    Magnus effect talks of difference in pressure caused due to difference in velocity to lift a structure. Lifting of asbestos roofs during cyclonic storms in based on this phenomenon. So, $$A\rightarrow 4$$
    Viscous force is wet friction and brings loss in internal energy. So, $$B\rightarrow 3$$
    At the same level in the same liquid in a container, the pressure is the same according to Pascal's law. So, $$C\rightarrow 1$$
    Hydraulic machines use the idea of Pascal's law to transfer equal pressure in all directions from the free surface where it is applied. So, $$D\rightarrow 1$$
  • Question 10
    1 / -0
    The velocity of the liquid coming out of a small hole of a vessel containing two different liquids of densities $$2\rho$$ and $$\rho$$ as shown in the figure is

    Solution
    Pressure at (1), $$P_1=P_{atm}+\rho g(2h)+2\rho gh$$
    Applying Bernoulli's theorem between points (1) and (2),
    $$(P_{atm}+2\rho gh)+(2\rho) gh=P_{atm}+\dfrac {1}{2}(2\rho )v^2$$
    $$\Rightarrow v=2\sqrt {gh}$$

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