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Mechanical Properties of Fluids Test - 62

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Mechanical Properties of Fluids Test - 62
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  • Question 1
    1 / -0
    In a vessel of water a hole is made at a depth of $$3.5\ m$$ from the free surface. The velocity of efflux will be:
    Solution

  • Question 2
    1 / -0
    Water flows in a stream line manner through a capillary tube of radius a. The pressure difference being P and the rate of flow is Q. If the radius is reduced to $$\cfrac { a }{ 4 } $$ and the pressure is increased to 4P, then the rate of flow becomes
    Solution

  • Question 3
    1 / -0
    The angle of contact at the interface of water glass is $${0^ \circ }$$, Ethyl-alcohol glass is $${0^ \circ }$$ Mercury glass is $${140^ \circ }$$ and Methyl iodide is $${30^ \circ }$$. A glass capillary is put in a trough containing one of these for liquids it is observed that the meniscus is convex. the liquid in the trough is :      
    Solution

    Given , angle of contact $$(θ) = 140°$$ 

    Radius of tube $$(r) = 1 mm = 10⁻³ m$$ 

    Surface tension $$(S) = 0.465 N/m$$ 

    Density of mercury$$ (ρ) = 13.6 × 10³ kg/m³$$ 

    Height of liquid rise or fall due to surface tension $$(h)$$ 

                  $$ = 2S cos θ/rρg = 2 × 0.465 × cos 140°/1 × 10⁻³ × 13.6 × 10³ × 9.8$$ 

    $$= 2 × 0.465 × (- 0.7660) / 10⁻³ × 13.6 × 10³ × 9.8 $$ 

    $$= - 5.34 mm $$ 

    Hence, the mercury level will depressed by $$5.34 mm.$$

      A glass capillary is put in a trough containing one of these for liquids it is observed that the meniscus is convex. the liquid in the trough is Ethyl alcohol.

  • Question 4
    1 / -0
    A tank is filled with two immiscible  liquids of densities $$2\rho$$ and $$\rho$$ each of height $$h$$. Two holes are made to the side wall at $$\dfrac{h}{2}$$ and $$\dfrac{3h}{2}$$ from upper surface of the liquid, then the ratio of velocity of efflux of the liquids through the holes
    Solution
    Let the velocity at hole  is $${ v }_{ 1 }$$
    Height is $$\dfrac { h }{ 2 } $$
    Therefore velocity is, $${ v }_{ 1 }=\sqrt { 2g\dfrac { h }{ 2 }  } \\ $$ 
    Now pressure at hole 2 is
    P= $$h\rho g+\dfrac { h }{ 2 } \times 2\rho g$$
    Applying Bernoulli's theorem, $${ P }_{ o }+2h\rho g={ P }_{ o }+\dfrac { 1 }{ 2 } (2\rho ){ v }_{ 2 }^{ 2 }$$
    where $${ P }_{ o }$$ is the atmospheric pressure
    Velocity at hole 2 is $${ v }_{ 2 }=\sqrt { 2g\dfrac { 3h }{ 2 }  } =\sqrt { 3gh } $$
    Now, $$\dfrac { { v }_{ 2 } }{ { v }_{ 1 } } =\dfrac { \sqrt { 3gh }  }{ \sqrt { gh }  } $$
    $$\dfrac { { v }_{ 2 } }{ { v }_{ 1 } } $$= $$\sqrt { 3 } :1$$
     

  • Question 5
    1 / -0
    A cylindrical vessel has some water in it. A small hole at the bottom is now opened. The ratio of times it takes to become $$75\%$$ empty to completely empty is
    Solution

  • Question 6
    1 / -0
    Water is filled upto same height in two identical closed containers $$A$$ and $$B$$. Container $$A$$ has vacuum over the water while container $$B$$ has air over the water. At the same depth of both the containers there is an opening on which identical balloons $$A$$ and $$B$$ are attached as shown in the figure given below. Then

    Solution
    Solution:- (A) Balloon $$A$$ will bulge more than balloon $$B$$. 
    Since the container $$A$$ has vacuum over the water, thus water will cover the vacuum area first and hence the balloon $$A$$ will bulge more than balloon $$B$$.
  • Question 7
    1 / -0
    if the blood vessels in a human being acted as simple pipes what would be the difference in blood pressure between the blood in a $$1.8\ m$$ tall man's feet and in his head when he is standing? Assume the spacific gravity of blood to be $$1.06$$.
    Solution

  • Question 8
    1 / -0
    If $$A$$ denotes the area of free surface of a liquid and $$h$$ the depth of an orifice of area of cross-section $$a$$, below the liquid surface, then the velocity $$v$$ of flow through the orifice is given by:
    Solution

    $$v_{1}=$$ velocity of surface of liquid

    $$v_{2}=$$ velocity of liquid far om orifice

    Acc. to continuity theorem.

    $$A v_{1}=a v_{2} \Rightarrow \dfrac{A v_{1}}{a}=v_{2}$$

    $$\Rightarrow \dfrac{a v_{2}}{A}=v_{1}$$

    Acc. to Bernoulli's Theorem

    $$P_{0}+\rho g h+\dfrac{1}{2} \rho v_{1}^{2}=P_{0}+\rho g(0)+\dfrac{1}{2} \rho v_{L}^{2}$$

    $$\rho g h+\dfrac{1}{2} \rho\left[\dfrac{a^{2} v_{1}^{2}}{A^{2}}-v_{1}^{2}\right]=0$$

    $$\dfrac{v_{1}^{2}}{2}\left[\dfrac{A^{2}-a^{2}}{A^{2}}\right]=g h$$

    $$v_{1}=\sqrt{2 g h} \sqrt{\dfrac{A^{2}}{A^{2}-a^{2}}}$$

    Answer: $$ \sqrt{2 g h} \sqrt{ \dfrac{A^{2}}{A^{2}-a^{2}}}$$

  • Question 9
    1 / -0
    The angle of contact at the interface of water-glass is $$0^\circ $$. Ethyl alcohol-glass is $$0^\circ $$. Mercury-glass is $$140^\circ $$ and Methyl iodide-glass is $$30^\circ $$. A glass capillary is put in trough containing one of these four liquids. It is observed that the meniscus is convex. The liquid in the trough is: 

    Solution
    Given , 
    Angle of contact $$(\theta)=140^o$$
    Radius of tube $$(r)= 1 mm =10^{-3}m$$ 
    Surface tension $$(S) = 0.465N/m$$ 
    Density of mercury$$ (ρ) = 13.6 \times 10^{3} kg/m^3$$ 
    Height of liquid rise or fall due to surface tension (h) 
     $$=\dfrac{2Scos{\theta}}{rρg} $$ 

     $$=\dfrac{2 \times 0.465 \times cos140^o }{1×10^{-3} \times 13.6 \times 10^{3} \times 9.8}$$

     $$=2 \times 0.465 \times (−0.7660)/10^{-3} \times 13.6 \times 10^{3}  \times 9.8$$

     $$=−5.34\,mm $$

    Hence, the mercury level will depressed by $$5.34$$ mm.
    The meniscus of liquid in a capillary tube will be convex upward if angle of contact is obtuse. It is so when one end of glass capillary tube is immersed in a though of mercury.

  • Question 10
    1 / -0
    A balloon of volume $$1500{m}^{3}$$ and weighing $$1650 kg$$ with all its equipment is filled with helium (density $$0.2 kg/{m}^{3}$$). if the density of air is $$1.3 kg/{m}^{3}$$, the pull on the rope tied to the ballon will be 
    Solution

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