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Mechanical Properties of Fluids Test - 19

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Mechanical Properties of Fluids Test - 19
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  • Question 1
    1 / -0
    A tank with vertical walls is mounted so that its base is at a height of $$1.2 m$$ above the horizontal ground. The tank is filled with water to a depth $$2.8m.$$ A hole is punched in the side wall of thetank at a depth $$x \ m$$ below the surface of water to have maximum range of the emerging stream.Then the value of $$x$$ in meter is
    Solution
    Velocity  of  ejection  at  a  depth  x  is $$ \sqrt{2gx}$$
    time  of  flight  $$ = \sqrt{\dfrac{2H}{9}} = \sqrt{\dfrac{2(1.2+2.8-x)}{9}}$$
    $$ = \sqrt{\dfrac{2(4-x)}{9}}$$
    $$\therefore$$  Horizontal   Range  $$R = Vt = \sqrt{4 x (4-x)} $$
    $$ = 2\sqrt{x(4-x)}$$
    $$ \dfrac{dR}{dx} = 0  \Rightarrow  x= \dfrac{4}{2} = 2m$$
  • Question 2
    1 / -0
    A wind - powered generator converts wind energy into electrical energy. Assume that the generator converts a fixed fraction of the wind energy intercepted by its blades into electrical energy. For wind speed $$V$$, the electrical power output will be proportional to
    Solution
    Applying bernoullis eqn at point 1 and 2,
    $$p_{0}+\dfrac{1}{2}f v^{2}=p_{r},\left [  p_{0}=0\right ]$$
    So,
    force on the wing$$=p_{1}\times A=\dfrac{1}{2}f v^{2}$$
    So,
    work done on wing$$=\dfrac{1}{2}f v^{2}.\dfrac{v}{k}=Kv^{3}$$
    So,
    power output in wing $$\propto v^{3}$$
  • Question 3
    1 / -0
    Water stands at a height of $$100 cm$$ in a vessel whose side walls are vertical. A , B and C are holes at height $$80cm, 50 cm,$$ and $$20 cm$$ respectively from the bottom of the vessel. The correct system of water flowing out is :
    Solution
     At  any  height  h,  velocity  of  water  ejection $$ = \sqrt{2gh}$$
     time  of  flight $$ t = \sqrt{\dfrac{2(H-h)}{g}}$$
    $$\therefore$$  range  $$R = vT = \sqrt{2gh} \times \sqrt{\dfrac{2(H-h)}{g}} = 2\sqrt{h(H-h)}$$
    $$\therefore$$  for $$ h  = 20cm  ,  80cm $$  $$R$$  is  same.
    Therefore
    $$R$$  is  maximum  for  $$h  = \dfrac{H}{2}$$
  • Question 4
    1 / -0
    The pressure at the top of a building of height $$200m$$ is $$500kPa$$. The minimum pressure required at the base of the building to pump water to a closed tank on the top of the building is($$g=10m/s^{2}$$)
    Solution
    So,
    Minimum pressure required at the base of building
    $$=500\times 10^{3}+1000\times 10\times 200$$
    $$=500\times 10^{5}+20\times 10^{5}=25\times 10^{5}Pa$$
    $$=2.5\times 10^{6}Pa$$

  • Question 5
    1 / -0
    There are two holes $$O_{1}$$ and $$O_{2}$$ in a tank of height H. The water emerging from $$O_{1}$$ and $$O_{2}$$ strikes the ground at the same points,as shown in fig. Then:

    Solution
    At any height h below the surface , velocity of ejection $$ V = \sqrt{2gh}$$
    time of flight $$t = \sqrt{2g (H-h)}$$ 
    $$\therefore$$ Range $$R = vt = 2\sqrt{h (H-h)}$$ 
    If $$ R_{1} = R_{2} \Rightarrow h_{1}(H-h_{1}) = h_{2} (H-h_{2})$$ 
    $$ \Rightarrow h_{1} = H-h_{2}$$ 
    $$h_{1}+h_{2} =H$$
  • Question 6
    1 / -0
    A horizontal pipe of non-uniform cross-section allows water to flow through it with a velocity 1ms$$^{-1}$$ when pressure is 50kPa at a point. If the velocity of flow has to be 2 ms$$^{-1}$$ at some other piont,the pressure at that point should be:
    Solution
    Applying Bernoulli's equation at point 1 and point 2,

    $$\Rightarrow P_{1}+\dfrac{1}{2}\rho V_{1}^{2}=p_{2}+\dfrac{1}{2}\rho V_{2}^{2}$$
    $$\Rightarrow 50\times 10^{3}+\dfrac{1}{2}\times 10^{3}\left ( 1 \right )^{2}=p_{2}+\dfrac{1}{2}\times 10^{3}\times 4$$
    $$\Rightarrow 5\times 10^{4}+500-2000=p_{2}$$
    $$\Rightarrow p_{2}=48.5kp{a}$$
  • Question 7
    1 / -0
    Air of density $$1.3 kg m^{-3}$$ blows horizontally with a speed of $$108 km h^{-1}$$. A house has a plane roof of area $$40 m^{2}$$. The magnitude of aerodynamic lift on the roof is.
    Solution
    Applying bernoullis theorem above and below the roof,
    $$p_{1}+\dfrac{1}{2}+v_{1}^{2}=p_{2}$$
    $$\Rightarrow p_{2}-p_{1}=\dfrac{1}{2}+v_{1}^{2}=\dfrac{1}{2}\times 1.3\times \left ( 30 \right )^{2}$$
    $$\Rightarrow$$  difference  in  pressure $$=585 N/m^{2}...........2$$
    So,
    Magnitude of aerodynamic life$$=1\times Area$$
    $$=585\dfrac N{m^{2}}\times 40m^{2}$$
    $$2.34\times 10^{4}N$$
  • Question 8
    1 / -0
    In a plant, sucrose solution of coefficient of viscosity $$0.0015 N.m^{-2}$$ is driven at a velocity of $$10^{-3} m s^{-1}$$ through xylem vessels of radius  $$2\mu m$$ and length $$5 \mu m$$ . The hydrostatic pressure difference across the length of xylem vessels in $$Nm^{-2}$$ is :
    Solution
    Fow rate $$q=v\times \pi r^2$$
    also $$q=\dfrac{\pi Pr^4}{8\mu l}=v\pi r^2$$
    now $$v=10^{-3}m/s\ ,\mu=0.0015N/m^2\ ,r=2\times 10^{-6}m$$
    on solving above equation and putting value in SI unit we get
    $$P=15 N/m^2$$
  • Question 9
    1 / -0
    Two identical tall jars are filled with water to the brim. The first jar has a small hole on the side wall at a depth $$h/3$$ and the second jar has a small hole on the side wall at a depth of $$2h/3$$, where h is the height of the jar. The water issuing out from the first jar falls at a distance $$R_{1}$$ from the base and the water issuing out from the second jar falls at a distance $$R_{2}$$ from the base. The correct relation between $$R_{1}  \ and \  R_{2}$$ is
    Solution
    At  any  height  h  from  surface, velocity  $$V = \sqrt{2gh}$$
    Time  of  flight $$ t = \sqrt{\dfrac{2(H-h)}{g}}$$
    where $$H$$ is the total height of jar. 
    $$ \therefore$$  Range  $$R = V\times t$$
    $$R = 2\sqrt{h(H-h)}$$

    Given, $$   h_{1} = \dfrac{h}{3} \  and  \ H=h$$
    $$ \Rightarrow $$ $$R_1 = 2\sqrt{\dfrac{h}{3}(h-\dfrac{h}{3})}$$ $$  = \dfrac{2\sqrt{2}h}{{3}}$$
    For $$  \  h_{2} = \dfrac{2h}{3}\  and \  H=h$$
    $$ \Rightarrow $$ $$R_2 = 2\sqrt{\dfrac{2h}{3}(h-\dfrac{2h}{3})}$$ $$  = \dfrac{2\sqrt{2}h}{{3}}$$
    $$\therefore  R_{1} = R_{2}$$
  • Question 10
    1 / -0
    There is a hole at the bottom of a large open vessel.If water is filled upto a height $$h$$, it flows out in time $$t$$ .If water is filled to a height $$4h$$, it will flow out in time is
    Solution
    $$ v-u = -gt$$

    $$ \Rightarrow  0 - \sqrt{2gh} = -gt$$

    $$ t = \sqrt{\dfrac{2h}{g}}$$

    For height $$ h^{1} = 4h    t^{1} = \sqrt{\dfrac{2 (4h)}{g}} = 2t$$
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