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Gravitation Test - 57

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Gravitation Test - 57
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  • Question 1
    1 / -0
    The height at which the weight of a body becomes $$\dfrac {1}{16}th$$, its weight on the surface of earth (radius $$R$$), is
    Solution
    weight w = mg 
    m = mass (constent)
    $$ \dfrac{w_{1}}{w_{2}} = \dfrac{g_{1}}{g_{2}}; g_{1} = \dfrac{GM}{R^{2}}$$
    $$ 9_{2} = \dfrac{GM}{(R+h)^{2}}$$ ;h = height
    So$$ \dfrac{w_{1}}{w_{2}} = \dfrac{(R+h)^2}{R^{2}}$$
    putting $$ \dfrac{w_{1}}{W_2} = 16 = \dfrac{(R+h)^{2}}{R^{2}}$$
    $$ \Rightarrow \dfrac{R+h}{R} = 4 \Rightarrow 1+\dfrac{h}{2} = 4 \Rightarrow \boxed{h = 3R }$$

  • Question 2
    1 / -0
    At what height above the surface of earth acceleration due to gravity becomes $$1 \ mm/s^2$$?
    [Take $$R$$ as radius of earth and acceleration due to gravity at the surface of earth $$g = 10 m/s^2$$]
    Solution

  • Question 3
    1 / -0
    If $$'R'$$ is the radius of the earth, then the height at which the weight of a body becomes $$\dfrac{1}{4}^{th}$$ of its weight on the surface of the earth is:
    Solution
    we know that acceleration due to gravity varies height h and the surface of the earth
    $${ g }^{ \prime  }=g\left( 1-\dfrac { 2h }{ R }  \right) $$
    hence the weight of the body 
    $$m{ g }^{ \prime  }=mg\left( 1-\dfrac { 2h }{ R }  \right) $$

    $$w^{ \prime  }=w\left( 1-\dfrac { 2h }{ R }  \right) $$

    $$w^{ \prime  }=w\left( 1-\dfrac { 2h }{ R }  \right) $$

    $$\dfrac { 1 }{ 4 } =\left( 1-\dfrac { 2h }{ R }  \right) $$

    $$\dfrac { 2h }{ R } =1-\dfrac { 1 }{ 4 } =\dfrac { 3 }{ 4 } $$

    $$h=\dfrac { 3R }{ 8 } $$


  • Question 4
    1 / -0
    A lift is descending with a constant velocity $$\ 'V'$$, A man in the lift drops a coin experiences an acceleration towards the floor equal to:
    Solution

  • Question 5
    1 / -0
    Two planet have radii in the ratio $$1:2$$ and densities in the ratio $$1:3$$. The value of the ratio between acceleration due to gravity on the first planet to that of the second planet is:
    Solution
    $$g=\dfrac{GM_p}{r^2}$$

    $$M_p=Density\times Volume=Density\times\dfrac{4\pi r^3}{3}$$
    $$g=\dfrac{G\times density\times 4\pi r^3}{3r^2}$$

    Thus g$$\propto r$$ and g$$\propto Density$$

    So,$$\dfrac{g_1}{g_2}=\dfrac{1\times 1}{2\times 3}=\dfrac{1}{6}$$ 
  • Question 6
    1 / -0
    A body weighs $$900$$N on the earth. Find its weight on a planet whose density is $$\dfrac{1}{3}^{st}$$ the density of earth and radius is $$\dfrac{1}{4}^{th}$$ that of the earth.
    Solution
    Weight of object on earth $$W = {\dfrac{GMm}{R^2}}$$

    Now, $$M = {\rho}V$$ =$${\dfrac{4\pi \rho R^{3}}{3}}$$

    $$\therefore W = {\dfrac{G \rho \pi R^{3} G m}{3 R^{2}}} = {\dfrac{4 \pi \rho R G m}{3}}$$

    $${\dfrac{W_P}{W_E}} = {(\dfrac{\rho_P}{\rho_E})}{(\dfrac{R_P}{R_E})}$$

             $$ = {\dfrac{1}{3}} \times {\dfrac{1}{4}}$$ = $${\dfrac{1}{12}}$$
     
    $${W_P} = {\dfrac{900}{12}} = 75 N$$

  • Question 7
    1 / -0
    The depth at which the value of acceleration due to gravity becomes $${\dfrac{1}{n}}$$ times the value at the surface is (R be the radius of the earth):
    Solution
    option C
    $${ g }^{ 1 }=g\left[ 1-\dfrac { d }{ R }  \right] $$

    $$\Longrightarrow \dfrac { g }{ n } =g\left[ 1-\dfrac { d }{ R }  \right] \Longrightarrow d=\left[ \dfrac { n-1 }{ n }  \right] R$$
  • Question 8
    1 / -0
    A particle when thrown. moves such that it passes from same height at $$2$$ and $$10 s$$, the height is:
    Solution

    If t1 and t2 are the time when the body is at the same height Then  $$h = \dfrac{1}{2} \times  g\times {t}_1\times  {t}_2$$ $$h = \dfrac{1}{2} \times  g\times {2}\times  {10}$$h = 10 g 

    So that the correct option is D






  • Question 9
    1 / -0
    The escape velocity of an object from the earth depends upon the mass of earth $$(M)$$, its mean density $$(\rho)$$, its radius $$(R)$$ and gravitational constant $$(G)$$, thus the formula for escape velocity is:
    Solution

  • Question 10
    1 / -0
    If the gravitational potential energy of two point masses infinitely away is taken to be zero then gravitational potential energy of a galaxy is 
    Solution

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