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Gravitation Test - 28

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Gravitation Test - 28
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  • Question 1
    1 / -0
    The Earth is assumed to be a sphere of radius R. A platform is arranged at a height R from the surface of the Earth. The escape velocity of a body from this platform is fv, where v is its escape velocity from the surface of the Earth. The value of f is:
    Solution
    According to question and by using COME
    $$-\dfrac{GMm} {R + R} +\dfrac{1} {2}m\left (fv \right )^{2}$$ = $$0 + 0$$
    $$\Rightarrow fv$$ = $$\sqrt{\dfrac{GM} {R}}$$ but $$v = \sqrt{\dfrac{2GM} {R}}$$
    Therefore $$f\sqrt{\dfrac{2GM} {R}}$$ = $$\sqrt{\dfrac{GM} {R}} \Rightarrow f$$ = $$\sqrt{\dfrac{1} {2}}$$
  • Question 2
    1 / -0
    At a place, the value of 'g' is less by 1% than its value on the surface of the Earth (Radius of Earth, $$R=6400 km$$). The place is :
    Solution
    Let acceleration due to gravity at a place be $$g_d$$. If g is acceleration due to gravity at the surface then,
    $$g_d=g(1-\frac {d}{R})$$
    $$0.99g=g(1-\frac {d}{R})$$
    $$\frac {d}{R}=(0.01)$$
    $$d=0.01\times 6400=64 km$$ below the surface of earth
  • Question 3
    1 / -0
    Depth from the surface of the earth at which is acceleration due to gravity is 25% of acceleration due to gravity at the surface
    Solution
    g at the surface is given as $$g_s=\dfrac{4}{3}\pi GR\rho$$
    and at a depth d it is given as $$g_d=\dfrac{4}{3}\pi G(R-d)\rho$$
    Thus $$\dfrac{g_d}{g_s}=\dfrac{R-d}{R}$$
    Thus for the depth where acceleration is 25% of the surface gravity we get $$g_d$$ as $$\dfrac{g}{4}$$
    or
    $$\dfrac{g}{4}=g\left ( 1-\dfrac{d}{R} \right )\Rightarrow d=\dfrac{3}{4}\times R = 4800 km$$    (R is 6371 km)
  • Question 4
    1 / -0
    The variation of g  with height or depth (r) is shown correctly by the graph in the figure (where R = radius of the earth),
    Solution
    $$g_h$$ at height h is given by $$g_h = \dfrac{GM}{(R+h)^2} = GM(R+h)^{-2}$$ which denotes a parabola
    $$g_x $$ at depth x is given by
    $$g_x = g \left [ \dfrac{R-x}{R} \right ]$$
    Which denotes is straight line. So, option A is correct.
  • Question 5
    1 / -0
    A man weighs $$60 kg$$ at earth's surface. At what height above the earth's surface his weight becomes $$30 kg$$? (radius of earth  $$=6400 km$$).
    Solution
    Above the earth's surface, $$g_1 = \dfrac{g}{(1+\dfrac{h}{R})^2}$$
    But changed weight = half of its weight on the earth.
    $$\Rightarrow g_1 = \dfrac{g}{2}$$
    $$\therefore h = 2624 km.$$
  • Question 6
    1 / -0
    At what altitude will the acceleration due to gravity be $$25\%$$ of that at the earth's surface $$($$given radius of earth is $$R)$$?
    Solution

    Hint : Use the formula $$g'=\dfrac{GM}{(R+h)^{2}}$$

    $$\textbf{Step1: Expression of acceleration due to gravity on earth's surface}$$

    Force on the body placed on Earth's surface is
    $$F = \dfrac{GMm}{R^2}$$
    But, $$F = mg$$ hence,
    $$g = \dfrac{GMm}{R^2}$$
    where, variables have their usual meanings.
    $$\textbf{Step2: Calculation of altitude}$$
    Now, force on the body at geo-potential  height say $$h$$ (altitude) where the acceleration due to gravity is $$25\%$$ of that at the earth's surface i.e.
    $$\dfrac{25 g}{100} = \dfrac{g}{4}$$

    use the formula $$g'=\dfrac{GM}{(R+h)^{2}}$$
    Hence, we can write
    $$\dfrac{g}{4} = \dfrac{GM}{(R+h)^2}$$

    $$\dfrac{g}{4} = \dfrac{gR^2}{(R+h)^2}$$

    $$(R+h)^2 = 4R^2$$
    Taking roots for both sides we get
    $$R+h = 2R$$
    $$h = R$$

     

  • Question 7
    1 / -0
    When a satellite moves around the earth in a certain orbit, the quantity which remains constant is:
    Solution

    Hint: Use the Keplers law

    Explanation:

    According to Kepler's rules of planetary motion, when a satellite/planet moves around the Earth/Sun in a certain orbit, aerial velocity remains constant.  

    Correct option is (C) areal velocity

  • Question 8
    1 / -0
    Let $$\omega$$ be the angular velocity of the earth's rotation about its axis. Assume that the acceleration due to gravity on the earth's surface has the same value at the equator and the poles. An object weighed at the equator gives the same reading as a reading taken at a depth a below earth's surface at a pole $$(d << R)$$ The value of $$d$$ is
    Solution
    Let  $$g_e$$ be the acceleration due to gravity on surface of earth, $$g'$$ be  the acceleration due to gravity at depth $$d$$ below the surface of earth and is given by
    $$g^{'} = g_e \left(1 - \dfrac{d}{R} \right)$$ ............................(1)
    The acceleration due to gravity of an object on latitude(below the surface of earth) is
    $$g^{'} = g_e - \omega^2 R \cos \phi$$
    where, $$\phi$$ is the solid angle at the center of earth sustained by the object.
    At the equator, $$\phi = 0^\circ$$
    $$\therefore \cos \phi = 1$$
    Hence, 
    $$g' = g_e - \omega^2 R$$ ...............(2)
    From (1) and (2), we can write
    $$ g_e \left(1 - \dfrac{d}{R} \right) = g_e - \omega^2 R$$ 

    $$ \Rightarrow\dfrac{dg_e}{R} =  \omega^2 R$$

    $$ \Rightarrow d = \dfrac{\omega^2 R}{g_e}$$

  • Question 9
    1 / -0
    The condition for a uniform spherical mass $$M$$ of radius $$r$$ to be a black hole is $$(G=$$ gravitational constant, $$g=$$ acceleration due to gravity $$)$$.
    Solution
    For black hole, light even can not escape from the surface of the star.
    Since $$v_{esc} = \sqrt{ \dfrac{2GM}{r}}$$, putting $$v_{esc} =c$$ where c is the velocity of light $$c = \sqrt{ \dfrac{2GM}{r}}$$,
    Hence, $$\sqrt{ \dfrac{2GM}{r}} \ge c$$
  • Question 10
    1 / -0
    A spring balance is graduated on sea level. If a body is weighted at consecutively increasing heights from earth's surface, the weight indicated by the balance :
    Solution
    A spring balance is graduated on sea level. If a body is weighed with at consecutively increasing heights from earth's surface, the weight indicated by the balance will go on decreasing continuously. This is because value of g decreases with height.
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