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Gravitation Test - 48

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Gravitation Test - 48
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  • Question 1
    1 / -0
    On a planet where $${ g }_{ planet }=0.2{ g }_{ earth }$$. What will be the difference in the height of column filled with mercury in a closed end manometer when the gas is filled withe pressure of $$2atm$$ on earth (Assuming:outside pressure to be $$1atm$$ on both planet; Volume of gas remain constant)
    Solution
    $$P=egh$$
    $$2atm=760\times2$$ mm of hg
    $$\Rightarrow\cfrac{P_1}{P_2}=\cfrac{e_1g_1h_1}{e_2g_2h_2}\\ \because P_1=P_2\& e_1=e_2\Rightarrow\cfrac{h_2}{h_1}=\cfrac{g_1}{g_2}\\ \quad\cfrac{h_2}{760\times2}=\cfrac{g}{0.2g}\\ \quad\Rightarrow h_2=\cfrac{760\times2}{0.2}=7600mm\\ \quad\quad=760cm$$
  • Question 2
    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

  • Question 3
    1 / -0
    A particle of mass M is situated at the centre of spherical shell of same mass and radius a. The gravitational potential at a point situated at a/2 distance from the centre will be
    Solution
    Let point $$A$$ is situated at $$a/2$$ distance from the center.
    Gravitational Potential at point $$A$$ due to spherical shell, $$V_1=-\dfrac{GM}{a}$$,
    Gravitational Potential at point $$A$$ due to mass $$M$$ at point $$O$$ , $$V_2=-\dfrac{GM}{(a/2)}=-\dfrac{2GM}{a}$$,
    $$\therefore $$ Total Gravitational Potential $$=V_1+V_2= -\dfrac{GM}{a} -\dfrac{2GM}{a}=-\dfrac{3GM}{a}$$

  • Question 4
    1 / -0
    Suppose(God forbid) due to some reason, the earth expands to make its volume eight-fold. What you expect your weight to be?
    Solution
    we know , gravity is
                      g= $$\dfrac{GM}{r^2}$$
        the radius of new one will become r'=2r
    then, g'=$$\dfrac{GM}{4r^2}$$
  • Question 5
    1 / -0
    KEPLER'S LAWS
    Which of the following orbits is a possible orbit for a planet?
    Solution

    Kepler’s first law of planetary motion is as follows:

    All planets move about the sun in in an elliptical orbit having sun at one of its foci. Also a radius vector joining any planet to the sun sweeps out equal areas in equal interval of time.

    An ellipse can be represented by the formula $$r=\dfrac{P}{1+\varepsilon \cos \theta }$$ where P is semi latus rectum, $$\varepsilon$$ is eccentricity and $$\theta $$ is the angle to the planet's current position from its closest approach.

     In options (a) and (b) sun is not at a focus while in (c) the planet is not in orbit around the sun. Only (d) represents the possible orbit for a planet.

  • Question 6
    1 / -0
    The height from earth's surface at which acceleration due to gravity becomes $$\dfrac {g}{4}$$ is (where $$g$$ is acceleration due to gravity on the surface of earth and $$R$$ is radius of earth).
    Solution
    We know that  $$g=\dfrac{GM_e}{R^2}$$

    And at height h from the earth surface $$ g_1=\dfrac{GM_e}{(R+h)^2}$$

    And here $$g_1=\dfrac{g}{4}$$

    So, $$ \dfrac{g}{4}=\dfrac{GM_e}{(R+h)^2}$$

    so, $$\dfrac{GM_e}{4R^2}=\dfrac{GM_e}{(R+h)^2}$$

    Hence, $$\dfrac{1}{4R^2}=\dfrac{1}{(R+h)^2}$$

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

    $$\implies\dfrac{R+h}{R}=2$$

    $$\implies R+h=2R$$

    $$\implies R=h$$

    Hence, at height equal to R from earth surface gravity will become $$\dfrac{g}{4}$$.
     Answer-(B)



  • Question 7
    1 / -0
    'G' represents
    I. Acceleration due to gravity.
    II. Weight
    III. Gravitational constant
    Which combination is correct?
    Solution
    $$G$$ denotes gravitational constant where as $$g$$ denotes acceleration due to gravity and weight is given by $$W=mg$$
  • Question 8
    1 / -0
    A smooth and bottomless tunnel is dug through the centre of earth. A particle is released from the surface of earth into the tunnel. Time to reach centre of tunnel is (approximately) equal to (where $$R =$$ Radius of earth).
    Solution
    Force on particle at any $$x$$ is $$\dfrac{GM'm}{x^2}$$
    But $$\dfrac{M'}{M}=\dfrac{x^3}{R^3}$$
    $$\dfrac{GM x^3 m}{R^3 x^2}=(\dfrac{GMm}{R^3})x$$
    Acceleration of particle, $$a=\dfrac{GM}{R^3}x=\dfrac{g}{R}x$$
    It is an SHM motion, $$T=2 \pi \sqrt{\dfrac{R}{g}}$$
    Time to reach center of earth  $$=\pi \sqrt{\dfrac{R}{g}}$$
    $$=3.14 \times \sqrt{\dfrac{6400 \times 10^3}{9.81}}=42.283$$ minutes
  • Question 9
    1 / -0
    From a solid sphere of mass $$M$$ and radius $$R$$ a spherical portion of radius $$\dfrac {R}{2}$$ is removed, as shown in the figure. Taking gravitational potential $$V = 0$$ at $$r = \infty$$, the potential at the centre of the cavity thus formed is : $$(G =$$ gravitational constant).

    Solution
    By superposition principle, $$v_1=\dfrac{-GM}{2R^3}[3R^2-(\dfrac{R}{2})^2]$$
    $$=-\dfrac{11GM}{8R^3}$$
    Also, $$v_2=-\dfrac{3}{2} \dfrac{G (M/8)}{(R/2)}=\dfrac{-3GM}{8R}$$
    The required potential is, $$v=v_1-v_2$$
    $$=-\dfrac{11GM}{8R}-(-\dfrac{3GM}{8R})$$
    $$V=-\dfrac{GM}{R}$$
  • Question 10
    1 / -0
    A hole is drilled along the earth's diameter and a stone is dropped into it. When the stone is at the centre of the earth, it has.
    Solution
    At the center of the earth everything is weightless as acceleration and potential energy vanish. So it has only mass.
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