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Gravitation Test - 54

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Gravitation Test - 54
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  • Question 1
    1 / -0
    If R is the radius of the earth, then the ratio of acceleration due to gravity on surface of the earth to acceleration due to gravity at height nR is:
    Solution
    Given 
    Radius of Earth$$=R$$
    Acceleration due to gravity $$g=\cfrac{GM}{R}$$
    Also
    $$g^{\prime}=g(\cfrac{1-2h}{R})$$
    Given height $$=nR$$
    $$g^{\prime}=g(\cfrac{1-2nR}{R})$$
    When body is raised by $$nR$$
    $$g^{\prime}=\cfrac{GM}{(R+nR)^2}\\g^{\prime}=\cfrac{GM}{R(1+n)^2}$$
    Now ratio of $$g$$ and $$g^{\prime}$$
    $$\Rightarrow(n+1)^2$$
  • Question 2
    1 / -0
    The value of $$g$$ on the earths surface is $$980\ cm/{sec}^{2}$$. Its value at a height of $$64\ Km$$ from the earth's surface is
    Solution
    At earth's surface. $$g=\dfrac{GM}{R^2}=9.8 m/s^2$$

    $$\dfrac{GM}{(6400 \times 10^3)^2}=9.8 m/s^2$$ ...(1)

    At a height 64 kms from earth's surface, 

    $$\dfrac{GM}{((6400+64) \times 10^3)^2}=g'$$ ...(2)

    (1) $$\div$$ (2)

    $$(\dfrac{6464}{6400})^2=\dfrac{9.8}{g'}$$

    $$g'=(\dfrac{6464}{6400})^2 \times 9.8=9.6069 m/s^2$$

    $$=960.69 cm/s^2$$
  • Question 3
    1 / -0
    The largest and the shortest distance of the earth from the sun are $$r_{1}$$ and $$r_{2}$$. Its distance from the sun when it is at perpendicular to the major-axis of the orbit drawn from the sun is:
    Solution
    From the property of ellipse
    $$\dfrac{2}{R}=\dfrac{1}{r_1}+\dfrac{1}{r_2}$$
    $$\dfrac{2}{R}=\dfrac{r_1+r_2}{r_1r_2}$$
    $$R=\dfrac{2r_1r_2}{r_1+r_2}$$

  • Question 4
    1 / -0
    The height of the point vertically above the earths surface at which the acceleration due to gravity becomes $$1\%$$ of its value at the surface is ($$R$$ is the radius of the earth)
    Solution

  • Question 5
    1 / -0
    At what height from the ground will be the value of $$g$$ be the same as 
    that in $$10 km$$ deep mine below the surface of earth.
    Solution
    Same changes in value of $$'g'$$ can be observe at a depth $$'x'$$ 
    and height $$'2x'$$ 
    given that the depth $$'d'=x=10km$$ 
    $$\therefore$$ the same charge can be observed at a height $$2x=20km$$
    Hence,
    the correct option  is $$A.$$
  • Question 6
    1 / -0
    A particle hanging from a spring stretches it by 1 cm at earth's surface. Radius of the earth is 6400 km. At a place 800 km above the earth's surface, the same particle will stretch the spring by 
    Solution
    The extension is $$x=\dfrac{mg}{k}$$
    At earth's surface, $$x=\dfrac{1}{100}=\dfrac{m \times \dfrac{GM}{R^2} }{k}$$..(1)
    At 800 km,above the earth's surface,
    $$x'=\dfrac{n\times \dfrac{GM}{(R+800)^2}}{k}$$ ..(2)
    (2) $$\div$$ (1)
    $$\dfrac{x'}{\dfrac{1}{100}}=\dfrac { \dfrac { GM }{ { \left( R+800 \right)  }^{ 2 } }  }{ \dfrac { GM }{ { R }^{ 2 } }  } =\dfrac { { R }^{ 2 } }{ { \left( R+800 \right)  }^{ 2 } }$$
    $$\Rightarrow x'\times 100=\dfrac { x' }{ { \left( 1+\dfrac { 800 }{ R }  \right)  }^{ 2 } } =\dfrac { x' }{ { \left( 1+\dfrac { 800 }{ 6400 }  \right)  }^{ 2 } } =\dfrac { 1 }{ 1.265 } \\ =0.79\times { 10 }^{ -2 }\quad m\\ =0.79\quad cm$$ 
  • Question 7
    1 / -0
    The value of acceleration due to gravity at a point P inside the earth and at another point Q outside the earth is g/2 .(g being acceleration due to gravity at the surface of the earth). Maximum possible distance in terms of radius of earth R between P and Q is:
    Solution
    In above the surface,
    $$\dfrac{g}{2} = \dfrac{GM}{(R+h)^2} ....1$$
    And for below the surface,
    $$\dfrac{g}{2} = \dfrac{GM}{(R-d)^2} ....2$$
    Equating both the above equation then we get,
    $$R^2 = h^2 + 2Rh$$
    And,
    $$R^2 = d^2 – 2Rd$$
    By solving quadratic for both hand d terms as:
    $$h = (\sqrt2 – 1)R$$
    And,
    $$d = (\sqrt2 + 1)R$$
    Thus,
    $$h + d = (\sqrt2 + 1)R + (\sqrt2 - 1)R$$
    $$ => 2\sqrt{2}R$$ meter.
  • Question 8
    1 / -0
    A body weight W Newton at the surface of the earth. Its weight at a height equal to half the radius of the earth will be :
    Solution
    Given, $$R=6400km,w=mg\Rightarrow g=\dfrac{w}{m}$$

    Now the weight of the body at the height is $$\dfrac{1}{2}R$$

    $$g'=g(1-\dfrac{d}{R})$$

    So the weight of the body at the $$\dfrac{1}{2} R$$

    $$W'=W(1-\dfrac{R}{2R})=W\dfrac{R}{2R})=\dfrac{W}{2}$$
  • Question 9
    1 / -0
    The height at which the value of acceleration due to gravity becomes 50% of that at the surface of the earth. (Radius of the earth = 6400 km) is (approximately) :
    Solution
    The  new value of $$gravity$$ at a height $$h$$ is given as $$g\prime=\dfrac{gR^2}{(R+h)^2}$$ 
    As visible from the formula that incresing $$h$$ results in decresing gravity.
    So just put $$g\prime=g/2$$ i.e. 50% less than $$g$$ where $$g$$ is gravity at surface. so we get $$ g/2= \dfrac{gR^2}{(R+h)^2}$$  or $$ \dfrac{1}{2}= \dfrac{R^2}{(R+h)^2}$$  
    or $$\dfrac{2}{1}= \dfrac{(R+h)^2}{R^2}$$ or $$\sqrt[2]{2}= \dfrac{R+h}{R}=1+ h/R$$ putting values we get $$\dfrac{h}{R}= 1.414-1=0.414$$

     so $$h=0.414R=2649.6Km$$
    Option C is correct.


  • Question 10
    1 / -0
    The ratio of acceleration due to gravity at a depth $$h$$ below the surface of earth and at a height $$h$$ above the surface for $$h<< R$$
    Solution
    Above the surface, $$g'_{above}=\dfrac{GM}{(R+h)^2}$$ (at depth h)
    Inside the earth, $$g'_{below}=\dfrac{GM}{R^2}(1-\dfrac{h}{R})$$
    $$\dfrac{g'_{below}}{g'_{above}}=\dfrac{\dfrac{1}{R^2} (1-\dfrac{h}{R})}{\dfrac{1}{(R+h)^2}}=\dfrac { 1-\dfrac { h }{ R }  }{ \dfrac { 2 }{ { \left( 1+\dfrac { h }{ R }  \right)  }^{ 2 } }  } $$
    But for $$\dfrac { h }{ R } <<<1$$
    $$\dfrac{g'_{below}}{g'_{above}}$$=$$(1-\dfrac { h }{ R } ){ \left( 1+\dfrac { h }{ R }  \right)  }^{ 2 }$$
    $$=(1-\dfrac { h }{ R } ){ \left( 1+\dfrac { 2h }{ R } +{ \left( \dfrac { h }{ R }  \right)  }^{ 2 } \right)  }\\ =1+\dfrac { 2h }{ R } +{ \left( \dfrac { h }{ R }  \right)  }^{ 2 }-\dfrac { h }{ R } -2{ \left( \dfrac { h }{ R }  \right)  }^{ 2 }-{ \left( \dfrac { h }{ R }  \right)  }^{ 3 }\\ =1+\dfrac { h }{ R } $$
    It increases linearly with $$'h'$$
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