Gravitation

NEET Physics · 96 questions · Page 10 of 10 · Click an option or "Show Solution" to reveal answer

Q91
Two objects of equal masses placed at certain distance from each other attracts each other with a force of F. If one-third mass of one object is transferred to the other object, then the new force will be :
A 29{2 \over 9} F
B 169{16 \over 9} F
C 89{8 \over 9} F
D F
Correct Answer
Option C
Solution

Let the masses are m and distance between them is l, then

F=Gm2l2F = {{G{m^2}} \over {{l^2}}}

. When 1/3rd mass is transferred to the other then masses will be

4m3{{4m} \over 3}

and

2m3{{2m} \over 3}

. so new force will be

F=G4m3×2m3l2=89Gm2l2=89FF' = {{G{{4m} \over 3} \times {{2m} \over 3}} \over {{l^2}}} = {8 \over 9}{{G{m^2}} \over {{l^2}}} = {8 \over 9}F
Q92
Assuming the earth to be a sphere of uniform mass density, the weight of a body at a depth d=R2d=\dfrac{R}{2} from the surface of earth, if its weight on the surface of earth is 200 N, will be: (Given R = radius of earth)
A 100 N
B 400 N
C 300 N
D 500 N
Correct Answer
Option A
Solution

The gravitational field strength, or equivalently, the weight of an object, decreases linearly from its surface value to zero at the center of a sphere of uniform mass density.

This is because only the mass inside the radius at which the object is located contributes to the gravitational force at that location.

If ( d=R2d = \dfrac{R}{2} ) is the depth below the surface of the Earth, then the radius of the sphere contributing to the gravitational force at that depth is ( Rd=RR2=R2R - d = R - \dfrac{R}{2} = \dfrac{R}{2} ).

Since the gravitational force (or weight) decreases linearly with the radius in a sphere of uniform density, the weight of the object at depth ( d=R2d = \dfrac{R}{2} ) is half its weight at the surface of the Earth.

So, if the weight of the body on the surface of the Earth is 200 N, its weight at depth ( d=R2d = \dfrac{R}{2} ) is half of that, or 100 N.

Therefore, the correct answer is 100 N.

Q93
Given below are two statements: one is labelled as Assertion A and the other is labelled as Reason R. Assertion A : A pendulum clock when taken to Mount Everest becomes fast. Reason R : The value of g (acceleration due to gravity) is less at Mount Everest than its value on the surface of earth. In the light of the above statements, choose the most appropriate answer from the options given below
A Both A and R are correct but R is NOT the correct explanation of A
B A is correct but R is not correct
C Both A and R are correct and R is the correct explanation of A
D A is not correct but R is correct
Correct Answer
Option D
Solution

When we go on the Mount Everest the value of gravitational acceleration decreases (g=g0(1+hRe)2)\left(g=\dfrac{g_{0}}{\left(1+\dfrac{h}{R_{e}}\right)^{2}}\right).

Therefore, the time period of oscillation (T=2πIg)\left(T=2 \pi \sqrt{\dfrac{I}{g}}\right) increases and the pendulum clock becomes slow thus the assertion is wrong but reason is correct.

Q94
The escape velocity of a body depends upon mass as
A m0{m^0}
B m1{m^1}
C m2{m^2}
D m3{m^3}
Correct Answer
Option A
Solution

Escape velocity,

ve=2gR=2GMRVem0{v_e} = \sqrt {2gR} = \sqrt {{{2GM} \over R}} \Rightarrow {V_e}\, \propto \,{m^0}

Where

M,RM,R

are the mass and radius of the planet respectively. In this expression the mass of the body

(m)(m)

is not present. The escape velocity is independent of the mass m or it depends on m0.

Q95
The height at which the acceleration due to gravity becomes g9{g \over 9} (where g=g= the acceleration due to gravity on the surface of the earth) in terms of R,R, the radius of the earth, is:
A R2{R \over {\sqrt 2 }}
B R/2R/2
C 2R\sqrt 2 \,\,R
D 2R2\,R
Correct Answer
Option D
Solution

Given that, at height h from ground the acceleration due to gravity becomes

g9{g \over 9}

. We know acceleration at earth surface due to gravity g =

GMR2{{GM} \over {{R^2}}}

and acceleration at height h due to gravity g' =

GM(R+h)2{{GM} \over {{{\left( {R + h} \right)}^2}}}

So

g9{{g} \over 9}

=

GM(R+h)2{{GM} \over {{{\left( {R + h} \right)}^2}}}

\Rightarrow

g9{{g} \over 9}

=

GMR2.R2(R+h)2{{GM} \over {{R^2}}}.{{{R^2}} \over {{{\left( {R + h} \right)}^2}}}

=

g.(RR+h)2g.{\left( {{R \over {R + h}}} \right)^2}
19=(RR+h)2\Rightarrow {1 \over 9} = {\left( {{R \over {R + h}}} \right)^2}
RR+h=13\Rightarrow {R \over {R + h}} = {1 \over 3}
3R=R+h\Rightarrow 3R = R + h

\therefore

h=2Rh = 2R
Q96
The mass of the moon is 1144\dfrac{1}{144} times the mass of a planet and its diameter is 116\dfrac{1}{16} times the diameter of a planet. If the escape velocity on the planet is vv, the escape velocity on the moon will be :
A v4\dfrac{\mathrm{v}}{4}
B v6\dfrac{\mathrm{v}}{6}
C V12\dfrac{\mathrm{V}}{12}
D v3\dfrac{\mathrm{v}}{3}
Correct Answer
Option D
Solution
Vescape =2GMRVplanet =2GMR=VVMoon =2GM×16144R=132GMRVMoon =VPlanet 3=V3\begin{aligned} & \mathrm{V}_{\text{escape }}=\sqrt{\frac{2 \mathrm{GM}}{\mathrm{R}}} \\ & \mathrm{V}_{\text{planet }}=\sqrt{\frac{2 \mathrm{GM}}{\mathrm{R}}}=\mathrm{V} \\ & \mathrm{V}_{\text{Moon }}=\sqrt{\frac{2 \mathrm{GM} \times 16}{144 \mathrm{R}}}=\frac{1}{3} \sqrt{\frac{2 \mathrm{GM}}{\mathrm{R}}} \\ & \mathrm{V}_{\text{Moon }}=\frac{\mathrm{V}_{\text{Planet }}}{3}=\frac{\mathrm{V}}{3} \end{aligned}
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