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Question: A rocket is fired from the earth towards the sun. At what distance from the earth’s centre is the gr...

A rocket is fired from the earth towards the sun. At what distance from the earth’s centre is the gravitational force on the rocket zero? Mass of the sun =2×1030kg=2\times {{10}^{30}}kg, mass of the earth =6×1024kg=6\times {{10}^{24}}kg. Neglect the effect of the other planets etc. (orbital radius =1.5×1011m=1.5\times {{10}^{11}}m).

Explanation

Solution

The force acting on a rocket at a particular distance from the centre of the earth is equal to the sum of forces of attraction of the rocket by the earth as well as the sun. This total force is equated to zero to find the distance of the rocket from the centre of the earth, where the gravitational force is zero.

Formula used:
The force of attraction between two bodies in space is given by
F=GMmR2F=-\dfrac{GMm}{{{R}^{2}}}
where
FF is the force of attraction
GG is the gravitational constant
MM is the mass of the first body
mm is the mass of the second body
RR is the distance between the first body and the second body

Complete answer:
Let us consider a rocket fired from the earth to the sun. Let the mass of the rocket be MM. We are asked to find the distance from the centre of the earth, at which the gravitational force on the rocket is zero. Let this distance be xx metres. We are provided that the mass of the sun is equal to 2×1030kg2\times {{10}^{30}}kg and the mass of the earth is equal to 6×1024kg6\times {{10}^{24}}kg. Let us call these masses Ms{{M}_{s}} and Me{{M}_{e}}, respectively. We are also given that the orbital radius of the earth is equal to 1.5×1011m1.5\times {{10}^{11}}m. This orbital radius of the earth is nothing but the distance between the centre of the sun and the centre of the earth. Let us call this distance rr meters. The distance between the rocket and the centre of the sun is equal to (rx)(r-x) meters as shown in the following figure.

The total force acting on the rocket is equal to the sum of the force of attraction due to the earth and the force of attraction of the sun on the rocket. Let us call this total force Ftotal{{F}_{total}}. Clearly,
Ftotal=Fe+Fs{{F}_{total}}={{F}_{e}}+{{F}_{s}}
where,
we have assumed that the force of attraction on the rocket due to the earth is Fe{{F}_{e}} and the force of attraction on the rocket due to the sun is Fs{{F}_{s}}. Let this be equation 1.
Now let us find the values of Fe{{F}_{e}} and Fs{{F}_{s}}.
The force of attraction between two bodies in space is given by
F=GMmR2F=-\dfrac{GMm}{{{R}^{2}}}
where
FF is the force of attraction
GG is the gravitational constant
MMis the mass of the first body
mm is the mass of the second body
RR is the distance between the first body and the second body

Let us use this general equation to find the values of Fe{{F}_{e}} and Fs{{F}_{s}}.
Clearly,
Fe=GMeMx2{{F}_{e}}=-\dfrac{G{{M}_{e}}M}{{{x}^{2}}} is the force of attraction between the earth and the rocket.
Fs=GMsM(rx)2{{F}_{s}}=\dfrac{G{{M}_{s}}M}{{{(r-x)}^{2}}} is the force of attraction between the sun and the rocket.
Note that the negative sign in the second expression vanishes.

Substituting these values in equation 1, we have
Ftotal=Fe+Fs=GMeMx2+GMsM(rx)2{{F}_{total}}={{F}_{e}}+{{F}_{s}}=-\dfrac{G{{M}_{e}}M}{{{x}^{2}}}+\dfrac{G{{M}_{s}}M}{{{(r-x)}^{2}}}
Let this be equation 2.

Now, we have to put Ftotal=0{{F}_{total}}=0in order to find the distance of the rocket from the earth where the gravitational force is zero.
Therefore, let us equate equation 2 to zero as follows.
Ftotal=GMeMx2+GMsM(rx)2=0{{F}_{total}}=-\dfrac{G{{M}_{e}}M}{{{x}^{2}}}+\dfrac{G{{M}_{s}}M}{{{(r-x)}^{2}}}=0
Clearly,
GMeMx2=GMsM(rx)2((rx)x)2=MsMe\dfrac{G{{M}_{e}}M}{{{x}^{2}}}=\dfrac{G{{M}_{s}}M}{{{(r-x)}^{2}}}\Rightarrow {{\left( \dfrac{\left( r-x \right)}{x} \right)}^{2}}=\dfrac{{{M}_{s}}}{{{M}_{e}}}
Let this be equation 3.

Substituting the values of Me,Ms{{M}_{e}},{{M}_{s}} and rr in equation 3, we have
((rx)x)2=MsMe=2×10306×1024=1063(rx)x=10331.732(rx)=103x{{\left( \dfrac{\left( r-x \right)}{x} \right)}^{2}}=\dfrac{{{M}_{s}}}{{{M}_{e}}}=\dfrac{2\times {{10}^{30}}}{6\times {{10}^{24}}}=\dfrac{{{10}^{6}}}{3}\Rightarrow \dfrac{\left( r-x \right)}{x}=\dfrac{{{10}^{3}}}{\sqrt{3}}\Rightarrow 1.732(r-x)={{10}^{3}}x

Substituting the value of rr, we have

1.732(1.5×1011)=x(103+1.732)103xx=1.732×1.5×1011103=2.598×108m1.732(1.5\times {{10}^{11}})=x({{10}^{3}}+1.732)\approx {{10}^{3}}x\Rightarrow x=\dfrac{1.732\times 1.5\times {{10}^{11}}}{{{10}^{3}}}=2.598\times {{10}^{8}}m

Here, we have taken
103+1.732103{{10}^{3}}+1.732\approx {{10}^{3}} because 1031.732{{10}^{3}}\gg 1.732
Therefore, the distance of the rocket from the centre of the earth at which the gravitational force is zero, when the rocket is fired from the earth to the sun is equal to
x=2.598×108mx=2.598\times {{10}^{8}}m

Note:
The force of attraction between two bodies in space follows sign convention. Here, in this question, the force of attraction on the rocket due to the earth is taken as negative because the rocket is moving away from the earth. At the same time, the force of attraction on the rocket due to the sun is taken as positive.