Angle between two planes: A plane in geometry is a flat surface that extends in two dimensions indefinitely but has no thickness. The angle formed...
Angle between Two Planes: Definition, Angle Bisectors of a Plane, Examples
November 10, 2024Do you know that when a ball is thrown up into the air from the surface of the Earth by our hand, it does not have enough energy to escape? So it falls back down because of Gravity. The reason why space rockets fly in outer space is that they travel at a high velocity. This is called Escape Velocity.
The velocity required to maintain a circular orbit at the same altitude equals the square root of 2 (or around 1.414) times the escape velocity. Let’s study the escape velocity formula and its application in the article below.
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The equation for the escape velocity can be derived by applying the law of conservation of energy. This law states that the sum of total potential and kinetic energy of the objects are constant.
The escape velocity equation is also a function separating the object’s centres and the celestial body from which it is escaping.
The derivation starts with the initial gravitational potential energy and the object’s kinetic energy at the given altitude. This total energy is then compared with the potential and the kinetic energies at infinite separation to determine the escape velocity equation.
When a stone is thrown up, it goes up to a maximum height and then returns. As the particle goes up, the gravitational potential energy increases and the particle’s kinetic energy decreases. The particle will continue to go up till its kinetic energy becomes zero and will return from there.
Example:- A object of mass \(\left( m \right)\) is on the surface of the earth having mass \(\left( M \right)\) and radius \(\left( R \right)\), and its initial speed is equal to its escape velocity\(\left( {{v_e}} \right)\). Moreover, at its final state, it will be at an infinite distance away from the planet. Its speed will be negligibly low (for minimum initial velocity).
Now, after considering initial and final conditions:-
We have,
Initial:-
Let the initial velocity of the object is \(v_e\).
The initial kinetic energy of the object is \({K_i} = \frac{1}{2}mv_e^2\) , and
The gravitational potential energy of the earth–object system near the surface of the Earth is
\({U_i} = – \frac{{GMm}}{R}\)
Where
\(M = \) The Mass of the Earth,
\(m = \) The Mass of the Object
\(R = \) The Radius of the Earth.
Now,
Total Initial Energy \( = {\left( {{K_i} + {U_i}} \right)_{{\rm{initial }}}} = \frac{1}{2}mv_e^2 – \frac{{GMm}}{R}\quad \ldots (1)\)
Final:- When it reaches a height \(h\) above the earth’s surface,
The final speed becomes \(v\).
Then, the final kinetic energy \({K_f} = \frac{1}{2}m{v^2}\) and,
The gravitational potential energy \({U_f} = – \frac{{GMm}}{{R + h}}\)
Now,
Total Final Energy \(\left( {{K_f} + {U_f}} \right) = \frac{1}{2}m{v^2} – \frac{{GMm}}{{R + h}}\quad \ldots (2)\)
So, By conservation of energy :-
We have : –
\({K_i} + {U_i} = {K_f} + {U_f}\)
\( \Rightarrow \frac{1}{2}mv_e^2 – \frac{{GMm}}{R} = \frac{1}{2}m{v^2} – \frac{{GMm}}{{R + h}}\)
Now for minimum initial velocity, \({K_f} = 0\), because the final velocity is arbitrarily small, and the final distance approaches infinity so, \({U_f} = 0\).
Then, we can write our equation as:-
\(\frac{1}{2}mv_e^2 – \frac{{GMm}}{R} = 0 + 0\)
\( \Rightarrow \frac{1}{2}mv_e^2 = \frac{{GMm}}{R}\)
\( \Rightarrow {v_e} = \sqrt {\frac{{2GM}}{R}} \quad \ldots .(3)\)
This critical initial velocity is called the escape velocity
Orbital Velocity:-Orbital Velocity is the minimum velocity required to put the satellite into its orbit around the Earth.
For the derivation, let us consider a satellite of mass \((m)\) revolving around the earth having mass \((M)\) and the radius \((R)\) in a circular radius \((r)\) at a height \((h)\) from the surface of the Earth. To revolve around the Earth, the Gravitational force between the satellite and the Earth provides a centripetal force.
As we know that, According to the law of gravitation, the force of gravity on the satellite at an altitude of \(h\) is given by:-
\({F_g} = \frac{{GMm}}{{{{(r)}^2}}} = \frac{{GMm}}{{{{(R + h)}^2}}}\,\,\,(r = R + h) \ldots (4)\)
And, the centripetal force required by the satellite to keep it in its orbit is given as
\({F_r} = \frac{{mV_o^2}}{r} = \frac{{mV_o^2}}{{R + h}}\quad \ldots .(5)\)
So, the satellite will orbit the earth if,
\({F_{{\rm{Gravitational }}}} = {F_{{\rm{Centripetal }}}}\)
\( \Rightarrow \frac{{GMm}}{{{{(R + h)}^2}}} = \frac{{mV_o^2}}{{R + h}}\)
\( \Rightarrow V_o^2 = \frac{{GM}}{{R + h}}\)
\( \Rightarrow {V_o} = \sqrt {\frac{{GM}}{{R + h}}} \)
Now when the satellite revolves close to the surface of the Earth then,(\(h = 0\), on comparing with the radius of the earth), and the orbital velocity becomes:-
\( \Rightarrow {V_o} = \sqrt {\frac{{GM}}{R}} \ldots (6)\)
Where,
\(M = \) Mass of the Earth,
\(R = \) Radius of the Earth,
\(m = \) Mass of the Satellite
\({V_o} = \) Orbital Velocity of the Satellite
\(H = \) Height of the satellite above the earth’s surface
There exists a relationship between escape velocity and orbital velocity. The mathematical relation between the escape velocity and the orbital velocity will be:-
From the expression of the Escape velocity,
We have:- \({v_e} = \sqrt {\frac{{2GM}}{R}} \quad \cdots (3)\)
And from the expression of the orbital velocity,
We have:- \({V_o} = \sqrt {\frac{{GM}}{R}} \quad \cdots (4)\)
Now, On dividing Eq \((3)\) and Eq \((4)\)
We have:-
\(\frac{{{v_e}}}{{{V_o}}} = \sqrt {\frac{{2GM}}{R}} \times \sqrt {\frac{R}{{GM}}} \)
\( \Rightarrow {v_e} = \sqrt 2 {V_o}\quad \cdots (7)\)
The above relation is valid for any orbit at a distance of \(r\) from the earth’s centre.
To escape from the earth surface, we calculate the escape velocity as shown below:-
As we know that:-
The Mass of the Earth \( = 5.98 \times {10^{24}}\;{\rm{kg}}\)
The Radius of the Earth \( = 6.38 \times {10^6}\;{\rm{m}}\)
Newtons Gravitational Constant, \(G = 6.673 \times {10^{ – 11}}{\rm{N}}\,{{\rm{m}}^2}\;{\rm{k}}{{\rm{g}}^{ – 2}}\).
Now we can find the escape velocity from the earth using the escape velocity formula:-
\({v_e} = \sqrt {\frac{{2GM}}{R}} \)
Now substituting all the above values, we have:-
\({v_e} = \sqrt {\frac{{2 \times \left( {6.673 \times {{10}^{ – 11}}} \right)\left( {5.98 \times {{10}^{24}}} \right)}}{{6.38 \times {{10}^6}}}} \)
\( \Rightarrow {v_e} = \sqrt {\frac{{\left( {7.981 \times {{10}^{14}}} \right)}}{{6.38 \times {{10}^6}}}} \)
\( \Rightarrow {v_e} = \sqrt {1.251 \times {{10}^8}} \)
\( \Rightarrow {v_e} = 11184\;{\rm{m}}\,{{\rm{s}}^{ – 1}}\)
\( \Rightarrow {v_e} = 11.2\;{\rm{km}}\;{{\rm{s}}^{ – 1}}\)
Therefore, the escape velocity from the Earth is \(11.2\;{\rm{km}}\;{{\rm{s}}^{ – 1}}\).
Q.1. What is the escape velocity from the moon if the radius of the moon is given as \(1.74 \times {10^6}\;{\rm{m}}\)? And the mass of the moon is \(7.35 \times {10^{22}}\;{\rm{kg}}\).
Ans: Given:- Radius of the moon \( = 1.74 \times {10^6}\;{\rm{m}}\)
Mass of the moon is \( = 7.35 \times {10^{22}}\;{\rm{kg}}\)
Newtons Gravitational constant, \(G = 6.673 \times {10^{ – 11}}\;{\rm{N}}\;{{\rm{m}}^2}\;{\rm{k}}{{\rm{g}}^{ – 2}}\)
We have:-
\({v_e} = \sqrt {\frac{{2GM}}{R}} \)
\( \Rightarrow {v_e} = \sqrt {\frac{{2 \times \left( {6.673 \times {{10}^{ – 11}}} \right)\left( {7.35 \times {{10}^{22}}} \right)}}{{1.74 \times {{10}^6}}}} \)
\( \Rightarrow {v_e} = 2374\;{\rm{m}}\,{{\rm{s}}^{ – 1}}\)
\( \Rightarrow {v_e} = 2.37\;{\rm{km}}\;{{\rm{s}}^{ – 1}}\)
Therefore, the escape velocity from the Earth is \(2.37\;{\rm{km}}\;{{\rm{s}}^{ – 1}}\).
Q.2. If the mass of a planet is eight times the mass of the earth and its radius is twice the Earth’s radius, what will be the escape velocity of that planet?
Ans: Given:- Mass of the planet \({M_1} = 8 \times \) Mass of the Earth \(\left( {{M_2}} \right)\)
The radius of the planet \({R_1} = 2 \times \) Radius of the Earth \(\left( {{R_2}} \right)\)
The Mass of the Earth \( = 5.98 \times {10^{24}}\;{\rm{kg}}\)
The Radius of the Earth \( = 6.38 \times {10^6}\;{\rm{m}}\)
Newtons Gravitational Constant, \(G = 6.673 \times {10^{ – 11}}\;{\rm{N}}\;{{\rm{m}}^2}\;{\rm{k}}{{\rm{g}}^{ – 2}}\)
The Mass of the planet \( = 8 \times 5.98 \times {10^{24}}\;{\rm{kg}}\)
The Radius of the planet \( = 2 \times 6.38 \times {10^6}\;{\rm{m}}\)
Now using the escape velocity formula,
Now we have:-\({v_e} = \sqrt {\frac{{2GM}}{R}} \)
\( \Rightarrow {v_e} = \sqrt {\frac{{2 \times \left( {6.673 \times {{10}^{ – 11}}} \right)\left( {8 \times 5.98 \times {{10}^{24}}} \right)}}{{2 \times 6.38 \times {{10}^6}}}} \)
\( \Rightarrow {v_e} = 22368.96\;{\rm{m}}\,{{\rm{s}}^{ – 1}}\)
\( \Rightarrow {v_e} = 22.36\;{\rm{km}}\;{{\rm{s}}^{ – 1}}\)
The escape velocity of the planet is \(22.36\;{\rm{km}}\;{{\rm{s}}^{ – 1}}\).
We hope this detailed article on Escape Velocity helps you in your preparation. If you get stuck do let us know in the comments section below and we will get back to you at the earliest.