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Important Derivations: Gravitation | Physics for SSS 3 PDF Download

Relation between Gravitational Field Intensity and Gravitational Potential


Integral Form:
V =
Important Derivations: Gravitation | Physics for SSS 3
( If E is given and V has to be found using this formula)

Differential Form:
E = -dV/dr (If V is given and E has to be found using this formula)
Important Derivations: Gravitation | Physics for SSS 3
(components along x, y and z directions).

Gravitational Potential of a Point Mass

Consider a point mass M, the gravitational potential at a distance ‘r’ from it is given by;
V = – GM/r.

Gravitational Potential of a Spherical Shell


Consider a thin uniform spherical shell of the radius (R) and mass (M) situated in space. Now,
Case 1: If point ‘P’ lies inside the spherical shell (r<R): 
As E = 0, V is a constant.
The value of gravitational potential is given by, V = -GM/R.

Case 2: If point ‘P’ lies on the surface of the spherical shell (r=R): 
On the surface of the earth, E = -GM/R2.
Using the relation
Important Derivations: Gravitation | Physics for SSS 3
over a limit of (0 to R), we get,
Gravitational Potential (V) = -GM/R.

Case 3: If point ‘P’ lies outside the spherical shell (r>R): 
Outside the spherical shell, E = -GM/r2.
Using the relation
Important Derivations: Gravitation | Physics for SSS 3
over a limit of (0 to r), we get,
V = -GM/r.

Gravitational Potential of a Uniform Solid Sphere

Consider a thin, uniform solid sphere of radius (R) and mass (M) situated in space. Now,
Case 1: If point ‘P’ lies inside the uniform solid sphere (r < R): 
Inside the uniform solid sphere, E = -GMr/R3.
Using the relation
Important Derivations: Gravitation | Physics for SSS 3
over a limit of (0 to r).
The value of gravitational potential is given by,
V = -GM [(3R2 – r2)/2R2]

Case 2: If point ‘P’ lies on the surface of the uniform solid sphere ( r = R ):
On the surface of a uniform solid sphere, E = -GM/R2. Using the relation
Important Derivations: Gravitation | Physics for SSS 3
over a limit of (0 to R) we get,
V = -GM/R.

Case 3: If point ‘P’ lies outside the uniform solid sphere ( r> R): 
Using the relation over a limit of (0 to r), we get, V = -GM/R.

Case 4: Gravitational potential at the centre of the solid sphere is given by V =(-3/2) × (GM/R).

Gravitational Self Energy

The gravitational self-energy of a body is defined as the work done by an external agent in assembling the body from the infinitesimal elements that are initially at an infinite distance apart.

Gravitational self energy of a system of ‘n’ particles:
Let us consider n particle system in which particles interact with each other at an average distance ‘r’ due to their mutual gravitational attraction; there are n(n – 1)/2 such interactions, and the potential energy of the system is equal to the sum of the potential energy of all pairs of particles, i.e.,

Important Derivations: Gravitation | Physics for SSS 3

Solved Problems

Example 1. Calculate the gravitational potential energy of a body of mass 10 kg and is 25 m above the ground.
Solution:
Given, Mass m = 10 Kg and Height h = 25 m
G.P.E is given as,
U = m × g × h = 10 Kg 9.8 m/s2 × 25 m = 2450 J.

Example 2. If the mass of the earth is 5.98 ×1024 kg and the mass of the sun is 1.99 × 1030 kg, and the earth is 160 million km away from the sun, calculate the GPE of the earth.
Solution:
Given, the mass of the Earth (m) = 5.98 × 1024 Kg and mass of the Sun (M) = 1.99 × 1030 Kg
The gravitational potential energy is given by:
U = -GMm/r
U = (6.673 ∗ 10-11 ∗ 5.98 ∗ 1024 ∗1.99∗1030)/(160∗109) = 4963 x 1030 J

Example 3. A basketball weighing 2.2 kg falls off a building to the ground 50 m below. Calculate the gravitational potential energy of the ball when it arrives below.
Solution:
GPE = (2.2 kg)(9.8 m/s2)(50 m) = 1078 J.

Example 4:
A 2 kg body free falls from rest from a height of 12 m. Determine the work done by the force of gravity and the change in gravitational potential energy. Consider the acceleration due to gravity to be 10 m/s2.
Solution:
Since, W = mgh
Substituting the values in the above equation, we get
W = 2 × 12 × 10 = 240 N
The change in gravitational potential energy is equal to the work done by gravity.
Therefore, Gravitational Potential Energy= 240 Joule.

Orbital Velocity Derivation

Orbital velocity is defined as the minimum velocity a body must maintain to stay in orbit.

Due to the inertia of the moving body, the body has a tendency to move on in a straight line. But, the gravitational force tends to pull it down. The orbital path, thus elliptical or circular in nature, represents a balance between gravity and inertia. Orbital velocity is the velocity needed to achieve a balance between gravity’s pull on the body and the inertia of the body’s motion. For a satellite revolving around the Earth, the orbital velocity of the satellite depends on its altitude above Earth. The nearer it is to the Earth, the faster the required orbital velocity.
A satellite runs into traces of Earth’s atmosphere, at lower altitudes, which creates drag. This drag causes decay the orbit, eventually making the satellite to fall back into the atmosphere and burn itself up.

Derivation of Orbital Velocity

To derive the orbital velocity, we concern ourselves with the following two concepts:

  • Gravitational Force
  • Centripetal Force

It is important to know the gravitational force because it is the force that allows orbiting to exist. A central body exerts a gravitational force on the orbiting body to keep it in its orbit. Centripetal force is also important, as this is the force responsible for circular motion.
For the derivation, let us consider a satellite of mass m revolving around the Earth in a circular orbit of radius r at a height h from the surface of the Earth. Suppose M and R are the mass and radius of the Earth respectively, then r = R + h.
To revolve the satellite, a centripetal force of

Important Derivations: Gravitation | Physics for SSS 3
is needed which is provided by the gravitational force
Important Derivations: Gravitation | Physics for SSS 3
between the satellite and the Earth.
Therefore, equating both the equations, we get
Important Derivations: Gravitation | Physics for SSS 3
Simplifying the above equation further, we get
Important Derivations: Gravitation | Physics for SSS 3
……(eqn 1)
But
GM = gR2
, where g is the acceleration due to gravity.
Therefore,
Important Derivations: Gravitation | Physics for SSS 3
Simplifying the above equation, we get
Important Derivations: Gravitation | Physics for SSS 3
Let g’ be the acceleration due to gravity in the ( at a height h from the surface)
Important Derivations: Gravitation | Physics for SSS 3
Simplifying further, we get
Important Derivations: Gravitation | Physics for SSS 3
……(eqn 2)
Substituting (2) in (1), we get
Important Derivations: Gravitation | Physics for SSS 3

Derivation of Escape Velocity

Derivation of escape velocity is a very common concept in the kinematics topic of physics, and often questions related to it are included in school exams. The escape velocity derivation is also important to understand the in-depth concepts better and thoroughly understand the related concepts.
With the help of the escape velocity formula, it is possible to calculate the minimum velocity that an object requires to overcome a particular planet’s or object’s gravitational pull. Here, the derivation of escape velocity is given in a very simple and easy-to-understand way that can help students learn this concept more effectively.

Derivation of Escape Velocity:

Before checking the escape velocity derivation, it is important to know what escape velocity is and what are its related concepts. Check out the escape velocity of Earth for a detailed understanding of the minimum velocity required to overcome the earth’s gravitational pull.

Escape Velocity Formula:
Important Derivations: Gravitation | Physics for SSS 3
Derivation:
Assume a perfect sphere-shaped planet of radius and mass M. Now, if a body of mass is projected from a point on the surface of the planet. An image is given below for better understanding:
Important Derivations: Gravitation | Physics for SSS 3

In the diagram, a line from the centre of the planet i.e. O is drawn till (OA) and extended further away from the surface. In that extended line, two more points are taken as and at a distance of and dx, respectively from the centre O.
Now, let the minimum velocity required from the body to escape the planet b
ve
Thus, kinetic energy will be
Important Derivations: Gravitation | Physics for SSS 3
At point P, the body will be at a distance from the planet’s centre and the force of gravity between the object and the planet will be
Important Derivations: Gravitation | Physics for SSS 3
To take the body from to i.e. against the gravitational attraction, the work done will be-> 
Important Derivations: Gravitation | Physics for SSS 3
Now, the work done against the gravitational attraction to take the body from the planet’s surface to infinity can be easily calculated by integrating the equation for work done within the limits x = R to x = ∞.
Thus,
Important Derivations: Gravitation | Physics for SSS 3
By integrating it further, the following is obtained: 
Important Derivations: Gravitation | Physics for SSS 3
Thus, the work done will be:
Important Derivations: Gravitation | Physics for SSS 3
Now, to escape from the surface of the planet, the kinetic energy of the body has to be equal to the work done against gravity going from the surface to infinity. So, 
K.E. = W 
Putting the value for K.E. and Work, the following equation is obtained:
Important Derivations: Gravitation | Physics for SSS 3
From this equation, the escape velocity can be easily formulated which is: 
Important Derivations: Gravitation | Physics for SSS 3
Putting the value of g = GM/R2, the value of escape velocity becomes: 
Important Derivations: Gravitation | Physics for SSS 3
From these two equations, it can be said that the escape velocity depends on the planet’s radius and the planet’s mass only and not on the body’s mass.

Escape Velocity of Earth:
From the above equation, the escape velocity for any planet can be easily calculated if the mass and radius of that planet are given. For earth, the values of g and R are:
g = 9.8 ms-2
R = 63,781,00 m
So, the escape velocity will be:
Important Derivations: Gravitation | Physics for SSS 3
Escape Velocity of Earth= 11.2 km/s.

The document Important Derivations: Gravitation | Physics for SSS 3 is a part of the SSS 3 Course Physics for SSS 3.
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FAQs on Important Derivations: Gravitation - Physics for SSS 3

1. What is the relation between gravitational field intensity and gravitational potential?
Ans. Gravitational field intensity and gravitational potential are related by the equation: Gravitational field intensity (g) = -gradient of gravitational potential (Φ) This means that the gravitational field intensity at a point is equal to the negative gradient of the gravitational potential at that point.
2. How can we derive the orbital velocity of a satellite?
Ans. The orbital velocity of a satellite can be derived using the equation: Orbital velocity (V) = √(GM/R) where G is the gravitational constant, M is the mass of the central body, and R is the distance between the satellite and the center of the central body. This equation can be derived by equating the centripetal force required for circular motion to the gravitational force between the satellite and the central body.
3. What is the derivation of escape velocity?
Ans. The escape velocity can be derived using the equation: Escape velocity (Ve) = √(2GM/R) where G is the gravitational constant, M is the mass of the central body, and R is the distance between the object and the center of the central body. The derivation involves setting the kinetic energy of the object equal to the gravitational potential energy at the surface of the central body, and then solving for the escape velocity.
4. How are gravitational field intensity and gravitational potential related to each other mathematically?
Ans. Gravitational field intensity and gravitational potential are mathematically related by the equation: Gravitational field intensity (g) = -gradient of gravitational potential (Φ) This equation represents the fact that the gravitational field intensity at a point is equal to the negative gradient of the gravitational potential at that point. The negative sign indicates that the gravitational field intensity points towards the center of the gravitational field.
5. What are some important derivations related to the topic of gravitation?
Ans. Some important derivations related to gravitation include: - Derivation of Kepler's Laws from Newton's law of gravitation - Derivation of the period of a satellite orbiting a central body - Derivation of the gravitational potential energy of an object in a gravitational field - Derivation of the gravitational force between two point masses - Derivation of the acceleration due to gravity on the surface of a planet or celestial body.
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