It is the region around a mass upto which another mass can experience its influence.
Gravitational field is described by the two quantities as shown in diagram given below :
(a) Gravitational field intensity
6.2.1 Gravitational Field Intensity
The intensity of gravitational field at a point is the force acting per unit mass of a test particle kept at that point i.e. . The direction of is same as that of .
It is a unit vector whose direction is always towards the source mass.
6.2.2 Field Due to Uniform Thin Spherical Shell
Consider a thin spherical shell or radius R, mass M and of negligible thickness. Out of the spherical shell we consider a small ring of thickness Rdq. The shaded ring has mass dm=(M/2)sinq dq. The field at p due to this ring is
Case I (p is outside the shell, r > a)
We see that the shell may be treated as a point particle of the same mass placed at its centre to calculate the gravitational field at an external point.
(inside the shell, r < a).
We see that field inside a uniform spherical shell is zero.
6.2.3 Relation between gravitational field and potential
Suppose the gravitation field at a point due to a given mass distributed is . By definition the force on a particle of mass m when it is at distance.
As the particle is displaced from the work done by the gravitational force on it is
The change in potential energy during this displacement is
The change in potential is, by equation
If we work in Cartesian coordinates, we can write
Equation (1) may be written as
dV = – ex dx – ey dy – Ez dz
If y and z remain constant, dy = dz = 0
The symbol means partial differentiation with respect to x treating y and z to be constants.
It is defined as the work done in moving unit mass from infinity to that point against the field. If W work is done in moving a mass m then V = W/m.
Its units are Joule/kg. It is a scalar quantity. its proper sign is negative. In integral from gravitational potential is given by . The gravitational potential on the surface of a sphere of mass M & radius R is, V = – GM / R
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