
Let V and E denote the gravitational potential and gravitational field at a point, respectively. It is possible to have
This question has multiple correct options
(a) \[V = 0\]and \[E = 0\]
(b) \[V = 0\]and \[E \ne 0\]
(c) \[V \ne 0\]and \[E = 0\]
(d)\[V \ne 0\]and \[E \ne 0\]
Answer
123.3k+ views
Hint: Gravitational potential at a point is nothing but work done in bringing a unit mass from infinity separation to that particular point. Whereas, the gravitational field is the amount of force experienced by some mass placed in the gravitational potential at that point. Relation between field and potential is given by $E = - \dfrac{{dV}}{{dr}}$ where, E is field and V is potential and r is position variable.
Formula Used:
Relation between electric field and potential: $E = - \dfrac{{dV}}{{dr}}$ ……(1)
Where,
V is potential at the given point differentiated with respect to distance from the source.
Complete step by step answer:
Given:
1. Potential at a point: V
2. Electric field at a point: E
To find: The possible combinations of V and E.
Step 1:
In case the point at which the electric field and potential is being measured is at infinite distance from the source: \[V = 0\]. Putting \[V = 0\]in eq (1), we get \[E = 0\]. So, option (a) is correct.
Step 2:
In case the point lies inside a spherical shell of mass M and radius R, gravitational potential will be given by: $V = \dfrac{{GM}}{R}$, where G is gravitational constant. Here, the potential is constant as it does not depend on the distance from the source. Now, using eq (1):
$
E = - \dfrac{{d(\dfrac{{GM}}{R})}}{{dr}} \\
E = 0 \\
$
In this case, \[V \ne 0\]and \[E = 0\], so option (c) is also correct.
Step 3:
In the general case, when V depends on r, its derivative(E) will also be a function of r. For example, Potential for a point outside a spherical shell located at a distance r from the centre will be given by: $V = \dfrac{{GM}}{r}$. Use eq (1) to find E:
$
E = - \dfrac{{d(\dfrac{{GM}}{r})}}{{dr}} \\
E = \dfrac{{GM}}{{{r^2}}} \\
$
Here, \[V \ne 0\]and \[E \ne 0\], so option (d) is also correct.
Final Answer
The options (a), (c), (d) are correct.
Note: It is remarkable to notice there is one to one correspondence between field properties of gravitational field and electric field. Only difference is the electric field can be repulsive as well but the gravitational field is always attractive.
Formula Used:
Relation between electric field and potential: $E = - \dfrac{{dV}}{{dr}}$ ……(1)
Where,
V is potential at the given point differentiated with respect to distance from the source.
Complete step by step answer:
Given:
1. Potential at a point: V
2. Electric field at a point: E
To find: The possible combinations of V and E.
Step 1:
In case the point at which the electric field and potential is being measured is at infinite distance from the source: \[V = 0\]. Putting \[V = 0\]in eq (1), we get \[E = 0\]. So, option (a) is correct.
Step 2:
In case the point lies inside a spherical shell of mass M and radius R, gravitational potential will be given by: $V = \dfrac{{GM}}{R}$, where G is gravitational constant. Here, the potential is constant as it does not depend on the distance from the source. Now, using eq (1):
$
E = - \dfrac{{d(\dfrac{{GM}}{R})}}{{dr}} \\
E = 0 \\
$
In this case, \[V \ne 0\]and \[E = 0\], so option (c) is also correct.
Step 3:
In the general case, when V depends on r, its derivative(E) will also be a function of r. For example, Potential for a point outside a spherical shell located at a distance r from the centre will be given by: $V = \dfrac{{GM}}{r}$. Use eq (1) to find E:
$
E = - \dfrac{{d(\dfrac{{GM}}{r})}}{{dr}} \\
E = \dfrac{{GM}}{{{r^2}}} \\
$
Here, \[V \ne 0\]and \[E \ne 0\], so option (d) is also correct.
Final Answer
The options (a), (c), (d) are correct.
Note: It is remarkable to notice there is one to one correspondence between field properties of gravitational field and electric field. Only difference is the electric field can be repulsive as well but the gravitational field is always attractive.
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