Electric and Gravitational Fields
(a) Features of Electric and Gravitational Fields
Field: A region where a force is exerted on objects due to a physical quantity like mass or charge.
Electric Field:
Electric field strength, E, is the force per unit charge on a small positive test charge placed at the point
Caused by electric charges.
Can be attractive or repulsive (like charges repel, opposite charges attract).
Coulomb’s Law:
The force between two point charges is given by:
F = 9 × 109 x Q1Q2 / r2
where 9 × 109 Fm-1 (k) is Coulomb’s constant, Q1 and Q2 are charges, and r is the separation.
Electric Field Strength E:
The force per unit positive charge at a point:
E = F / q
Gravitational Field:
Gravitational field strength, g, is the force per unit mass on a small test mass placed at the point
Caused by mass.
Always attractive.
Newton’s Law of Universal Gravitation:
The force between two masses is given by:
F = G x M1M2 / r2
where G is the gravitational constant, M1 and M2 are masses, and r is the separation.
Gravitational Field Strength g:
The force per unit mass at a point:
g = F / m
Inverse Square Law:
Both electric and gravitational forces decrease with the square of the distance (1/r2).
(b) Gravitational Field Outside a Spherical Body
Newton’s Shell Theorem:
Outside a uniform spherical mass (e.g., Earth), the gravitational field behaves as if all mass were concentrated at a single point at the centre.
Gravitational Field Strength Outside a Sphere:
g= GM / r2
where M is the total mass of the sphere and r is the radial distance from the centre.
(c) Field Lines (Lines of Force)
Field Lines:
Imaginary lines that show the direction of force in a field.
Electric Field Lines:
Point away from positive charges.
Point toward negative charges.
Gravitational Field Lines:
Always point toward the mass (gravity is always attractive).
Also radial for a point mass.
Density of Field Lines:
Indicates field strength (closer lines = stronger field).
(d) Equipotential Surfaces
Equipotential Surface:
A surface where the potential is the same at all points.
For a Point Charge or Mass:
Equipotential surfaces are spheres centred around the charge or mass.
Work Done on an Equipotential Surface:
Zero, since moving along the surface does not change potential energy.
Perpendicular to Field Lines:
Electric and gravitational equipotentials are always at right angles to the respective field lines.
(e) Calculating Net Potential and Resultant Field Strength
Electric Potential V:
The electric potential at a point due to a charge q is:
V=kq / r
For multiple charges, add potentials algebraically (since potential is a scalar quantity).
Gravitational Potential Φ:
The gravitational potential at a point due to a mass M is:
Φ = −GM / r
Always negative (gravity is always attractive).
Also follows superposition (sum of individual potentials).
Field Strength (Vector Quantity):
The net electric field at a point:
Enet = ∑ Ei
The net gravitational field at a point:
gnet = ∑ gi
Directions must be considered when summing vectors.
(f) Equation ΔUP=mgΔh Small Height Changes
Gravitational Potential Energy (UP) Change:
ΔUP=mgΔh
where g is constant over small height changes (near Earth’s surface).
For Large Distance Changes:
When g varies significantly, use:
UP = − GMm / r
instead of mgΔh