An area in which an object experiences a non-contact force
Force fields
Can be represented as vectors, which describe the direction of the force that would be exerted on the object
Can be represented as diagrams containing field lines, the distance between field lines represents the strength of the force exerted by the field in that region
Force fields
Formed during the interaction of masses, static charge or moving charges
Types of force fields
Gravitational fields
Electric fields
Gravity
Acts on any objects which have mass and is always attractive
Newton's law of gravitation
The magnitude of the gravitational force between two masses is directly proportional to the product of the masses, and is inversely proportional to the square of the distance between them
Uniform gravitational field
Exerts the same gravitational force on a mass everywhere in the field
Radial gravitational field
The force exerted depends on the position of the object in the field
Gravitational field strength (g)
The force per unit mass exerted by a gravitational field on an object
Gravitational potential (V)
The work done per unit mass when moving an object from infinity to that point
Gravitational potential difference (ΔV)
The energy needed to move a unit mass between two points
Equipotential surfaces
Surfaces which are created through joining points of equal potential together, therefore the potential on an equipotential surface is constant everywhere
No work is done when moving along an equipotential surface
Gravitational potential (V)
Inversely proportional to the distance between the centres of the two objects (r)
The area under the gravitational field strength (g) vs distance (r) graph gives the gravitational potential difference
Kepler's third law
The square of the orbital period (T) is directly proportional to the cube of the radius (r)
Total energy of an orbiting satellite
Constant, made up of kinetic and potential energy
Escape velocity
The minimum velocity an object must travel at to escape the gravitational field at the surface of a mass
Synchronous orbit
Where the orbital period of the satellite is equal to the rotational period of the object it is orbiting
Geostationary satellite
Orbits directly above the equator with an orbital period of 24 hours, always staying above the same point on Earth
Low-orbit satellites
Have significantly lower orbits than geostationary satellites, travel much faster, and have smaller orbital periods
Coulomb's law
The magnitude of the force between two point charges in a vacuum is directly proportional to the product of their charges, and inversely proportional to the square of the distance between the charges
Air can be treated as a vacuum when using Coulomb's law, and for a charged sphere, charge may be assumed to act at the centre of the sphere
If charges have the same sign the force will be repulsive, and if the charges have different signs the force will be attractive
The magnitude of electrostatic forces between subatomic particles is magnitudes greater than the magnitude of gravitational forces
Electric field strength (E)
The force per unit charge experienced by an object in an electric field
The gravitational and electrostatic force between two protons with centres 2 pm (2 x 10^-12 m) apart are much larger
Calculating gravitational force
1. F = GMm/r^2
2. F = (6.67 x 10^-11 N m^2/kg^2) x (1.67 x 10^-27 kg) x (1.67 x 10^-27 kg) / (2 x 10^-12 m)^2 = 4.65 x 10^-41 N
Calculating electrostatic force
1. F = (1/4πε0) x (Q1 x Q2)/r^2
2. F = (1/4π x 8.85 x 10^-12 F/m) x (1.6 x 10^-19 C) x (1.6 x 10^-19 C) / (2 x 10^-12 m)^2 = 3.75 x 10^-5 N
Ratio of electric force over gravitational force
F_electric/F_gravitational = (3.75 x 10^-5 N) / (4.65 x 10^-41 N) = 8.05 x 10^35
The electrostatic force between the two protons is 8.05 x 10^35 times greater than the gravitational force
Calculating electric field strength in a uniform field
1. E = F/Q
2. E = V/d
Calculating electric field strength in a radial field
E = (1/4πε0) x Q/r^2
Electric field lines
Show the direction of the force acting on a positive charge
Uniform field has parallel and equally spaced field lines
Radial field has field lines that depend on the distance between the charges
Calculating work done by moving a charged particle between parallel plates
1. Work done = F x d
2. F = E x Q
3. d = ΔV/E
4. Work done = Q x ΔV
Charged particles in a uniform electric field follow a parabolic path, with positive charges moving in the direction of the field and negative charges moving opposite to the field
Absolute electric potential (V)
The potential energy per unit charge of a positive point charge at that point in the field
Calculating electric potential in a radial field
V = (1/4πε0) x Q/r
Electric potential difference (ΔV)
The energy needed to move a unit charge between two points
Work done in moving a charge across a potential difference is equal to the product of potential difference and charge</b>