All objects with mass create a gravitational field around them
The field extends all the way to infinity, but it gets weaker as the distance from the centre of mass if the object increases becoming negligible at long distances
Any other object with mass placed in a gravitational field will experience an attractive force towards the centre of mass of the object creating the field
Gravitational field strength --> The gravitational force exerted per unit mass on a small object placed at that point within the field
g = F/m
Gravitational field patterns can be mapped around an object with gravitational field lines
These lines don't cross, and the arrows on the lines show the direction of the field, which is the direction of the force on a mass at that point in the field
Gravitational force is always attractive, the direction of the gravitational field is always towards the centre of mass of the object producing the field
A stronger field is represented by field lines that are closer together
The field lines around a spherical mass form a radial field
If the field lines are parallel & equidistant, the field is said to be a uniform gravitational field
In a uniform field, the gravitational field strength doesn't change
Newton's law of gravitation states the force between 2 point masses is:
directly proportional to the product of the masses
inversely proportional to the square of their separation
F is directly proportional Mm/r^2
-G shows that gravitational force is attractive
F = -GMm/r^2
The attractive force F between objects decreases with distance in an inverse - square relationship
Multiple objects:
If several objects are involved, the resultant force can be determined by vector addition
The gravitational field strength g at a distance r from the centre of an object of mass M is:
g = -GM/r^2
In a radial field the gravitational field strength at a point is:
directly proportional to the mass of the object creating the gravitational field
inversely proportional to the square of the distance from the centre of mass of the object
Kepler's1st law: The orbit of a planet is an ellipse with the sun at one of the 2 foci
An ellipse is a elongated circle with 2 foci. The orbits of all the planets are elliptical
The orbits have a low eccentricity ( a measure if how elongated the circle is)
Kepler's2nd law: A line segment joining a planet & the sun sweeps out equal areas during equal intervals of time
Kepler's3rd law: The square of the orbit period T of a planet is directly proportional to the cube of its average distance r from the sun
T^2 = (4 x pi^2 / GM ) x r^3
the ratio T^2 / T^3 is a constant and equal to 4 x pi^2 / GM
the gradient of a graph of T^2 against r^3 must be equal to 4 x pi^2 / GM
For any satellite in orbit, the gravitationalforce F is given by
F = mv^2 / r = GMm / r^2
Since the only force acting on a satellite is the gravitationalattraction between it & the Earth, it is always falling towards the Earth
As it is travelling so fast, it travels such a great distance that as it falls the Earth curves away beneath it, keeping it at the same height above the surface
v^2 = GM / r
Uses of satellites:
Communications: satellite phones ( not mobile phones), TV, some types of satellite radio
Military uses: reconnaissance
Scientific research
Weather & climate: predicting & monitoring the weather across the globe & monitoring long - term changes in climate
Global positioning
Geostationary satellites:
be in orbit above the Earth's equator
rotate in the same direction as the Earth's rotation
have an orbital period of 24 hours
Gravitational potential Vg --> Work done per unit mass to move an object to that point from infinity
Infinity refers to a distance so far from the object producing the gravitational field that the gravitational field strength is zero
Gravitational potential is a scalar quantity - it only has magnitude
All masses attract each other. It takes energy, external work must be done, to move objects apart
Gravitational potential is a maximum at infinity
All values if gravitational potential are negative
Gravitational potential in a radial field:
The gravitational potential at any point in a radial field around a point mass depends on 2 factors
The distance r from the point mass producing the gravitational field to that point
the mass M of the point mass
The gravitational potential Vg is directly proportional to M and inversely proportional to r
Vg = -GM / r
All values of Vg within the region of the gravitational field will be negative and when r tends to infinity the Vg = 0
Changes in gravitational potential:
Moving towards a point mass results in a decrease in gravitational potential
Moving away from a point mass results in an increase in gravitational potential
Gravitational potential energy --> work done to move the mass from infinity to a point in a gravitational field
E = mVg
E = -GMm / r
Escape velocity:
In order to escape the gravitational field of a mass like a planet, an object must be supplied with energy equal to the gain in gravitational potential energy needed to lift it out of the field
In order for the projectile to have just enough energy to leave the gravitational field, the loss of kinetic energy must equal the gain in gravitational potential energy
1/2mv^2 = GMm / r
The minimum velocity v for this condition to be met is called the escape velocity
V^2 = 2GM / r
The escape velocity on a given planet is therefore the same for all objects regardless of their mass