13. Gravitational fields
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13.1 Gravitational field
13.1.1A gravitational field is an example of a field of force and define
• understand that a gravitational field is an example of a field of force and define gravitational field as force per unit mass
13.1.2A gravitational field by means of field lines
• represent a gravitational field by means of field lines
13.2 Gravitational force between point masses
13.2.1That, for a point outside a uniform sphere, the mass of the sphere may be
• understand that, for a point outside a uniform sphere, the mass of the sphere may be considered to be a point mass at its centre
13.2.2Newton’s law of gravitation F = Gm1m2 / r2 for the force between two point
• recall and use Newton’s law of gravitation F = Gm1m2 / r2 for the force between two point masses
13.2.3Circular orbits in gravitational fields by relating the gravitational force
• analyse circular orbits in gravitational fields by relating the gravitational force to the centripetal acceleration it causes
13.2.4A satellite in a geostationary orbit remains at the same point above the
• understand that a satellite in a geostationary orbit remains at the same point above the Earth’s surface, with an orbital period of 24 hours, orbiting from west to east, directly above the Equator
13.3 Gravitational field of a point mass
13.3.1Derive, from Newton’s law of gravitation and the definition of gravitational
• derive, from Newton’s law of gravitation and the definition of gravitational field, the equation g = GM / r 2 for the gravitational field strength due to a point mass
13.3.2G = GM / r 2
• recall and use g = GM / r 2
13.3.3G is approximately constant for small changes in height near the Earth’s
• understand why g is approximately constant for small changes in height near the Earth’s surface
13.4 Gravitational potential
13.4.1Gravitational potential at a point as the work done per unit mass in
• define gravitational potential at a point as the work done per unit mass in bringing a small test mass from infinity to the point
13.4.2Φ = –GM / r for the gravitational potential in the field due to a point mass
• use ϕ = –GM / r for the gravitational potential in the field due to a point mass
13.4.3The concept of gravitational potential leads to the gravitational potential
• understand how the concept of gravitational potential leads to the gravitational potential energy of two point masses and use EP = –GMm / r