chapter 18 - gravitational fields Flashcards
field lines
- density of lines is prop to field strength
- always perp to surface
- never cross
- always attractive (gravitational)
gravitational fields
a region in space where any mass experiences a force of attraction
- act anything with a mass
- are infinite
- always attractive
- at surface are considered uniform
gravitational field strength
force per unit mass
generally g = F/m
for a point mass g = -GM/r²
radial fields equation
F = GMm/r²
F ∝1/r²
G = 6.67*10^-11 Nm^2kg^-2
uniform fields equation
F = mg
newtons law of gravitation
F ∝ Mm - prop to product of masses
F ∝ 1/r² - inversely prop to seperation squared
F = -GMm/r²
gravitational field strength graph
g against 1/r²
- always in neg quadrant
- straight line
g against r
- always in neg quadrant
- staight line down then curve back up
- straight line section until rE (assume uniform density)
satellites
- geostationary
- polar
geostationary
- orbital period 24h
- stay above same country + therefore are all at a specific height - equatorial orbit
- same direction as Earth
- uses: communications, weather prediction, GPS
- 35,768 km above Earths surface
polar
- pole to pole orbit
- low orbit - 200-1000km
- faster speeds
- cover a number of countries
- uses: spying, weather prediction
equipotentials
lines of equal gravitational energy
keplers 1st law
the orbit of a planet is an ellipse with the sun at one of the two foci
- but most orbits have low eccentricity and can be modelled as circles
keplers 2nd law
a line segment joining a planet and the sun sweeps out equal areas during equal time intervals
(planets travel faster nearer the sun)
keplers 3rd law
the square of the orbital period of a planet is directly proportional to the cube of its average distance from the sun
T² ∝R³
gravitational potential
Vg at any point in a gravitational field is defined as the work done per unit mass to move an object to that point from infinity
infinity is a distance so far away from the object producing the field that g = 0
= -GM/r