Gravitational Fields Flashcards

1
Q

Describe Newton’s law of gravitation.

A

The force between two masses is:
Always attractive,
Directly proportional to the product of the masses,
Inversely proportional to the square of the distance between them.

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2
Q

Give the equation for the force between two masses.

A

F = GMm / r2

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3
Q

Define gravitational field strength in words.

A

Force per unit mass on an object due to a gravitational field.

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4
Q

Give the equation that defines gravitational field strength.

A

g = F / m

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5
Q

Give two units for gravitational field strength.

A

N kg-1
m s-2

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6
Q

Is gravitational field strength scalar or vector? What significance does this have when combining field strengths?

A

Vector quantity.
Direction must be considered when combining.

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7
Q

What do gravitational field lines show?

A

The direction of the force,
that a mass would feel in a gravitational field.

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8
Q

Sketch a radial gravitational field and describe the key features.

A

Field lines meet in the centre.
Field strength decreases with distance.
Shown by field lines getting further apart.

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9
Q

Give the equation for gravitational field strength in a radial field.

A

g = GM / r2

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10
Q

Sketch a uniform gravitational field and describe the key features.

A

Field strength is constant.
Shown by equally spaced parallel lines.
The surface of a planet can be approximated as a uniform field.

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11
Q

Define gravitational potential at a point in a gravitational field.

A

Work done per unit mass
To move an object from infinity to that point.

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12
Q

Give the equation for gravitational potential in a radial field.

A

V = -GM / r

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13
Q

Why is gravitational potential negative?

A

Gravitational potential is defined as zero at infinity.
And work needs to be done on an object to move it to infinity.

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14
Q

Give the equation for calculating work done moving an object in a gravitational field (i.e. change in GPE).

A

ΔW = mΔV

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15
Q

What are gravitational equipotentials?

A

Lines or surfaces connecting points of equal gravitational potential
(Usually shown at equal intervals of gravitational potential.)

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16
Q

How much work is done moving an object along an equipotential?

A

Zero as there is no change in gravitational potential.

17
Q

What do you know about the direction of equipotentials relative to field lines?

A

Equipotentials and field lines are always perpendicular.

18
Q

Explain the spacing of the equipotentials in a radial field.

A

Get further apart as distance from mass increases.
For a given energy per unit mass, an object can be moved further, as field strength decreases.

19
Q

Explain the spacing of the equipotentials in a uniform field.

A
  • Equally spaced as distance from mass increases. - For a given energy per unit mass, an object can be moved an equal distance, as field strength is constant.
20
Q

Give the equation that relates gravitational potential V and gravitational field strength g.

A

g = -ΔV / Δr

21
Q

Complete: gravitational field strength can also be referred to as…

A

Gravitational potential gradient.

22
Q

What does the magnitude of the gradient of a graph of gravitational potential V against distance r represent?

A

Gravitational field strength (g).

23
Q

If equipotentials are closer together, what does this tell you?

A

Greater rate of change of gravitational potential V with distance r (i.e. greater ΔV/ Δr).
Which means a greater gravitational field strength g.

24
Q

What does the area under a graph of gravitational field strength g against distance r represent?

A

Gravitational potential difference ΔV.

25
Q

Is gravitational potential scalar or vector? What significance does this have when combining potential?

A

Scalar quantity.
Direction does not need to be considered.

26
Q

At a point between the Earth and Moon, the overall gravitational potential is at a maximum. What do you know about the gravitational field strength at this point?

A

It is zero.
The gradient = - g and at a turning point this is zero.

27
Q

Show that the linear speed v of a satellite is inversely proportional to the square root of its orbital radius r.

A

Equate centripetal force and gravitational force.

28
Q

Show that the square of the orbital period T of a satellite is proportional to the cube of the orbital radius r (i.e. Kepler’s 3rd law).

A

Equate centripetal force and gravitational force.

29
Q

If the radius r of a satellite’s orbit increases, what happens to its linear speed v and orbital period T?

A

Linear speed decreases.
Time period increases.

30
Q

What do you know about the total energy of a satellite?

A

Total energy = kinetic energy + gravitational potential energy
Total energy is constant at all points in the orbit.

31
Q

Define escape velocity.

A

The minimum speed an unpowered object needs,
In order to leave the gravitational field,
And not fall back due to gravitational attraction.

32
Q

Derive an equation for escape velocity.

A

Consider energy change: initial Ek converted to Ep.
1/2 mv2 = mΔV

33
Q

Describe the key features of geostationary satellites.

A

Always above the same point on Earth.
In the plane of the equator (moving west to east)
Orbital period = 24 hours.
(Said to be in a ‘synchronous’ orbit with the Earth.)
(36 000 km from surface of Earth – can show this.)

34
Q

Explain why geostationary satellites are useful in telecommunication signals.

A

The satellite is stationary relative to the Earth’s surface.
So transmitters and receivers stay aligned with the satellite and do not need to be adjusted.

35
Q

Describe the key features of low orbiting satellites.

A

Orbit between 180 and 2000 km above the Earth.
Cheaper to launch and require less powerful transmitters.
Multiple satellites needed to maintain constant coverage.
Often lie in a plane that includes the poles so they can scan over the whole surface.

36
Q

Explain why low orbit satellites are useful in imaging (e.g. spying and weather).

A

Close enough to Earth’s surface to see a high level of detail.