Gravitational Fields and Oscillations Flashcards

1
Q

How are gravitational fields represented by field lines?

A

Arrows show direction of the field, and separation of lines show field strength

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2
Q

What is Newton’s Law of Gravitation?

A

Any two point masses attract each other with a force that is directly proportional to the product of their masses and inversely proportional to the square of their separation.

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3
Q

Express Newton’s Law of Gravitation mathematically

A

F= -GMm/r^2

The minus sign shows the force is attractive

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4
Q

What is gravitational field strength?

A

The gravitational field strength at a point is the gravitational force exerted per unit mass on a small object placed at that point.

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5
Q

Derive a formula for gravitational field strength from the formula for gravitational force.

A

g=F/m
As F= -GMm/r^2,
g= -GM/r^2

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6
Q

How can you find orbital velocity?

A

By equating centripetal and gravitational force:
mv^2/r = GMm/r^2
v^2=GM/r

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7
Q

How can you find the orbital period?

A

As speed= distance/time
v= 2pi x r/ T (where T is the orbital period)
so 4pi^2r^2/T^2 = GM/r (from equating centripetal and gravitational force)
T^2 = 4pi^2r^3 / GM

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8
Q

What is Kepler’s Third Law of Planetary Motion?

A

The square of the orbital period is proportional to the cube of the planet’s distance from the Sun

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9
Q

Describe the features of a geostationary orbit.

A

24 hours
Remains above a fixed point on the Earth
Used for television broadcasting and telecommunications transmissions

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10
Q

Give two examples of oscillations.

A

A swinging pendulum

A trolley tethered to two springs displaced from its equilibrium position

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11
Q

Define the terms: displacement, amplitude, period and frequency

A

Displacement x- distance from equilibrium position
Amplitude a- maximum displacement
Period T- time for one complete oscillation
Frequency f- Number of oscillations per unit time (1/T)

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12
Q

Define the terms phase and phase difference

A

Phase- the point an oscillating mass has reached within the complete cycle of an oscillation
Phase difference-the fraction of oscillation that two oscillations are out of step with each other (only applicable for identical oscillations)

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13
Q

Give some examples of simple harmonic motion

A

Vibrating string of a guitar
The vibrating electrons when an alternating current flows in a wire
The vibrating air molecules when a pure sound wave travel through them

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14
Q

What are the three requirements for simple harmonic motion?

A
  1. An oscillating mass
  2. An equilibrium position
  3. A restoring force that acts to return the mass to its equilibrium position, directly proportional to the displacement x and directed towards the equilibrium position
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15
Q

What is angular frequency?

A

As an oscillation can be represented by 2pi radians, there must be 2pi x f oscillations in one unit time. This is the angular frequency of oscillation. As f = 1/T, angular frequency also = 2pi/T

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16
Q

Define simple harmonic motion.

A

A body executes simple harmonic motion if its acceleration is directly proportional to its displacement from its equilibrium position, and is always directed towards the equilibrium position.

17
Q

Give the equation that defines simple harmonic motion.

A

a = -(2pi f)^2x (where a is acceleration, f is frequency and x is displacement)

18
Q

When does a mass executing simple harmonic motion have maximum speed?

A

When it passes through the equilibrium position

19
Q

What is the formula for the maximum speed of a mass executing simple harmonic motion?

A

V= 2pifA (where A is amplitude)

20
Q

Between which two forms is energy interchanging during simple harmonic motion?

A

Potential and kinetic energy

21
Q

How are the amounts of potential and kinetic energy affected by displacement?

A

Potential energy is at its maximum when displacement is maximum( +/- A), and kinetic energy is at its maximum at the equilibrium position. At all values of displacement, total energy (KE + PE) is the same.

22
Q

What is damping?

A

When resistive forces remove energy from an oscillating system, causing amplitude to decay exponentially with time, as well as the decrease of the maximum speed.

23
Q

Why does damping cause amplitude to decay exponentially rather than linearly?

A

Velocity is proportional to amplitude, so at first the mass is moving rapidly as the amplitude is large. Energy is lost quickly and the amplitude decays at a high rate. As the amplitude decreases, the mass is moving more slowly and so energy is lost more slowly, so the amplitude decreases at a lower rate.

24
Q

How are frequency and amplitude of a simple harmonic oscillator related?

A

The frequency and amplitude are independent of each other.

25
Q

Give an example of a use of damping.

A

Shock absorbers damp the oscillating springs in cars to prevent long-term vibration after going over a bump

26
Q

What is resonance?

A

When a system capable of oscillating freely is forced to oscillate, and the forcing frequency matches the natural frequency of the system, the amplitude of the oscillations grow dramatically.

27
Q

Give an example of how damping can reduce the effects of resonance.

A

During earthquakes, resonance can occur, resulting in serious damage to buildings. In order to reduce this effect, the buildings may be built on foundations that absorb the energy of the shock waves, damping the oscillations.

28
Q

Describe how damping and resonance are related.

A

As the degree of damping increases, the amplitude of the resonant vibrations decreases.

29
Q

Describe the use of resonance in microwave cooking

A

Microwaves used in cooking have a frequency that matches the natural frequency of the vibration of water molecules. The water molecules vibrate and absorb the energy of the microwave radiation. The molecules get hotter and the energy spreads through the food, cooking it.

30
Q

Describe the use of resonance in radio

A

Radio aerials pick up many different frequencies, and the tuner can be adjusted to resonate at the frequency of the transmitting station you are interested in, and its circuit produces a large-amplitude signal for this frequency only.