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Define (i) angular velocity, (ii) centripetal force - Leaving Cert Physics - Question 6 - 2005

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Define (i) angular velocity, (ii) centripetal force. State Newton’s Universal Law of Gravitation. A satellite is in a circular orbit around the planet Saturn. Deri... show full transcript

Worked Solution & Example Answer:Define (i) angular velocity, (ii) centripetal force - Leaving Cert Physics - Question 6 - 2005

Step 1

Define (i) angular velocity

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Answer

Angular velocity (ω\, \omega) is defined as the rate of change of angular displacement with respect to time. It is represented mathematically as:

ω=θt\omega = \frac{\theta}{t}

where θ\theta is the angular displacement in radians and tt is the time in seconds.

Step 2

Define (ii) centripetal force

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Answer

Centripetal force is the force required to keep an object moving in a circular path, directed towards the center of the circle. It can be described as:

Fc=mv2rF_c = \frac{mv^2}{r}

where mm is the mass of the object, vv is its tangential velocity, and rr is the radius of the circular path.

Step 3

State Newton’s Universal Law of Gravitation

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Answer

Newton’s Universal Law of Gravitation states that the gravitational force (FF) between two masses (m1m_1 and m2m_2) separated by a distance (rr) is given by:

F=Gm1m2r2F = G \frac{m_1 m_2}{r^2}

where GG is the universal gravitational constant.

Step 4

Derive the relationship between the period of the satellite, the mass of Saturn and the radius of the orbit

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Answer

For a satellite in circular orbit, the gravitational force provides the necessary centripetal force:

GMmr2=mv2rG \frac{M m}{r^2} = \frac{m v^2}{r}

where MM is the mass of Saturn and mm is the mass of the satellite. The velocity vv can be expressed as:

v=2πrTv = \frac{2\pi r}{T}

Substituting for vv gives:

GMmr2=m(2πrT)2rG \frac{M m}{r^2} = \frac{m (\frac{2\pi r}{T})^2}{r}

This simplifies to:

GM=(2π)2rT2G M = \frac{(2\pi)^2 r}{T^2}

Rearranging for T2T^2:

T2=4π2r3GMT^2 = \frac{4\pi^2 r^3}{G M}

This is the desired relationship.

Step 5

Calculate the radius of the satellite’s orbit around Saturn

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Answer

Given that the period T=380T = 380 hours, we convert this to seconds:

T=380×3600=1368000sT = 380 \times 3600 = 1368000 \, \text{s}

Using the derived formula:

T2=4π2r3GMT^2 = \frac{4\pi^2 r^3}{G M}

We rearrange:

r3=GMT24π2r^3 = \frac{G M T^2}{4\pi^2}

Substituting values:

  • G=6.7×1011N m2/kg2G = 6.7 \times 10^{-11} \, \text{N m}^2 / \text{kg}^2
  • M=5.7×1026kgM = 5.7 \times 10^{26} \, \text{kg}
  • T=1368000T = 1368000 s

Calculating gives:

r3=(6.7×1011)(5.7×1026)(13680002)4π21.37×106mr^3 = \frac{(6.7 \times 10^{-11})(5.7 \times 10^{26})(1368000^2)}{4\pi^2} \approx 1.37 \times 10^{6} \, \text{m}

Thus:

r1.2×106mr \approx 1.2 \times 10^6 \, \text{m}.

Step 6

How long does it take the signal to travel to earth?

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Answer

The time taken (tt) for the signal to travel a distance (dd) is given by:

t=dvt = \frac{d}{v}

where d=1.2×1012md = 1.2 \times 10^{12} \, \text{m} and v=3.0×108m/sv = 3.0 \times 10^8 \, \text{m/s}. Thus:

t=1.2×10123.0×1084000s1.1h.t = \frac{1.2 \times 10^{12}}{3.0 \times 10^{8}} \approx 4000 \, \text{s} \approx 1.1 \, \text{h}.

Step 7

Explain why the frequency of the received radio signal changes as the satellite orbits Saturn

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Answer

The Doppler effect explains the change in frequency of the received signal. As the satellite moves towards the Earth, the frequency increases (blue shift) because the source is moving closer. Conversely, as it moves away, the frequency decreases (red shift). This is due to the relative motion between the satellite (the source) and the Earth (the detector) affecting the observed frequency.

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