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Topic 9.2 
1.3.1 - Newton, Cannons & Satellites
Newton’s Thought Experiment 
 Isaac Newton’s 3 laws of motion and his 
law of universal gravitation gave him the 
idea of placing objects into orbit. 
 N1: An object will continue in a straight line 
at constant speed unless a force acts. 
 N2: An unbalanced force causes an 
acceleration, i.e. a change in speed or 
direction. 
 NLUG: Any two objects with mass, exert a 
gravitational attraction on each other.
Newton’s Thought Experiment 
• He considered what would happen if a cannon ball were to be 
shot at different speeds from the top of a very high mountain on 
the equator. 
• As the velocity of the projectile increased, so did the range. 
• He also noted that the radius of curvature increased as well. 
• He proposed that at the correct velocity, the projectile would 
curve at the same rate as the Earth’s surface. 
• The projectile would orbit the Earth. 
• Exceed this speed and the projectile would be able to escape 
the Earth’s gravity.
Free Falling Spacemen 
• Astronauts in space are not really weightless! 
• They are not in zero-gravity! 
• If they were then there would be no force acting on them. 
• So they would, by N1 and N2, continue in a straight line and 
not orbit the Earth. 
• They are really “Free-falling” around the Earth at the 
same rate of curvature as the Earth. 
• They are falling towards the Earth but constantly missing.
Escaping Earth 
•The velocity required for a projectile 
to fully escape the Earth’s 
gravitational field is called the 
escape velocity. 
•This can be given by applying the 
law of conservation of energy. 
•KE of projectile = change in GPE 
mv2 = mgDh = G Mm 
2 
r 
1
Escaping Earth 
v G M 
R 
2 = 
2 
v GM 
R 
2 
= 
•Notice that the mass of the projectile is 
not a factor in determining escape 
velocity. 
•Use your table of mass and planetary 
radius (earlier homework) to calculate the 
escape velocity from each of the solar 
system planets.
Satellites 
• To place a satellite into orbit around the Earth, 
requires that it be launched with a velocity, less 
than the escape velocity. 
• The satellite is said to be “bound” by Earth’s gravity. 
• This velocity is around 8kms-1!
Launching Satellites 
• Consider the impulse required to launch a 50kg 
satellite into orbit from the Earth’s surface. 
• Required velocity = 8kms-1. 
• Initial velocity = 0 kms-1. 
• Impulse = m (v-u) 
= 50 (8000-0) 
= 400 000 Ns
Launching Satellites 
Consider the Force required to 
launch a satellite. 
Thrust – Weight = ma 
T - mg = ma 
If the impulse calculated earlier was 
applied over a time of 10 seconds 
then the trust force would be 40kN 
This would mean that the satellite 
experiences a force of 40kN and 
an acceleration of 790ms-2 
Thrust 
Weight
Launching Satellites 
Another way of thinking of 
this is the satellite feels a 
force of 40000N 
This is eighty times its 
normal weight of 500N 
This can be written as 80g! 
This may be fine for a 
mechanical object, but 
would instantly kill a 
human! 
Thrust 
Weight
Launching Humans 
Humans can tolerate forces up to 5g for short periods of 
time before G-LOC (G loss of consciousness) 
Well trained pilots with proper equipment can survive 9g 
for short times. 
Assume a maximum force of 5g is applied to an 80kg 
astronaut. 
What is the force required to launch him into space? 
What is the impulse required to launch him into orbit? 
How long must the launch force be applied for?
A Helping Hand 
• Most space ports are located close(ish) to the 
equator and toward the eastern coast of the 
continents. 
• This reduces the force required to accelerate 
the rocket, as it would already have the speed 
of the Earth at take off. 
• If the radius of the Earth is 6400km what is the 
velocity of a rocket on the equator?
Types of Orbit 
There are two basic types of satellite orbit: 
Geostationary – the satellite orbits with the 
same angular velocity as the Earth. 
Low Earth Orbit – the satellite orbits closer to 
the Earth at high speed. 
What could these two orbits be used for?
Satellite Orbits 
NASA Satellite Tracker
Orbital Decay 
The Edge of space is 
considered to start at 
100km. 
But, the edge of the 
atmosphere is not a hard 
edge! 
A few gas molecules extend 
outwards into space. 
Satellites in low Earth orbit 
continually collide with these 
molecules, losing energy. 
We say that the orbit decays!
Orbital Decay 
To prevent orbital decay, modern satellites carry 
more fuel than is needed to reach orbit. 
The extra fuel is used to “boost” the satellite back 
up into a stable orbit.
Re-entry 
In orbit, a spacecraft has high kinetic energy and high 
gravitational potential energy relative to the ground. 
To safely return to Earth, this excess energy must be 
dissipated. 
First small “retro-rockets” are used to slow the rocket 
down. 
Friction with the upper layers of the atmosphere is 
allowed to do the rest.
Re-Entry 
The angle of re-entry is also important. 
Too steep and the accelerations may kill the 
pilots. 
Too shallow could cause the spacecraft to 
bounce off the atmosphere. 
The correct angle is between 5 and 7 degrees 
to the atmosphere!
Shuttle Re-Entry 
http://www.youtube.com/watch?v=qQkqCCRAa38

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1.3.1 newton cannons and satellites

  • 1. Topic 9.2 1.3.1 - Newton, Cannons & Satellites
  • 2. Newton’s Thought Experiment  Isaac Newton’s 3 laws of motion and his law of universal gravitation gave him the idea of placing objects into orbit.  N1: An object will continue in a straight line at constant speed unless a force acts.  N2: An unbalanced force causes an acceleration, i.e. a change in speed or direction.  NLUG: Any two objects with mass, exert a gravitational attraction on each other.
  • 3. Newton’s Thought Experiment • He considered what would happen if a cannon ball were to be shot at different speeds from the top of a very high mountain on the equator. • As the velocity of the projectile increased, so did the range. • He also noted that the radius of curvature increased as well. • He proposed that at the correct velocity, the projectile would curve at the same rate as the Earth’s surface. • The projectile would orbit the Earth. • Exceed this speed and the projectile would be able to escape the Earth’s gravity.
  • 4.
  • 5. Free Falling Spacemen • Astronauts in space are not really weightless! • They are not in zero-gravity! • If they were then there would be no force acting on them. • So they would, by N1 and N2, continue in a straight line and not orbit the Earth. • They are really “Free-falling” around the Earth at the same rate of curvature as the Earth. • They are falling towards the Earth but constantly missing.
  • 6. Escaping Earth •The velocity required for a projectile to fully escape the Earth’s gravitational field is called the escape velocity. •This can be given by applying the law of conservation of energy. •KE of projectile = change in GPE mv2 = mgDh = G Mm 2 r 1
  • 7. Escaping Earth v G M R 2 = 2 v GM R 2 = •Notice that the mass of the projectile is not a factor in determining escape velocity. •Use your table of mass and planetary radius (earlier homework) to calculate the escape velocity from each of the solar system planets.
  • 8. Satellites • To place a satellite into orbit around the Earth, requires that it be launched with a velocity, less than the escape velocity. • The satellite is said to be “bound” by Earth’s gravity. • This velocity is around 8kms-1!
  • 9. Launching Satellites • Consider the impulse required to launch a 50kg satellite into orbit from the Earth’s surface. • Required velocity = 8kms-1. • Initial velocity = 0 kms-1. • Impulse = m (v-u) = 50 (8000-0) = 400 000 Ns
  • 10. Launching Satellites Consider the Force required to launch a satellite. Thrust – Weight = ma T - mg = ma If the impulse calculated earlier was applied over a time of 10 seconds then the trust force would be 40kN This would mean that the satellite experiences a force of 40kN and an acceleration of 790ms-2 Thrust Weight
  • 11. Launching Satellites Another way of thinking of this is the satellite feels a force of 40000N This is eighty times its normal weight of 500N This can be written as 80g! This may be fine for a mechanical object, but would instantly kill a human! Thrust Weight
  • 12. Launching Humans Humans can tolerate forces up to 5g for short periods of time before G-LOC (G loss of consciousness) Well trained pilots with proper equipment can survive 9g for short times. Assume a maximum force of 5g is applied to an 80kg astronaut. What is the force required to launch him into space? What is the impulse required to launch him into orbit? How long must the launch force be applied for?
  • 13. A Helping Hand • Most space ports are located close(ish) to the equator and toward the eastern coast of the continents. • This reduces the force required to accelerate the rocket, as it would already have the speed of the Earth at take off. • If the radius of the Earth is 6400km what is the velocity of a rocket on the equator?
  • 14. Types of Orbit There are two basic types of satellite orbit: Geostationary – the satellite orbits with the same angular velocity as the Earth. Low Earth Orbit – the satellite orbits closer to the Earth at high speed. What could these two orbits be used for?
  • 15. Satellite Orbits NASA Satellite Tracker
  • 16. Orbital Decay The Edge of space is considered to start at 100km. But, the edge of the atmosphere is not a hard edge! A few gas molecules extend outwards into space. Satellites in low Earth orbit continually collide with these molecules, losing energy. We say that the orbit decays!
  • 17. Orbital Decay To prevent orbital decay, modern satellites carry more fuel than is needed to reach orbit. The extra fuel is used to “boost” the satellite back up into a stable orbit.
  • 18. Re-entry In orbit, a spacecraft has high kinetic energy and high gravitational potential energy relative to the ground. To safely return to Earth, this excess energy must be dissipated. First small “retro-rockets” are used to slow the rocket down. Friction with the upper layers of the atmosphere is allowed to do the rest.
  • 19. Re-Entry The angle of re-entry is also important. Too steep and the accelerations may kill the pilots. Too shallow could cause the spacecraft to bounce off the atmosphere. The correct angle is between 5 and 7 degrees to the atmosphere!