How Does Doubling a Satellite's Mass Affect Its Orbital Speed and Stability?

In summary: Earth on them at that height ??For number 3, for the force on m, it would be the sum of all the individual gravitational forces from each M, taking into account the angles and distances between them. The gravitational field at the center of curvature would be zero since there is no mass at that point.
  • #1
nns91
301
1

Homework Statement


1. If the mass of a satellite is doubled, the radius of its orbit can remain constant if the speed of the satellite:
a. increases by a factor of 8
b. increases by a factor of 2
c. does not change
d. is reduced by a factor of 8
e. is reduced by a factor of 2

2. Astronauts orbiting in a satellite 300km above the surface of the Earth feel weightless. Why ? Is the force of gravity exerted by the Earth on them negligible at this height ?

3. Five equal masses M are equally spaced on the arc of a semicircle of radius R. m is located at the center of curvature of the arc. (a) If M is 3kg,m is 2kg, and R is 10cm, what is the force on m due to the 5 masses. If m is removed, what is the gravitational field at the center of curvature of the arc ?

Homework Equations



F= -Gm1m2/ r^2, T^2= 4pi^2r^3/GM(s)

The Attempt at a Solution



1. I chose e but I am wrong. What would be the appropriate way to find out the answer of this question ??

2. I said that the distance r^2 is really big so F is negligible at this height. I am wrong again. How should I explain this ??

3. So I did this problem wrong. Is it true that 4 of M are canceled because they are opposite ? So the only mass that affect is M which is right above m right ?
 
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  • #2
nns91 said:
1. I chose e but I am wrong. What would be the appropriate way to find out the answer of this question ??

2. I said that the distance r^2 is really big so F is negligible at this height. I am wrong again. How should I explain this ??

3. So I did this problem wrong. Is it true that 4 of M are canceled because they are opposite ? So the only mass that affect is M which is right above m right ?

In 1. you have the equation for the period... what happens when you change the mass of the satellite?

In 2. ... what forces are acting on the astronaut?

In 3. ... no. Draw the x,y components of gravitational force.
 
  • #3
1. If I double the mass then T^2 will be reduced by a factor of 2. Thus, T will be reduced by square root of 2. ??

2. Gravitational force ??
 
  • #4
All orbit problems should begin with Fc = Fg (the centripetal force is provided by the gravitational force). Putting in the details,
mv^2/R = GmM/R^2 where m is the mass of the satellite, M of the Earth.
or R*v^2 = GM
This is a Kepler's Law for circular orbits. You can use it to answer question 1.

For #2, if the force of gravity was negligible the satellite would move in a straight line rather than in circular motion. Being in a circular orbit means that the force of gravity is exactly right to provide the centripetal force necessary to remain in circular motion. The force accelerates the satellite (and the people inside) toward the center of the Earth with a = v^2/R. This is exactly the same thing that happens when you jump out of an airplane with no parachute (and no significant air resistance). Except that there is a tangential velocity that makes the satellite avoid hitting the Earth as it falls.

Is it true that 4 of M are canceled because they are opposite ? So the only mass that affect is M which is right above m right ?
No. That would apply to 2 of the M's if they are at the extremities of the semicircular arc. The others all have a component that doesn't cancel out. You have to do some serious work on this, using F = GmM/R^2 for each M. Don't forget the angles as you work out the horizontal and vertical components for each F.
 
  • #5
#2. The spacecraft ’s orbital velocity and rate of gravitational attraction per its altitude are such that it allows continuous free-fall precisely per the curvature of the Earth hence altitude is neither gained nor lost. In essence, equilibrium has been established between Earth’s rate of gravitational attraction and per the spacecraft ’s orbital velocity allowing endless free-fall with virtually no detectable forces experienced by the spacecraft ’s occupants.

This differs considerably from the centripetal force exerted upon an object being rotated on Earth. At the center of a rotating object (such as when a person rotates a ball per a length of string), the person does not produce an attraction toward the center axis as the Earth does to the spacecraft therefore, the only manner in which the rotating ball can be altered from its otherwise tangential direction is per the centripetal force constantly applied via the string as it rotates, which of course, can be felt and measured. So long as the ball on the string maintains a constant velocity per a circular path, it will experience a continuous change in its tangential direction, which produces a continuous acceleration on the rotating ball. The only time the ball does not feel this constant acceleration is if the string is released or the string breaks, in which case, the ball simply travels straight per its tangential direction until it hits the ground. The ball being rotated at a constant velocity via the string is incapable of experiencing equilibrium (no sense of force or acceleration from any direction) while being rotated at a constant velocity, which is totally unlike that of the spacecraft and its occupants per its constant orbital velocity.

So, an object being rotated on the Earth at a constant velocity is still quite different than an object orbiting the planet at a constant velocity hence, the end results of these two concepts are as different as the concepts themselves.
 
  • #6
For number 1, is it does not change since velocity is independent of mass of satellite ??
For number 2, then why does the astronaut feel weightless ?
 
Last edited:
  • #7
Yes, you have #1.
For #2 I can only repeat that he is accelerating just like he would after jumping out of an airplane without a parachute.
 
  • #8
nns91 said:
For number 2, then why does the astronaut feel weightless ?

From F = m*a if he is accelerating then if there is something against which the acceleration resists, you know like the floor, if you put a scale there then it will measure a force of something on top, as in the case of the astronaut - his/her weight.

But the question says the astronaut is weightless. So is it the case that gravity is not acting, or is it that there is another force acting such that gravity is counter balanced and the net effect is 0 acceleration (in the frame of reference of the living module)?
 
  • #9
Is that because centripetal force and gravitational force are balance so the man is weightless ?
 
  • #10
nns91 said:
Is that because centripetal force and gravitational force are balance so the man is weightless ?

Yes, but don't forget to answer the rest of the question. You can calculate gravitational acceleration is at that height for instance.
Is the force of gravity exerted by the Earth on them negligible at this height ?
 

1. What is gravity?

Gravity is a fundamental force of nature that causes objects with mass to be attracted to each other. It is responsible for keeping planets in orbit around the sun and objects on Earth from floating away.

2. Who discovered gravity?

Sir Isaac Newton is credited with discovering the universal law of gravitation in the 17th century. However, the concept of gravity has been studied and observed by scientists and philosophers for centuries.

3. What are Kepler's laws of planetary motion?

Kepler's laws of planetary motion are three laws that describe the movement of planets around the sun. The first law states that planets move in elliptical orbits with the sun at one focus. The second law states that a line joining a planet and the sun sweeps out equal areas in equal times. The third law states that the square of the orbital period of a planet is proportional to the cube of its average distance from the sun.

4. How does gravity affect objects in space?

Gravity affects objects in space by causing them to orbit around a larger, more massive object such as a planet or star. It also governs the motion of celestial bodies and holds galaxies together.

5. Can gravity be explained by Einstein's theory of relativity?

Yes, Einstein's theory of general relativity provides a more accurate and comprehensive explanation of gravity compared to Newton's law of gravitation. It describes how gravity arises from the curvature of space and time caused by the presence of mass and energy.

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