Question on Orbits and Kepler/Uni. Grav. Laws

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Homework Help Overview

The discussion revolves around a problem related to orbital mechanics, specifically focusing on the distances involved when a moon is at different points in its orbit around a planet. The original poster is trying to determine the distance from the moon to the center of the planet when the moon is at a specific point, using concepts from Newton's law of gravitation and Kepler's laws.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • The original poster attempts to apply gravitational principles and centripetal acceleration to solve for the distance but questions their calculations after receiving feedback. Other participants suggest using Kepler's second law and conservation of angular momentum as alternative approaches, while some express uncertainty about using Kepler's third law in this context.

Discussion Status

Participants are exploring various methods to approach the problem, with some suggesting that the original poster reconsider their calculations. There is an acknowledgment of the limitations of applying Kepler's third law directly, and a focus on conservation laws is emerging as a potentially more suitable direction for solving the problem.

Contextual Notes

Some participants note the absence of specific values for mass, eccentricity, or the length of the semimajor axis, which complicates the application of Kepler's laws. The discussion reflects a mix of understanding and confusion regarding the appropriate use of different physical principles in this scenario.

RoboNerd
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Homework Statement


The picture has the problem question.
image1.JPG


OK.

When the moon is at point B, the distance from the moon to the center of the planet is most nearly:

A) (1/25) * rA
B) (1/5) * rA
C) (1/ sqrt(5) ) * rA
D) rA
E) sqrt(5) * rA.

Homework Equations



Newton's law of gravitation. kepler's third law

The Attempt at a Solution


[/B]
Ok. I am told that the correct answer is B but I do not know why.

I got A instead. Here's what I did.

I solved from my rA for the planet at point A.

I apologize for my bad math formatting, but I am in a rush and can not use latex. Hope you understand.

Gravitational force causes centripetal acceleration:

G * mPlanet * mMoon mMoon * (v0)^2
--------------------------- = -----------------------
(rA)^2 rA.

I cancel mMoon and one of my rA terms and I solve for v0^2. I got v0^2 to be equal to
G * mPlanet/r.

I then did the same thing for my planet in position B.
G * mPlanet * mMoon mMoon * (5v0)^2 mMoon * 25 * v0^2
--------------------------- = ----------------------- = ----------------------
(rB)^2 rB. rB

I plugged in my calculated result for v0^2 for position A into the expression and solved for rB.
My G and my mPlanet terms cancel. I got rB = rA/25.

Where did I mess up?

Thanks in advance.
 
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Hi,

I'm absolutely not an expert in that field but I may have another approach:

Maybe you should consider the second Kepler's law: the conservation of the area in a given time.

The moon travels v0*t in the time t, if you consider a small enough time, you have the small angle approximation which provides tan(theta)=theta so the area is vo*t*rA

This value has to be equals to 5*v0*t*rB, so rA is 5 times bigger than rB...

Is it ok for you ?

Regards,

Anton
 
I read up a little on kepler's second law but they did not teach it in my high school class, so I am afraid to use that approach, especially with the small angle approximation.

I do see how your approach works and makes sense... but my AP Physics exam is looking for the third law, and I am trying to use it, if possible.

Thanks a lot for that interesting thought!
 
The problem is that for elliptical orbits the centripetal force does not balance the gravitational force. That's why the planet's speed changes and the orbit is not circular.

A better approach is to use a conservation law. Kepler's 2nd law is really a statement about conservation of angular momentum, and you should look at the problem from that point of view. The two points of interest in this problem (apogee and perigee) are particularly amenable to this approach (why?).
 
Ahh. I see the pitfall now.

Kepler's 2nd law makes sense now.

I see why kepler's third does not make sense.

Thanks!
 
but is there any way I can use Kepler's third at all? modified, perhaps?
 
RoboNerd said:
I plugged in my calculated result for v0^2 for position A into the expression and solved for rB.
My G and my mPlanet terms cancel. I got rB = rA/25.

Between 25 and 5 you clearly have squared something by mistake, I haven't done the calculations but you should check if you didn't consider v0² instead of v0 somewhere...
 
RoboNerd said:
but is there any way I can use Kepler's third at all? modified, perhaps?
If there is it would probably be a very round-about way. You have to work with the information given, which does not directly give you the length of the semimajor axis of the orbit or the period. Nor are you given any actual mass values or velocities, and you aren't even supplied with an eccentricity value to help find other related parameters, so the Newton form of Kepler III is no help.

I think this problem is constructed specifically to be solved using conservation of angular momentum.
 
RoboNerd said:
but is there any way I can use Kepler's third at all? modified, perhaps?
Please state Kepler's Third Law for us.
 
  • #10
Ok. I see how kepler's third law would not work. and I took (5 times v0)^2 and wrote it as 25 times v0^2. i do not think i made a mistake there.

kepler's third law is that the period squared is proportional to radius of orbit cubed.
 
  • #11
and they did state the masses to be m and 49m, so I could use them, no?
 
  • #12
RoboNerd said:
and they did state the masses to be m and 49m, so I could use them, no?
Well, yes and no. A simple ratio of masses for primary and satellite won't tell you much about the orbit since that depends on the total mechanical energy and the eccentricity. Kepler III gives you a handle on comparing the periods and sizes of different orbits in a system, but not much about one single orbit. You might be able to do something with the complete Newton version of Kepler III and define your own mass unit and a gravitational parameter μ (equivalent to GM) to fit the system. Then you'd still need to use an equation other than Kepler to relate velocity and radius for a single orbit.
 
  • #13
hmmm... that sounds a bit over my head with my limited knowledge of physics. thanks a lot, though!
 

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