Doubt in Gravitation: Understanding the Orbital Motion of Two Stars

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Homework Help Overview

The discussion revolves around the orbital motion of two stars, specifically addressing the nature of their orbits around a common center of mass (CM) and the implications for centripetal acceleration. The original poster expresses confusion regarding the correct application of distances in the context of gravitational forces and centripetal motion.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the relationship between the distances of the stars from the CM and the expressions for centripetal acceleration. The original poster questions why the distance 'd' cannot be used in the centripetal acceleration formula instead of 'r1'.
  • Some participants clarify that the stars are indeed orbiting around their common CM and discuss the implications of this on the forces acting on each star.
  • There is a consideration of how the motion of one star appears from the perspective of the other, raising questions about the trajectory observed from different reference frames.

Discussion Status

The conversation is ongoing, with participants providing insights and clarifications regarding the nature of the orbits and the forces involved. Some participants have acknowledged their misunderstandings and are seeking further clarification on related concepts, indicating a productive exchange of ideas.

Contextual Notes

There is a mention of the complexity of the mathematics involved in describing the trajectories of the stars, as well as the potential for different types of orbits depending on the system's energy. The discussion also reflects a learning environment where participants are encouraged to explore their reasoning and assumptions.

Vibhor
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Homework Statement



Suppose two stars are orbiting each other in circular orbits with angular speed ##\omega## .M1 is at distance r1 from CM wheras M2 is at distance r2 such that r1+r2=d where d is the distance between them . Now i have a little doubt whether the stars are orbiting around their common CM or they are orbiting each other . If we consider them orbiting CM then for M1 ##\frac{GM_1M_2}{d^2}=M_1\omega^2 r_1## .But it is wrong to write ##\frac{GM_1M_2}{d^2}=M_1\omega^2 d## .Could someone help me understand what is wrong with the latter expression ? Why can't we write centripetal acceleration to be ##M_1\omega^2 d##.Please pardon me for missing something obvious . Many thanks !

Homework Equations




The Attempt at a Solution

 
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Orbiting around the common CM means the same as orbiting each other.
The force of gravity is inversely proportional to the square of the distance between the stars. There is nothing at the CM to attract any of them.
But you can write the centripetal acceleration of the stars as M1ω2r1 and M2ω2r2. Both are equal to GM1M2/d2. Also, r1+r2=d, and r1=dM2/(M1+M2) and r2=dM1/(M1+M2).

ehild
 
I agree with what you have said . But i still don't understand why is it correct to have r1 in the expression for centripetal acceleration and not d . Sorry if I am sounding dumb .
 
Vibhor said:
I agree with what you have said . But i still don't understand why is it correct to have r1 in the expression for centripetal acceleration and not d . Sorry if I am sounding dumb .

Because rotation of each star is about the CM, thus r1 and r2 for the radii of rotation, not d. Just imagine one star at a time rotating about the CM.
 
rude man said:
Because rotation of each star is about the CM, thus r1 and r2 for the radii of rotation, not d. Just imagine one star at a time rotating about the CM.

I understand how M1 is orbiting CM. But M1 does have an angular velocity about M2 which means M1 is rotating about M2. This in turn means that the expression for centripetal acceleration should have 'd'. I still can't convinve myself what is wrong in this.
 
M1 is not rotating circularly about M2. M1 is rotating circularly about the CM. If you fix the position of M2, then the trajectory of M1 is not a circle. Only a circle has constant centripetal force.
 
Ok . I have realized the flaw in my reasoning.Sorry for putting up a real bad question . Another thing i would like to know is what is the trajectory of M2 as seen from M1 ? How would M2 move as seen from the reference frame of M1? Thanks !
 
Two body data

This two body data sheet attachment might come in handy.
Dean
 

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Both stars move along the same circle with the same angular velocity. In a co-rotating frame of reference, they are in rest, both of them. So M1 sees M2 in rest, with respect to itself - the distance does not change. But M2 seems to move along a circle of radius d with respect to the far-away stars.
(If M1 rotates also around its axis, the situation is different. Think of the Earth and Sun. You see the Sun rise and set, and going along a circle on the sky - why? )

ehild
 
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  • #10
Vibhor said:
Ok . I have realized the flaw in my reasoning.Sorry for putting up a real bad question . Another thing i would like to know is what is the trajectory of M2 as seen from M1 ? How would M2 move as seen from the reference frame of M1? Thanks !

Put M2 at the center of a polar coordinate system and the orbit of M1 would still be a circle.

The general solution can include circle, ellipse (e ≠ 0), parabola or hyperbola, depending on the kinetic energy of the system. In your case though it's a circle. The equation in this coordinate system is

r= k2/K = your "d"
k = r2 dθ/dt
K = G M2

This is not trivial math!
 

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