My_Wan,
I agree with you on this. And this can be easily deduced by a fundamental situation and then to be safely and securely generalized. The rule is concerned with locally-fixed-particles body, not any system. And this is done in many of the mechanics-specialized books.
But, I just want to wonder about gravitational waves. Away from GR, if there is no gravitational waves, then is a particle (affecting another particle) was moving, the new Force at any space-point after a time will depend upon that instantaneous distance from the particle at that time. So as to say, effect will be transmitted at ZERO-TIME! Or... Remote Effect. And this was totally rejected by Newton, although not having spoken about Gravitational Waves. It was a paradox for him, especially in the last of his age.
What do you think buddy?
I think that all the calulations of the problem may be done in the below:
Meq * Rcm> = Sum{ mi * Int[ Int[ G * Meq (ri'>)/(ri^2) ]dt ]dt }.
Where: 1. > denotes a vector, 2. '> denotes a unit vector, 3. mi is the mass of the particle, 4. ri> is the displacement vector of the particle from the Rcm>, 5. Rcm> is the position vector of the centre of mass 6. Meq is the summation of all masses, 7. Sum: summation and 8. Int: integration.
Differentiating both sides, we get the acceleration of the CM. Of course, R.H.S is also in both sides of this derived ODE, but, we can test the R.H.S. to check this special system. It may help.
By the way, we can reach:
Meq * Acm> = Sum(over i){ Sum(over j<>i) { mi * mj * G * [ (ri'>)/(ri^2)+(rj'>)/(rj^2) ] } }.
where Acm> is the acceleration vector of the CM.
Please forgive me not to go into these details. As I already got determined that the Rule was somewhat commonly generalized (and understood) in error.
It is related to rigid bodies.
Yours,
Amr Morsi.