Star moving through a cloud of particles

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SUMMARY

The discussion focuses on the mass increase of a star moving through a particle cloud, specifically deriving the equation for the rate of mass increase, given by \(\frac{dM}{dt} = \pi \rho v \left(R^2 + \frac{2GMR}{v^2}\right)\). The solution involves analyzing the collision of the star with particles in a cylindrical volume, leading to the first term of the equation. The second term is derived by considering the gravitational acceleration experienced by particles at varying distances from the star, although some participants expressed difficulty in completing this derivation.

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  • Basic understanding of conservation of energy principles.
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Homework Statement


A star of mass M and radius R is moving with velocity v through cloud of particles of density \rho. If all the particles that collide with the star are trapped by it, show that the mass of the star will increase at a rate
\frac{dM}{dt} = \pi \rho v \left(R^2 + \frac{2GMR}{v^2}\right).


The Attempt at a Solution


Assuming the motion of the star is rectilinear, it's evident that in a time \Delta t the star will collide with all the particles in a cylinder of length v \delta t, which has mass \pi R^2 \pho v \Delta t. This gives the first term in the desired equation after division by v \Delta t.

As for the second term... I'm stuck. Here's what I've tried: Consider the particles in a 'slab' (of thickness dr) of the aforementioned cylinder a distance r away from the center of the star at the beginning of the time interval \Delta t. This slab will experience an acceleration GM/r^2. Hence, assuming it started from rest, it will travel a distance \frac{GM (\Delta t)^2}{r^2} in the time interval \Delta t. Et cetera. I don't know how to proceed from this point.
 
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hi fluxions! :smile:

(have a pi: π and a rho: ρ and a delta: ∆ :wink:)

try it from the frame of reference of the star (with a wind of particles of velocity v), and use conservation of energy :smile:
 

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