Solving Angular Velocity of Particle Skimming a Planet

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The discussion focuses on calculating the angular velocity of a particle skimming the surface of a planet in a parabolic orbit. The participant derived the angular velocity formula as ω=4√(MG/d³) but expressed uncertainty about the correctness of their approach and the definition of the variable d. They noted that the minimum radius for a parabolic orbit is d/2, which corresponds to the planet's radius at the point of closest approach. Suggestions were made to express mass in terms of density and radius to clarify the relationship between the variables. The conversation emphasizes the need for a clearer definition of d and its role in the calculations.
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Homework Statement


A particle travels in a parabolic orbit in a planet's gravitational field and skims the surface at its closest approach. The planet has mass density ρ. Relative to the center of the planet, what is the angular velocity of the particle as it skims the surface?


Homework Equations


L=mr^{2}\omega
r_{min}=\frac{L^{2}}{m\gamma(1+\epsilon)}, where ε is the eccentricity of the orbit, and γ = GMm.



The Attempt at a Solution


Okay, I used the knowledge that the minimum radius for a parabolic orbit is d/2, d being the focal length of the parabola. Because the particle is skimming the surface of the planet at this point, the radius of the planet must also be d/2. I equated that to the expression of rmin, substituting in the expression for L and using d/2 as r. I ended up getting
\omega=4\sqrt{\frac{MG}{d^{3}}}.
The units of this come out properly, but I have this nagging feeling that I did something wrong along the way. Can someone point out my error?
 
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One problem occurs to me: What's d? I mean, its value in terms of the variables given in the problem statement?

You'll want to find an expression for the angular velocity that uses the variables given. You can work with the density to find the mass in terms of the radius. Add G to the mix for an expression for μ...
 

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