How Do You Calculate the Period of Radial Oscillations in a Neutron Star?

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Homework Help Overview

The discussion revolves around calculating the period of radial oscillations in a neutron star, modeled as a uniformly dense sphere. Participants explore the implications of hydrostatic equilibrium and the relationship between pressure and density in this context.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • The original poster attempts to derive the period of oscillations using hydrostatic equilibrium and questions the implications of obtaining a negative pressure value. They also inquire about calculating the time for oscillation from the center to the surface and back.
  • Some participants emphasize the importance of boundary conditions and integration constants in the calculations, while also questioning how to determine the pressure at the surface of the neutron star.
  • Others suggest that the pressure at the surface should be zero, which could help in deriving the integration constant.

Discussion Status

The discussion is active, with participants raising questions about boundary conditions and the implications of their calculations. There is a focus on clarifying concepts related to pressure and density, and some guidance has been offered regarding the integration constant and its relevance to the problem.

Contextual Notes

Participants note that the problem does not specify boundary conditions, leading to uncertainty in how to proceed with the calculations. The lack of explicit information on these conditions is a point of contention in the discussion.

June_cosmo
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Missing template due to originally being posted in different forum.
Assuming a neutron star is a uniformly dense sphere of radius 10km and mass =1.4 mass of sun, derive the period of radial oscillations.First use hydrostatic equilibrium to calculate p, then the velocity of sound is $$v= \sqrt{ \gamma p / \rho}$$, so the period of pulsation is time it takes from r=0 to r=R and come back.

I first used hydrostatic equilibrium:$$ \frac{dp}{dr}=- \frac{GM(r)\rho}{r^2}$$
and $$M(r)= \frac{4}{3} \pi r^3 \rho$$ so that $$ p(r)=- \frac {2}{3} \pi \rho^2r^2$$,
so question 1: how does there is a negative value?
question 2:how do I calculate time from r=0 to r=R and back?
 
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Don't forget the integration constant. What is the boundary condition for pressure?
June_cosmo said:
question 2:how do I calculate time from r=0 to r=R and back?
That follows from the velocity.
 
mfb said:
Don't forget the integration constant. What is the boundary condition for pressure?
That follows from the velocity.
Thanks for your answer. No the problem doesn't say the boundary condition. How do I know that?
 
Last edited:
June_cosmo said:
No the problem doesn't say the boundary condition. How do I know that?
What do you expect as pressure at the surface?
 
mfb said:
What do you expect as pressure at the surface?
Because P(r) decrease along r it would be 0? so I can derive the constant?
 
It is zero, as particles would move outwards otherwise. Yes, this allows to find the constant.
 
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