Gravitational Potential Energy of Envelope around star

In summary, to calculate the gravitational potential energy of the envelope of a giant star with a radius of 200 Rsun, with a core of mass 0.6 Msun and an extended envelope of mass 0.2 Msun, you can use the equation U = -[G * (0.6 Msun + 0.2 Msun) * 0.2 Msun]/200 Rsun. The thickness of the envelope is not necessary in this calculation.
  • #1
godzilla5002
3
0
I am confused about this question:

A giant star has a radius of 200 Rsun, with core of mass 0.6 Msun surrounded by an extended envelope of mass 0.2 Msun.
(a) Estimate the gravitational potential energy of the envelope.



When it says the envelope, does this mean the 'shell' surrounding the interior, where you can use the conservation of mass equation of a shell => dm/dr = 4pi*p*r^2 and Plugging it into Gravitational potential energy equation: dU = -[G M(r)*dm]dr/r. In this case dm is the mass of envelope and M(r) is 0.6Msun and r would be 200Rsun. Not sure what dr would be, since it is the thickness of the envelope. Thanks
 
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  • #2
for any help!

Hello there,

Thank you for your question. It seems like you are on the right track with your approach to solving this problem. However, there are a few things to consider when calculating the gravitational potential energy of the envelope.

Firstly, when we talk about the envelope of a star, we are referring to the outer layers of the star, including the outermost layer known as the photosphere. So in this case, the envelope would refer to the layers of the star beyond the core, not just the shell immediately surrounding it.

Secondly, the conservation of mass equation for a shell that you mentioned is used to calculate the mass contained within a spherical shell, not the thickness of the shell. In this case, we already have the mass of the envelope given to us (0.2 Msun), so we do not need to use this equation.

To calculate the gravitational potential energy of the envelope, we can use the equation you mentioned: dU = -[G M(r)*dm]/r. But instead of using the conservation of mass equation, we can simply use the mass of the envelope (0.2 Msun) and the radius of the giant star (200 Rsun) to calculate the potential energy at the surface of the envelope.

So the final equation would be: U = -[G * (0.6 Msun + 0.2 Msun) * 0.2 Msun]/200 Rsun. The thickness of the envelope is not needed in this calculation.

I hope this helps clarify the approach to solving this question. Please let me know if you have any further questions. Good luck!
 

Related to Gravitational Potential Energy of Envelope around star

1. What is gravitational potential energy?

Gravitational potential energy is the energy possessed by an object due to its position in a gravitational field. It is the energy that is required to move the object from its current position to another position in the gravitational field.

2. How is the gravitational potential energy of an envelope around a star calculated?

The gravitational potential energy of an envelope around a star can be calculated using the formula U = -G(m1m2)/r, where G is the gravitational constant, m1 and m2 are the masses of the star and the envelope, and r is the distance between them.

3. What factors affect the gravitational potential energy of an envelope around a star?

The gravitational potential energy of an envelope around a star is affected by the mass of the star, the mass of the envelope, and the distance between them. The greater the masses and the closer the distance, the higher the gravitational potential energy.

4. How does the gravitational potential energy of an envelope around a star affect its stability?

The gravitational potential energy of an envelope around a star is directly related to its stability. The higher the gravitational potential energy, the less stable the envelope is. This means that the envelope is more likely to collapse onto the star due to the strong gravitational pull.

5. Can the gravitational potential energy of an envelope around a star be converted into other forms of energy?

Yes, the gravitational potential energy of an envelope around a star can be converted into other forms of energy, such as kinetic energy or thermal energy. This conversion can occur when the envelope collapses onto the star, releasing a significant amount of energy in the process.

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