Calculate Gravitational Self-Energy of the Sun

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Homework Help Overview

The discussion revolves around calculating the gravitational self-energy of the Sun, focusing on the theoretical framework rather than numerical solutions. Participants explore the concept of gravitational energy required to remove particles from the Sun's surface to infinity.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the need for an integral to calculate the energy for each particle, considering the Sun's density and structure. They propose slicing the Sun into layers and calculating the gravitational energy between these layers and the outer shell. Questions arise regarding the integration variable and limits for the integral.

Discussion Status

Several participants have shared their approaches to setting up the integral, with some confirming the correctness of each other's methods. There is an ongoing exploration of how to properly express the integrals and the variables involved, but no consensus has been reached on a final method.

Contextual Notes

Participants note the assumption of constant density and the challenge of integrating over a three-dimensional object. There is mention of a specific expected answer, but the focus remains on the process of deriving it rather than confirming the result.

stunner5000pt
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Calculate the gravitational self energy of the sun (without using numbers)

Textbook says that this is the nergy needed to take every particle from the sun's surface to infinity

there are an infinite number of particles on the sun ...
would there be some sort of integral that relates the energy needed to take one particle from the sun's surface ?

something like this - for one particle mass i, energy needed ot take it out from the sun's surface [tex]U_{i}(r) = -G \frac{M_{s} m_{i}}{r_{si}}[/tex]
but since this is a 3D object how would one go about setting up an integral like this??
 
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First, let's assume that the sun density [tex]\rho[/tex] is constant.

then, let's slice the sun from the center. If we add a layer of [tex]d R[/tex], at a distance [tex]R[/tex] from the center, then the layer mass will be [tex]dM_R=4\pi \rho R^2 dR[/tex]. Now we need to find the gravitational energy between that layer and the outer shell. So let's slice the outer shell as well: [tex]dU_R=-GM_R\int{ \frac{4 \pi \rho r^2 dr}{r}}[/tex], the integration from [tex]R[/tex] to [tex]R_0[/tex], the sun's radius. After that we need to find out [tex]\int {dU_R}[/tex].
 
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There is gravitational energy between the layer and the inner sphere (at a particular R). The mass of the inner sphere is just (4/3)pi*R^3*density

If we integrate [tex]GM_{layer}M_{innersphere}/R[/tex] over all R from 0 to the radius of the sun... I think we get the answer.

EDIT: Shyboy's method is also exactly right. I got the same answer both ways. Apologies.
 
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what is
[tex]\int dU_{R}[/tex]

what would the integration variable be then??

p.s. The answer is supposed to be [tex]\frac{3}{5} G \frac{M^2}{R}[/tex]

did you guys get that??
 
looks like so. I missed [tex]d[/tex] before [tex]M[/tex]. It should be [tex]dM_R[/tex] instead of [tex]M_R[/tex]. And I wish I can put limits in the integral but dont
know how (to lasy to find it) :(
 
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int_{lower bound}^{upper bound}

ex:

[tex]\int_a^{b-\epsilon_0}[/tex]
 
stunner5000pt said:
what is
[tex]\int dU_{R}[/tex]

what would the integration variable be then??

p.s. The answer is supposed to be [tex]\frac{3}{5} G \frac{M^2}{R}[/tex]

did you guys get that??

Yes. Here's what I did:

[tex]M_{layer} = 4\pi r^2\rho dr[/tex]

[tex]M_{inner} = \frac{4}{3}\pi r^3\rho[/tex]

Remove the layers of the sun away to infinity starting with the outermost layer.

Energy required to take a single layer out to infinity=
[tex]0 - (- \frac{GM_{layer}M_{inner}}{r})=[/tex]
[tex]\frac{16G\pi^2 \rho^2 r^4 dr}{3}[/tex]

If we integrate this from r=0 to r=R (giving the energy to take away all the layers), we get
[tex]\frac{16\rho^2 \pi^2 R^5}{15}[/tex]

If we use [tex]M=(4/3)\pi R^3\rho[/tex], solve for [tex]\rho[/tex] and plug into the above... we get
[tex]\frac{3}{5} G \frac{M^2}{R}[/tex]
 
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