Accretion discs - Orbital angular momentum

M2(Ga2/M)^(1/2) = M1(Ga1/M)^(1/2) - M2(Ga2/M)^(1/2) = M1(Ga1/M)^(1/2) - M2(Ga2/M)^(1/2) = M1(Ga1/M)^(1/2) - M2(Ga2/M)^(1/2) = M1(Ga1/M)^(1/2) - M2(Ga2/M)^(1/2) = M1(Ga1/M)^(1/2) - M2(Ga2/M)^(1/2) ≈ M1(Ga1/M
  • #1
Sheepattack
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0

Homework Statement


There is a binary system accreting via Rcohe lobe overflow, where mass is transferred fromthe donor to the accretor and then lost in an isotropic wind.

State an expression for the orbital angular momentum of the accretor, J1 and then use keplers third law to find an expression for the orbital angular speed

The Attempt at a Solution



am really stuck on this one. I know that the total angular mometum of the system can be written J = M1M2(Ga/M)1/2 but i don't know how to split this into a term for the accretor. At the moment i have come up with J1 = M1a1^2w

keplers third law can be written a3w2=GM

any help or pointers will be greatly appreciated!
 
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  • #2


Hi there,

Firstly, let's define the variables in this system. M1 is the mass of the accretor, M2 is the mass of the donor, a1 is the distance from the accretor to the center of mass, and w is the angular speed of the system.

The total angular momentum of the system can be written as J = M1M2(Ga1/M)^(1/2). To find the expression for the orbital angular momentum of the accretor, we can use the fact that the mass of the accretor is much larger than the mass of the donor (M1 >> M2). Therefore, we can approximate the total angular momentum as J ≈ M1(Ga1/M)^(1/2). Now, to find the expression for the orbital angular momentum of the accretor, we can simply subtract the contribution of the donor's angular momentum, which is given by J2 = M2(Ga2/M)^(1/2) where a2 is the distance from the donor to the center of mass. So, the expression for the orbital angular momentum of the accretor, J1, is:

J1 = J - J2 ≈ M1(Ga1/M)^(1/2) - M2(Ga2/M)^(1/2)

Next, we can use Kepler's third law, which states that the square of the orbital period is proportional to the cube of the orbital distance, to find an expression for the orbital angular speed, w. Since we are dealing with a binary system, we need to use the reduced mass, μ = M1M2/(M1+M2), in Kepler's third law. So, we have:

a1^3w^2 = G(M1+M2) ⇒ w^2 = G(M1+M2)/a1^3

Substituting this expression into our equation for J1, we get:

J1 = M1(Ga1/M)^(1/2) - M2(Ga2/M)^(1/2) ≈ M1(Ga1/M)^(1/2) - M2(Ga2/M)^(1/2) = M1(Ga1/M)^(1/2) - M2(Ga2/M)^(1/2) = M1(Ga1/M)^(1/2) -
 

1. What are accretion discs?

Accretion discs are structures that form around a central object, such as a star or black hole, and are made up of gas and dust particles. These particles are pulled in by the gravitational force of the central object and form a rotating disc around it.

2. How do accretion discs form?

Accretion discs form when a large amount of gas and dust is present around a central object. As the gas and dust particles orbit the object, they collide and lose energy, causing them to spiral towards the center and form a disc.

3. What is orbital angular momentum?

Orbital angular momentum is a measure of the rotation of an object around a central point. In the case of accretion discs, it refers to the angular momentum of the gas and dust particles as they orbit the central object.

4. Why is orbital angular momentum important in accretion discs?

Orbital angular momentum is important in accretion discs because it is the main mechanism that allows the particles to lose energy and spiral towards the central object. Without orbital angular momentum, the particles would continue to orbit at a constant distance from the central object.

5. How is orbital angular momentum related to the formation of planets?

The formation of planets is closely linked to orbital angular momentum in accretion discs. As the particles in the disc lose energy and spiral towards the central object, they can also clump together and form larger bodies, such as planets. This process is known as planetesimal accretion.

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