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Question: A binary star consists of two stars A (mass 2.2 \(M_s\)) and B (mass 11 \(M_s\)), where \(M_s\) is m...

A binary star consists of two stars A (mass 2.2 MsM_s) and B (mass 11 MsM_s), where MsM_s is mass of the sun. They are separated by distance d and a rotation about their centre of mass, which is stationary. The ratio of the total angular momentum of the binary star to the angular momentum of start B about the centre of mass is
A. 6
B. 2
C. 3
D. 1

Explanation

Solution

Determine the position of the two masses first then find the angular momentum based on the distances from the centre of mass. The centre of mass will become the axis and angular frequency about this will be the same for both the particles.
Formula used:
The angular momentum of a body about an axis is given by
L=IωL = I \omega
where I is the moment of inertia given by:
I=mr2I = mr^2.

Complete answer:
Let the centre of mass be situated at the origin. Let r1r_1 be the distance of star A (to the left of origin) and r2r_2 be the distance of second star B from the centre of mass (origin).

We are given
r2(r1)=dr_2 - (-r_1) = d
is the separation between the two bodies.
The position center of mass is given as:
rCM=m1r1+m2r2m1+m2r_{CM} = \dfrac{m_1 r_1 + m_2 r_2}{m_1 + m_2 } .
Making the substitutions according to our conditions, we may write:
0=2.2Ms(r1)+11Ms(dr1)(2.2+11)Ms0 = \dfrac{2.2 M_s ( -r_1)+ 11 M_s (d - r_1 ) }{( 2.2 + 11) M_s}
    11d=13.2r1\implies 11d = 13.2 r_1 or,
r1=56dr_1 = \dfrac{5}{6} d.
Now, r2=16dr_2 = \dfrac{1}{6} d becomes obvious.

The angular momentum of star B can be written as:
LB=Iω=(11Ms)(16d)2ωL_B = I \omega = (11 M_s)\left( \dfrac{1}{6} d \right)^2 \omega
The total angular momentum can be written as the sum of angular momentum of star A angular momentum of star B
    L=(2.2Ms)(56d)2ω+(11Ms)(16d)2ω\implies L = (2.2 M_s)\left( \dfrac{5}{6} d \right)^2 \omega + (11 M_s)\left( \dfrac{1}{6} d \right)^2 \omega
where we are substituted the respective distances from the centre of mass (or the axis) in the moment of inertia. A little simplification can give us:
L=(2.2×25+11)Ms(d6)2ω=66Ms(d6)2ωL = (2.2 \times 25 + 11) M_s \left( \dfrac{d}{6} \right)^2 \omega = 66 M_s \left( \dfrac{d}{6} \right)^2 \omega .
Taking the ratios now, we get:
LLB=66Ms(d6)2ω11Ms(d6)2ω=6\dfrac{L}{L_B} = \dfrac{66 M_s \left( \dfrac{d}{6} \right)^2 \omega }{11 M_s \left( \dfrac{d}{6} \right)^2 \omega } = 6.

So, the correct answer is “Option A”.

Note:
For the motion of two bodies around an axis, the total angular momentum can be written as a sum of angular momentum of the centre of mass and angular momentum for relative motion. This type of expression requires calculation of reduced mass for the system. The correct answer can be found using this too.