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Question: A double star consists of two stars having masses \(m\) and \(2m\) separated by a distance \(r\). Wh...

A double star consists of two stars having masses mm and 2m2m separated by a distance rr. Which of the following options is correct?
A) The radius of the circular path traced by 2m2m is 2r3\dfrac{{2r}}{3} .
B) The kinetic energy of the heavier star is double that of the lighter star.
C) The period of revolution of the stars is not the same.
D) The angular momentum of the lighter star is more.

Explanation

Solution

The two stars have a mutual gravitational attraction which provides the centripetal force of rotation for each star. The two stars thus revolve about the centre of mass of the system. The distance of the star (lighter star or heavier star) from the centre of mass of the system will be the radius of the circular path described by it as it revolves.

Formulas used:
-The gravitational force of attraction between the two bodies is given by, FG=GMmr2{F_G} = \dfrac{{GMm}}{{{r^2}}} where MM and mm are the masses of the heavier body and lighter body respectively, GG is the gravitational constant and rr is the distance of separation between them.
-The centripetal force acting on a mass mm is given by, Fc=mω2r{F_c} = m{\omega ^2}r where ω\omega is the angular velocity of the mass and rr is the radius of the circle described by the mass.
-The kinetic energy of a mass mm is given by, K=12m(rω)2K = \dfrac{1}{2}m{\left( {r\omega } \right)^2} where ω\omega is the angular velocity of the mass and rr is the radius of the circle described by the mass.
-The angular momentum of a mass mmis given by, L=mr2ωL = m{r^2}\omega where rr is the radius of the circle described by the mass and ω\omega is the angular velocity of the mass.

Complete step by step answer.
Step 1: Sketch a figure depicting the double star system and list its parameters.

The two stars of masses mm and 2m2m are separated by a distance rr as shown in the above figure.
The centre of mass of the system lies at a distance r1{r_1} from the lighter mass and r2{r_2} from the heavier mass. These distances will be the radius of the circle described by the revolution of the stars.
We know from the concept of centre of mass, mr1=2mr2m{r_1} = 2m{r_2} .
r1=2r2\Rightarrow {r_1} = 2{r_2}
From the figure we have r=r1+r2r = {r_1} + {r_2} .
r2=rr1\Rightarrow {r_2} = r - {r_1}
So substituting for r1=2r2{r_1} = 2{r_2} in the above relation we get, r2=r2r2{r_2} = r - 2{r_2}
r2=r3\Rightarrow {r_2} = \dfrac{r}{3} and r1=2r3{r_1} = \dfrac{{2r}}{3}
Thus the radius of the circular orbit of the heavier mass is r3\dfrac{r}{3} .
So option A is incorrect.
Step 2: Express the centripetal force of each star to obtain their respective angular velocities and then their period of revolution.
Lighter star
The centripetal force of the lighter star is given by, Fc=mω12r1{F_c} = m{\omega _1}^2{r_1} where ω1{\omega _1} is its angular velocity and r1=2r3{r_1} = \dfrac{{2r}}{3} is the radius of its circular orbit.
The centripetal force is equal to the gravitational force of attraction.
i.e., Fc=FG{F_c} = {F_G}
The gravitational force of attraction between the stars is given by, FG=G2m×mr2{F_G} = \dfrac{{G2m \times m}}{{{r^2}}} where 2m2m and mm are the masses of the heavier star and lighter star respectively, GG is the gravitational constant and rr is the distance of separation between them.
So we have mω12(2r3)=G2m×mr2m{\omega _1}^2\left( {\dfrac{{2r}}{3}} \right) = \dfrac{{G2m \times m}}{{{r^2}}}
Cancelling out the similar terms and simplifying the above equation we get, ω12(r3)=Gmr2{\omega _1}^2\left( {\dfrac{r}{3}} \right) = \dfrac{{Gm}}{{{r^2}}}
ω12=3Gmr3\Rightarrow {\omega _1}^2 = \dfrac{{3Gm}}{{{r^3}}} or ω1=3Gmr3{\omega _1} = \sqrt {\dfrac{{3Gm}}{{{r^3}}}}
Then the period of revolution of the lighter star will be T1=2πω1=2πr33Gm{T_1} = \dfrac{{2\pi }}{{{\omega _1}}} = 2\pi \sqrt {\dfrac{{{r^3}}}{{3Gm}}}
Heavier star
The centripetal force of the heavier star of mass 2m2m is given by, Fc=2mω22r2{F_c} = 2m{\omega _2}^2{r_2} where ω2{\omega _2} is its angular velocity and r2=r3{r_2} = \dfrac{r}{3} is the radius of its circular orbit.
The centripetal force is equal to the gravitational force of attraction.
i.e., Fc=FG{F_c} = {F_G}
The gravitational force of attraction between the stars is given by, FG=G2m×mr2{F_G} = \dfrac{{G2m \times m}}{{{r^2}}} where 2m2m and mm are the masses of the heavier star and lighter star respectively, GG is the gravitational constant and rr is the distance of separation between them.
So we have 2mω22(r3)=G2m×mr22m{\omega _2}^2\left( {\dfrac{r}{3}} \right) = \dfrac{{G2m \times m}}{{{r^2}}}
Cancelling out the similar terms and simplifying the above equation we get, ω22(r3)=Gmr2{\omega _2}^2\left( {\dfrac{r}{3}} \right) = \dfrac{{Gm}}{{{r^2}}}
ω22=3Gmr3\Rightarrow {\omega _2}^2 = \dfrac{{3Gm}}{{{r^3}}} or ω2=3Gmr3{\omega _2} = \sqrt {\dfrac{{3Gm}}{{{r^3}}}}
Thus two stars have the same angular velocity ω1=ω2=ω=3Gmr3{\omega _1} = {\omega _2} = \omega = \sqrt {\dfrac{{3Gm}}{{{r^3}}}}
Then the period of revolution of the heavier star will be the same as that of the lighter star given by, T1=T2=2πr33Gm{T_1} = {T_2} = 2\pi \sqrt {\dfrac{{{r^3}}}{{3Gm}}} .
So option C is incorrect.
Step 3: Express the relation for the kinetic energies of the two stars
The kinetic energy of the lighter star of mass mm is given by, K1=12m(r1ω)2{K_1} = \dfrac{1}{2}m{\left( {{r_1}\omega } \right)^2} ------ (1)
Substituting for r1=2r3{r_1} = \dfrac{{2r}}{3} in equation (1) we get, K1=12m(2r3)2×ω2=2mr2ω29{K_1} = \dfrac{1}{2}m{\left( {\dfrac{{2r}}{3}} \right)^2} \times {\omega ^2} = \dfrac{{2m{r^2}{\omega ^2}}}{9}
Thus the kinetic energy of the lighter star is K1=2mr2ω29{K_1} = \dfrac{{2m{r^2}{\omega ^2}}}{9}
For the heavier star, the kinetic energy will be K2=12×2m(r2ω)2{K_2} = \dfrac{1}{2} \times 2m{\left( {{r_2}\omega } \right)^2} ------- (2)
Substituting for r2=r3{r_2} = \dfrac{r}{3} in equation (2) we get, K2=12×2m(r3)2×ω2=mr2ω29{K_2} = \dfrac{1}{2} \times 2m{\left( {\dfrac{r}{3}} \right)^2} \times {\omega ^2} = \dfrac{{m{r^2}{\omega ^2}}}{9}
Thus the kinetic energy of the heavier star is K2=mr2ω29{K_2} = \dfrac{{m{r^2}{\omega ^2}}}{9}
So we have K1=2K2{K_1} = 2{K_2}
So option B is incorrect.
Step 4: Express the relation for the angular momentum of the two stars.
For the lighter star, the angular momentum is L1=mr12ω=4mr2ω9{L_1} = m{r_1}^2\omega = \dfrac{{4m{r^2}\omega }}{9}
For the heavier star, the angular momentum is L1=mr22ω=mr2ω9{L_1} = m{r_2}^2\omega = \dfrac{{m{r^2}\omega }}{9}
So we have L1>L2{L_1} > {L_2} .

Thus the correct option is D.

Note: The position of the centre of mass of a system consisting of two different masses will be closer to the heavier mass. This idea was used while sketching the figure of the double-star system. As the two stars rotate in their circular orbit, the centre of mass of the double-star system will remain stationary. The relation for the linear velocity v=rωv = r\omega is used while expressing the centripetal force, kinetic energy and angular momentum of the stars.