A double-lined eclipsing binary has a circular orbit ( )

PHYSICS · Multi-part · Fermi University Physics · Astrophysics & Cosmology · Celestial mechanics and planetary systems · Celestial mechanics and planetary systems

Stars from the Inside, Ch Binary stars: fitted orbits, modelled eclipses and the Roche geometry

Problem

A double-lined eclipsing binary has a circular orbit (e=0e=0), period P=4.00 dP = 4.00\,\mathrm{d}, and radial-velocity semi-amplitudes K1=150 km s−1K_1 = 150\,\mathrm{km\,s^{-1}} and K2=50 km s−1K_2 = 50\,\mathrm{km\,s^{-1}}. Its light curve shows total eclipses consistent only with an inclination indistinguishable from i=90∘i=90^\circ (edge-on). The light-curve model gives fractional radii corresponding to actual radii R1=4.60 R⊙R_1 = 4.60\,R_\odot (the star whose own velocity amplitude is K1K_1) and R2=1.60 R⊙R_2 = 1.60\,R_\odot (the star whose own velocity amplitude is K2K_2). You may use the double-lined mass relations m1sin⁡3i=P(1−e2)3/2(K1+K2)2K22πG,m2sin⁡3i=P(1−e2)3/2(K1+K2)2K12πG,\begin{aligned} m_{1}\sin^3 i &= \frac{P(1-e^2)^{3/2}(K_1+K_2)^2K_2}{2\pi G}, \\ m_{2}\sin^3 i &= \frac{P(1-e^2)^{3/2}(K_1+K_2)^2K_1}{2\pi G}, \end{aligned} and the Eggleton formula for the volume-equivalent Roche-lobe radius of a star of mass ratio qq (its own mass over its companion's), rLa=0.49 q2/30.6 q2/3+ln⁡(1+q1/3).\frac{r_L}{a} = \frac{0.49\,q^{2/3}}{0.6\,q^{2/3}+\ln(1+q^{1/3})}. ((a)) Find the masses m1m_1 and m2m_2 in solar masses. ((b)) Find the orbital separation aa in solar radii. ((c)) Find the Roche-lobe radius of each star, and decide whether each star lies inside, or fills, its lobe. ((d)) Classify the system as detached, semi-detached or contact, and state which star (if any) is transferring mass. ((e)) Given that, all else equal, a more massive star exhausts its core hydrogen and evolves off the main sequence sooner than a less massive star born at the same time, explain the puzzle this system's masses and radii pose.

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