Spectroscopy of the X-ray transient GRO J1655 40 gives an orbital period

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

Stars from the Inside, Ch Accretion power: mass transfer, discs and the weighing of black holes

Problem

Spectroscopy of the X-ray transient GRO J1655−-40 gives an orbital period P=2.62 dP = 2.62\,\mathrm{d}, a radial-velocity semi-amplitude of the visible donor star K2=228 km s−1K_2 = 228\,\mathrm{km\,s^{-1}}, an orbital inclination i=70.2∘i = 70.2^\circ from ellipsoidal light-curve modelling, and a mass ratio q=M2/M1=0.334q = M_2/M_1 = 0.334 (donor mass over compact-object mass) from rotational broadening of the donor's absorption lines (Orosz & Bailyn 1997, ApJ 477, 876; van der Hooft et al. 1998, ApJ 494, 275). The maximum mass a neutron star's equation of state can support is taken as Mmax⁡,NS≈3 M⊙M_{\max,\rm NS} \approx 3\,M_\odot (Chapter 13). ((a)) Compute the mass function of the compact object, f(M1)=PK23/2πGf(M_1) = PK_2^3/2\pi G, and state what can be concluded about the nature of the compact object from this number alone, without using ii or qq. ((b)) Using M1sin⁡3i/(1+q)2=f(M1)M_1\sin^3i/(1+q)^2 = f(M_1), combine f(M1)f(M_1) with the quoted ii and qq to obtain the compact object's mass M1M_1.

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