In a globular cluster

PHYSICS · Multi-part · Fermi University Physics · Astrophysics & Cosmology · Stellar death and compact objects · Astrophysical fluid dynamics and plasmas

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

Problem

In a globular cluster, a metal-poor 0.8 M⊙0.8\,M_\odot giant fills its Roche lobe and feeds a neutron star of mass M=1.4 M⊙M = 1.4\,M_\odot, radius R∗=10 kmR_* = 10\,\mathrm{km}, moment of inertia I=1.0×1038 kg m2I = 1.0\times10^{38}\,\mathrm{kg\,m^2} and surface dipole field B∗=3.0×104 TB_* = 3.0\times10^{4}\,\mathrm{T}. The giant's nuclear evolution drives transfer at M˙=1.0×10−9 M⊙ yr−1\dot M = 1.0\times10^{-9}\,M_\odot\,\mathrm{yr^{-1}}, and the neutron star starts out spinning slowly. ((a)) Compute the accretion efficiency η=GM/R∗c2\eta = GM/R_*c^2 and the accretion luminosity L=ηM˙c2L = \eta\dot Mc^2, and compare LL with the Eddington luminosity LEdd=4πGMmpc/σTL_{\rm Edd} = 4\pi GMm_pc/\sigma_T. Can the neutron star take all the gas it is offered? ((b)) Compute the magnetospheric radius rm=[2πB∗2R∗6/(μ0M˙2GM)]2/7r_m = \left[2\pi B_*^2R_*^6/(\mu_0\dot M\sqrt{2GM})\right]^{2/7} and the equilibrium spin period Peq=2πrm3/GMP_{\rm eq} = 2\pi\sqrt{r_m^3/GM}. ((c)) Gas that joins the star from the disc's inner edge brings with it the specific angular momentum of a Keplerian orbit at rmr_m. Show that the spin-up torque is N=M˙GMrmN = \dot M\sqrt{GMr_m}, and estimate the time needed to spin the star up from a slow spin to PeqP_{\rm eq}, holding M˙\dot M, rmr_m and II fixed. ((d)) How much mass does the neutron star accrete in that time? Compare it with the 0.6 M⊙0.6\,M_\odot envelope the giant can give before only its 0.2 M⊙0.2\,M_\odot helium core is left, and say whether this binary can recycle the neutron star into a millisecond pulsar.

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