A planet around a star of spectroscopically determined mass is detected both by…

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

Stars from the Inside, Ch Planetary systems: formation estimates, transits and the atmospheres of other worlds

Problem

A planet around a star of spectroscopically determined mass M∗=1.00 M⊙M_* = 1.00\,M_\odot is detected both by radial velocity and by transit photometry, on a circular orbit of period P=5.00 dP = 5.00\,\mathrm{d}. The radial-velocity curve has semi-amplitude K=40 m s−1K = 40\,\mathrm{m\,s^{-1}}. The transit light curve has depth δ=1.00%\delta = 1.00\%, total duration T14=4.04 hT_{14} = 4.04\,\mathrm{h} (first to fourth contact) and flat-bottom duration T23=3.24 hT_{23} = 3.24\,\mathrm{h} (second to third contact). ((a)) The spectroscopic-binary mass function for a single-lined system is f(m)=PK32πG=(mpsin⁡i)3(M∗+mp)2f(m) = \dfrac{PK^3}{2\pi G} = \dfrac{(m_p\sin i)^3}{(M_* + m_p)^2} for a circular orbit. Take the limit mp≪M∗m_p \ll M_* to find the planet's minimum mass mpsin⁡im_p\sin i, in Jupiter masses. ((b)) From δ\delta, T14T_{14} and T23T_{23} find the radius ratio k=Rp/R∗k = R_p/R_*, the impact parameter bb, and a/R∗a/R_*. ((c)) Use a/R∗a/R_* and Kepler's third law to find the star's mean density ρ∗\rho_*, and compare it with the Sun's mean density, 1.41×103 kg m−31.41\times10^{3}\,\mathrm{kg\,m^{-3}}. State whether the comparison is consistent with an unevolved Sun-like star of this mass.

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