A transiting planet around a star gives a light curve with transit depth

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 transiting planet around a star gives a light curve with transit depth δ=0.0100\delta = 0.0100, period P=1.20 dP = 1.20\,\mathrm{d}, total transit duration T14=1.30 hT_{14} = 1.30\,\mathrm{h} and flat-bottom duration T23=1.05 hT_{23} = 1.05\,\mathrm{h}. Assume a circular, near edge-on orbit so that T14≈(P/π)(R∗/a)(1+k)2−b2T_{14}\approx (P/\pi)(R_*/a)\sqrt{(1+k)^2-b^2} and T23≈(P/π)(R∗/a)(1−k)2−b2T_{23}\approx (P/\pi)(R_*/a)\sqrt{(1-k)^2-b^2}, where k=Rp/R∗k = R_p/R_*. ((a)) Find kk, bb and a/R∗a/R_*. ((b)) Find the stellar mean density ρ∗\rho_*. ((c)) The Rossiter-McLaughlin anomaly for this system is antisymmetric about mid-transit, positive (redshifted) in the first half of the transit and equal and opposite in the second, with a peak amplitude of 15 m s−115\,\mathrm{m\,s^{-1}}, and the star has vsin⁡i∗=3.0 km s−1v\sin i_* = 3.0\,\mathrm{km\,s^{-1}}. Using Δv≈k2vsin⁡i∗1−b2\Delta v \approx k^2v\sin i_*\sqrt{1-b^2}, comment on whether the data are consistent with λ≈0\lambda\approx0.

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