A different transiting planet gives , , ,

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 different transiting planet gives δ=0.0200\delta = 0.0200, P=2.50 dP = 2.50\,\mathrm{d}, T14=2.80 hT_{14} = 2.80\,\mathrm{h}, T23=2.00 hT_{23} = 2.00\,\mathrm{h}. Assume a circular, near edge-on orbit and the duration relations of the previous problem. ((a)) Find kk, bb and a/R∗a/R_*. ((b)) Find ρ∗\rho_*. ((c)) The star has vsin⁡i∗=5.0 km s−1v\sin i_* = 5.0\,\mathrm{km\,s^{-1}}. During transit the radial-velocity anomaly rises to +40 m s−1+40\,\mathrm{m\,s^{-1}} (redshifted) in the first half and then swings to −55 m s−1-55\,\mathrm{m\,s^{-1}} (blueshifted) in the second half, an asymmetric, time-skewed pattern. Compute the maximum anomaly expected for an aligned orbit and say what the observed asymmetry implies about λ\lambda.

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