Image Details
 
                    Caption: Figure 2.
Long-term integrations of orbital and rotational parameters of some transiting planets and their host star. Tidal quality
   parameters 
   Q′
   
       and 
   Q′
   
      p
    are initially set to 10
   6 but vary with the semimajor axis as 
   Q
    and 
   Q′
   
      p
    are initially set to 10
   6 but vary with the semimajor axis as 
   Q
   
       = 
   Q
      p
    = 1/(
   nΔ
   t) where Δ
   t is a constant tidal time lag. (a) Semimajor axis of OGLE-TR-132b, HD 209458b (solid lines), and eccentricity of HD 209458b
   (dashed line) as a function of time. The thin dashed line is the usual exponential damping approximation of 
   e with a 4.1 × 10
   8 yr relaxation time assuming that only tides raised on the planet are considered and stable tidal equilibrium states exist;
   (b) rotational periods of HD 209458, HD 209458b (solid lines), and HD 209458's obliquity (dashed line) as a function of time.
   The initial rotational period of HD 209458b and HD 209458 stellar obliquity are arbitrarily set to half a day and 20° to evaluate
   the respective timescales of their tidal evolution.
    = 
   Q
      p
    = 1/(
   nΔ
   t) where Δ
   t is a constant tidal time lag. (a) Semimajor axis of OGLE-TR-132b, HD 209458b (solid lines), and eccentricity of HD 209458b
   (dashed line) as a function of time. The thin dashed line is the usual exponential damping approximation of 
   e with a 4.1 × 10
   8 yr relaxation time assuming that only tides raised on the planet are considered and stable tidal equilibrium states exist;
   (b) rotational periods of HD 209458, HD 209458b (solid lines), and HD 209458's obliquity (dashed line) as a function of time.
   The initial rotational period of HD 209458b and HD 209458 stellar obliquity are arbitrarily set to half a day and 20° to evaluate
   the respective timescales of their tidal evolution.
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