TY - JOUR
T1 - Frequency dependence of tidal Q
AU - Greenberg, Richard
N1 - Funding Information:
I thank Rory Barnes and Brian Jackson for inspiring conversations, and Stanton Peale, Sylvio Ferraz-Mello, and Michael Efroimsky for comments on the manuscript. This research is supported by NASA’s Planetary Geology and Geophysics program.
Publisher Copyright:
© 2009. The American Astronomical Society. All rights reserved.
PY - 2009/6/10
Y1 - 2009/6/10
N2 - For studies of tidal evolution, values of the key parameter Q, and its frequency dependence, are often derived from estimates of internal energy dissipation when a satellite, planet, or star is physically distorted. Such estimates come from geophysical or astrophysical modeling, from seismic data, from ad hoc assumptions, or from constraints based on current spins and orbits. In a standard procedure, Q values are used to determine the lag in the response to each Fourier component of the tidal potential. The separate components are then co-added. The basis for this procedure is the analogy of the damped, driven, harmonic oscillator. However, this lag-and-add procedure would not be justifiable even for such a simple system, except for a very specific dependence of Q on frequency. There is no reason to expect the lag-and-add procedure to be relevant for a complex system, because the relationship between dissipation rates and tidal lags is unknown. This widely applied type of model is a reasonable approximation only if the decomposed tidal potential involves a narrow range of frequencies, and thus may only be appropriate for analyses to low order in orbital eccentricity and inclination.
AB - For studies of tidal evolution, values of the key parameter Q, and its frequency dependence, are often derived from estimates of internal energy dissipation when a satellite, planet, or star is physically distorted. Such estimates come from geophysical or astrophysical modeling, from seismic data, from ad hoc assumptions, or from constraints based on current spins and orbits. In a standard procedure, Q values are used to determine the lag in the response to each Fourier component of the tidal potential. The separate components are then co-added. The basis for this procedure is the analogy of the damped, driven, harmonic oscillator. However, this lag-and-add procedure would not be justifiable even for such a simple system, except for a very specific dependence of Q on frequency. There is no reason to expect the lag-and-add procedure to be relevant for a complex system, because the relationship between dissipation rates and tidal lags is unknown. This widely applied type of model is a reasonable approximation only if the decomposed tidal potential involves a narrow range of frequencies, and thus may only be appropriate for analyses to low order in orbital eccentricity and inclination.
KW - Celestial mechanics
KW - Planetary systems
KW - Planets and satellites: general
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U2 - 10.1088/0004-6256X/698/1/L42
DO - 10.1088/0004-6256X/698/1/L42
M3 - Article
AN - SCOPUS:85037703071
SN - 2041-8205
VL - 698
SP - L42-L45
JO - Astrophysical Journal Letters
JF - Astrophysical Journal Letters
IS - 1
ER -