Thalassa (moon) Monday, June 22, 2009


Thalassa

Naiad or Thalassa as seen by Voyager 2
(smearing has caused excessive elongation)
Discovery
Discovered by Richard J. Terrile[1] and Voyager Imaging Team
Discovered in September 1989
Orbital characteristics[2]
Epoch 18 August 1989
Semi-major axis 50 075 ± 1 km
Eccentricity 0.0002 ± 0.0002
Orbital period 0.31148444 ± 0.00000006 d
Inclination 0.21 ± 0.02° (to Neptune equator)

0.21° (to local Laplace plane)

Is a satellite of Neptune
Physical characteristics
Dimensions 108×100×52 km[3][4]
Mean radius 41 ± 3 km[5]
Mass ~3.5 × 1017 kg
(based on assumed density)
Mean density ~1.2 g/cm3 (estimate)
Rotation period assumed synchronous
Axial tilt ~zero presumably
Albedo (geometric) 0.09[3][4]
Surface temp. ~51 K mean (estimate)
Atmosphere none
A simulated view of Thalassa orbiting Neptune.

Thalassa (pronounced /θəˈlæsə/ thə-LASS, or as in Greek Θάλασσα), also known as Neptune IV, is the second innermost satellite of Neptune. Thalassa was named after a daughter of Aether and Hemera from Greek mythology. "Thalassa" is also the Greek word for "sea".

Thalassa was discovered sometime before mid-September, 1989 from the images taken by the Voyager 2 probe. It was given the temporary designation S/1989 N 5.[6] The discovery was announced (IAUC 4867) on September 29, 1989, but the text only talks of "25 frames taken over 11 days", giving a discovery date of sometime before September 18. The name was given on 16 September 1991[7].

Thalassa is irregularly shaped and shows no sign of any geological modification. It is likely that it is a rubble pile re-accreted from fragments of Neptune's original satellites, which were smashed up by perturbations from Triton soon after that moon's capture into a very eccentric initial orbit.[8] Unusually for irregular bodies, it appears to be roughly disk-shaped.

Since the Thalassian orbit is below Neptune's synchronous orbit radius, it is slowly spiralling inward due to tidal decceleration and may eventually impact Neptune's atmosphere, or break up into a planetary ring upon passing its Roche limit due to tidal stretching. Relatively soon after, the spreading debris may impinge upon Despina's

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