Moons of Saturn 14 October 2013
Jan 29, 2016
Moons of Saturn
14 October 2013
Iapetus
Mimas
Enceladus
Most large Jovian Planet satellites are smaller than our moon. Based on the geological principles controlling Terrestrial Planets, we expect cold, dead worlds,
covered by craters…
Io Europa Triton Enceladus Titan (Jupiter) (Neptune) (Saturn)
NOT SO!
Instead, we got Io (left) Enceladus (right) and other active moons.
Enceladus… the next Io???
Enceladus --- the next Io?
Magnetic perturbation-> local ionization
Stellar occultation -> gas in plumes
So, what is cryovolcanism?
Enceladus’ Cryovolcanic Style
Enceladus’ Cryovolcanic Style
• Enceladus jets: water escapes at ~200 kg/sec!
• Io’s eruptions don’t reach escape velocity!
• Why the difference?
UVIS
UVIS has 4 separate channels:
• Far UltraViolet (FUV)• 110 to 190 nm
• 3 slit widths => 2.8, 4.8, 24.9 nm spectral resolution
• 2D detector: 1024 spectral x 64 one-mrad spatial pixels
• Extreme UltraViolet (EUV)• 55 to 110 nm
• 3 slit widths => 2.8, 4.8, 19.4 nm spectral resolution
• 2D detector: 1024 spectral x 64 one-mrad spatial pixels
• Solar occultation port
• High Speed Photometer (HSP)• 2 - 8 msec time resolution
• Hydrogen – Deuterium Absorption Cell (HDAC)
For the occultations we used the • HSP with 2 msec time resolution• FUV with 512 spectral channels (1.56 nm resolution), 5 sec integration time
UVIS
UVIS has 4 separate channels:
• Far UltraViolet (FUV)• 110 to 190 nm
• 3 slit widths => 2.8, 4.8, 24.9 nm spectral resolution
• 2D detector: 1024 spectral x 64 one-mrad spatial pixels
• Extreme UltraViolet (EUV)• 55 to 110 nm
• 3 slit widths => 2.8, 4.8, 19.4 nm spectral resolution
• 2D detector: 1024 spectral x 64 one-mrad spatial pixels
• Solar occultation port
• High Speed Photometer (HSP)• 2 - 8 msec time resolution
• Hydrogen – Deuterium Absorption Cell (HDAC)
For the occultations we used the • HSP with 2 msec time resolution• FUV with 512 spectral channels (1.56 nm resolution), 5 sec integration time
Plume Composition is Water Vapor
The absorption spectrum of water is shown compared to Enceladus’ plume spectrum (I/I0) for a water column density of n = 1.5 x 1016 cm-2
I=I0 exp (-n*)
I0 computed from 25 unocculted samples
n = column density
= absorption cross-section, function of wavelength
Estimation of Enceladus Water Flux
• S = flux = N * h2 * v = n/h * h2 * v = n * h * v
WhereN = number density / cm3
h2 = areav = velocityn = column density measured by UVIS
Estimate h from plume dimension, = 80 km
Estimate v from thermal velocity of water molecules in vapor pressure equilibrium with warm ice (600 m/sec for surface temperature ~ 180K – note that escape velocity = 230 m/sec)
S = 1.5 x 1016 * 80 x 105 * 60 x 103 = 0.7 x 1028 H2O molecules / sec
= 200 kg / sec
h
v
Plume Structure (2005)
Water vapor abundance calculated from each 5 sec spectrum.
The 2005 water profile is best fit by an exponential curve.
The best fit scale length is 80 km
Enceladus Plume Occultation of zeta Orionis October 2007
• In October 2007 zeta Orionis was occulted by Enceladus’ plume• Perfect geometry to get a horizontal cut through the plume and detect density variations indicative of gas jets• Objective was to see if there are gas jets corresponding to dust jets detected in images
Groundtrack of Ray
2005 2007
Enhanced HSP absorption features a, b, c, and d can be mapped to dust jets located by Spitale and Porco (2007) along the tiger stripes
Plume or jets?
• The plume of gas and dust from Enceladus includes a number of individual jets seen by Cassini camera and by UVIS
Best fit of 8 sources from Spitale & Porco to match UVIS occultation profile
Brightness of water vapor over Enceladus South pole from UVIS 8-jet model
Tiger Stripes
IR images -> Temperature:Tiger Stripesare warm.
Tiger Stripes close-up
Even closer!