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Imke	
  de	
  Pater	
  (UC	
  Berkeley)	
  
Outline
• Jupiter:	
  the	
  planet
• Why	
  study	
  Jupiter?	
  Origin	
  of	
  	
  our	
  Solar	
  System
• Recent	
  work	
  by	
  our	
  group
• The	
  Juno	
  Mission
HST/NASA
• Largest	
  planet	
  in	
  our	
  SS
• ~12	
  x	
  larger	
  than	
  Earth
• ~300	
  times	
  more	
  mass
• ~85%	
  H2,	
  15%	
  He
• trace	
  amounts	
  CH4,	
  NH3,	
  
H2O,	
  H2S	
  (on	
  Sun:	
  C,N,O,S)
Cassini,	
  Oct.	
  31	
  – Nov.	
  9,	
  2000
HST/NASA
Cassini,	
  Oct.	
  31	
  – Nov.	
  9,	
  2000
HST/NASA
So,	
  Why	
  study	
  Jupiter?
• Composition	
  and	
  internal	
  
structure	
  Jupiter	
  à
information	
  on	
  conditions	
  
of	
  our	
  solar	
  nebula	
  during	
  
the	
  time	
  the	
  Sun	
  and	
  
planets	
  formed.
Fundamental	
  Question:	
  
How	
  did	
  our	
  Solar	
  System	
  Form?
Composition	
  of	
  a	
  planet	
  can	
  be	
  determined	
  
through	
  remote	
  sensing	
  or	
  in	
  situ	
  (probe)
IRTF
20
0
titude
o
o
a b c
Visible	
  	
  (HST)	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  5	
  µm	
  (IRTF)	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  2	
  cm	
  (VLA)
1995-­‐1996:	
  Galileo	
  Probe	
  entry
Determine	
  composition	
  through	
  
observations	
  at	
  different	
  wavelengths
Beebe	
   Ortiz	
  et	
  al.,	
  1998 de	
  Pater	
  et	
  al.	
  2001
IRTF
20
0
titude
o
o
a b c
Visible	
  	
  (HST)	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  5	
  µm	
  (IRTF)	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  	
  2	
  cm	
  (VLA)
1995-­‐1996:	
  Galileo	
  Probe	
  entry
Radio: clouds	
  are	
  transparant;	
  
Most	
  of	
  the	
  opacity	
  is	
  caused	
  
by	
  NH3 gas.	
  At	
  longer	
  
wavelengths	
  radiation	
  is	
  
received	
  from	
  deeper	
  levels	
  
in	
  the	
  atmosphere.	
  à NH3
abundance	
  very	
  similar	
  to	
  
solar	
  N	
  value.	
  
Beebe	
   Ortiz	
  et	
  al.,	
  1998 de	
  Pater	
  et	
  al.	
  2001
Two	
  questions	
  surface:	
  
• What	
  is	
  the	
  H2O	
  abundance	
  in	
  Jupiter’s	
  deep	
  atmosphere?
• How	
  to	
  reconcile	
  the	
  groundbased (radio)	
  measurement	
  
of	
  NH3 with	
  the	
  Galileo	
  Probe	
  data?
Owen	
  et	
  al.	
  1999
How	
  can	
  we	
  “loose”	
  NH3 gas	
  between	
  4 and	
  8	
  bar?
• Chemistry;	
  perhaps	
  H2S	
  binds	
  with	
  more	
  than	
  1	
  NH3
molecules?	
  Or	
  the	
  water	
  cloud	
  takes	
  up	
  more	
  NH3	
  than	
  
hitherto	
  assumed?	
  Lab	
  work	
  ongoing
• Dynamics:	
  updrafts,	
  downdrafts,	
  drying	
  out	
  air,	
  as	
  the	
  
zone-­‐belt	
  generic	
  picture.
10–16
10–14
10–12
10–10
10–8
Cloud density rate Rx
(g cm–3
cm–1
)
300
250
200
150
Temperature(K)
7.0
5.0
4.0
3.0
2.0
1.5
1.0
0.5
0.75
Pressure(bar)
Water solution
Water ice
NH4
SH solid
NH3
ice
Wong	
  et	
  al.,	
  2014
In	
  order	
  to	
  solve	
  the	
  NH3 and	
  H2O	
  questions,	
  we	
  
obtained	
  data	
  to	
  probe	
  below	
  Jupiter’s	
  clouds:
• Spectroscopic	
  data	
  at	
  5	
  µm
• Maps	
  at	
  radio	
  wavelengths	
  at	
  2-­‐6	
  cm	
  (4-­‐18	
  GHz)	
  
De	
  Pater	
  et	
  al.,	
  2011
5-­‐µm	
  image	
  of	
  Jupiter’s	
  
northern	
  hemisphere.
In	
  hot	
  regions	
  (hot	
  
spots,	
  5-­‐µm	
  rings	
  
around	
  vortices)	
  we	
  
probe	
  down	
  to	
  5-­‐7	
  bar
Bjoraker et	
  al.,	
  2015
Zones	
  exhibit	
  narrow	
  CH3D	
  line	
  
profiles.	
  Modeling	
  indicates	
  the	
  
presence	
  of	
  a	
  cloud	
  at	
  ~4	
  bars,	
  which	
  
must	
  be	
  a	
  water	
  cloud.
à Consistent	
  with	
  historical	
  picture	
  of	
  
rising	
  air	
  in	
  zones,	
  sinking	
  in	
  belts;	
  H2O	
  
must	
  be	
  >1.2	
  x	
  solar	
  O.
Hot	
  Spots,	
  Belts,	
  
and	
  high-­‐latitude	
  
regions	
  exhibit	
  
broad	
  CH3D	
  line	
  
profiles	
  
àprobing	
  ~7	
  bar	
  
àNo	
  opaque	
  H2O	
  
clouds.
5-­‐µm	
  Spectra
de	
  Pater	
  et	
  al.,	
  2016
Radio	
  observations	
  at	
  2	
  -­‐ 6	
  cm	
  (or	
  4	
  – 18	
  GHz)	
  
NH3
Solution
H2
O
NH4
SH
Equilibrium NH3
(Fig. 3A, profile a)
Depleted NH3
(Fig. 3A, profile e)
17.4 GHz
4.42 GHz
7.45 GHz
11.5 GHz
14.2 GHz
1.46 GHz
17.4 GHz
4.42 GHz
7.45 GHz
11.5 GHz
14.2 GHz
1.46 GHz
A B
Fig. 1
0
10
1
0.1
10
1
0.1
0.5 1 1.5
100 200 300 400
Normalized contribution functions
Pressure(bar)
Pressure(bar)
Temperature (K)
0 0.5 1 1.5
100 200 300 400
Normalized contribution functions
Temperature (K)
JUPITER:
Radio spectrum
Temperature (K)
De	
  Pater	
  et	
  al.,	
  2016
NH4SH	
  à
NH3-­‐ice	
  à
brg c
Temperature (K)
TP profile
de	
  Pater	
  et	
  al.,	
  2016
de	
  Pater	
  et	
  al.,	
  2016
2	
  cm
2	
  cm
6 cm
3.5	
  cm
de	
  Pater	
  et	
  al.,	
  2016
SUMMARY:	
  
• Microwave	
  maps	
  show	
  spatial	
  
variations	
  in	
  Tb,	
  resembling	
  
visible	
  light	
  maps.	
  
• Radio-­‐hot	
  belt	
  at	
  ~8	
  deg N
• Localized	
  NH3 depletions	
  
(hot	
  spots)	
  down	
  to	
  >	
  8	
  bar
• Localized	
  upwellings (plumes)	
  from	
  P	
  >	
  8	
  bar:	
  planetary	
  
wave,	
  connecting	
  the	
  5-­‐µm hot	
  spots	
  and	
  plumes.
• Plumes	
  explain	
  radio	
  – Galileo	
  conundrum
NASA’s	
  Juno	
  Mission
• Launch	
  Aug	
  5th 2011.
• Arrival	
  July	
  4th 2016	
  
• 2700	
  miles	
  above	
  the	
  jovian
cloud	
  tops	
  in	
  a	
  polar	
  orbit
• Key	
  goals:
– Gravity	
  field	
  mapping	
  to	
  
detect	
  the	
  presence	
  of	
  a	
  
core.	
  
– Microwave	
  mapping	
  to	
  
peer	
  beneath	
  the	
  clouds,	
  
constrain	
  oxygen.
• 32	
  orbits:	
  	
  1-­‐8	
  for	
  remote	
  
sensing	
  and	
  microwave.
• 9-­‐32	
  for	
  gravity	
  mapping
• De-­‐orbit	
  March	
  2018.
Slide	
  adapted	
  from	
  Orton
26
Juno’s	
  	
  Specific	
  Science	
  Objectives
Origin
Determine	
  water	
  abundance	
  and	
  constrain	
  
core	
  mass	
  to	
  decide	
  among	
  alternative	
  
theories	
  of	
  origin.
Interior
Understand	
  Jupiter's	
  interior	
  structure	
  and	
  
dynamical	
  properties	
  by	
  mapping	
  its	
  
gravitational	
  and	
  magnetic	
  fields
Atmosphere
Map	
  variations	
  in	
  atmospheric	
  
composition,	
  cloud	
  opacity	
  and	
  dynamics	
  
to	
  depths	
  greater	
  than	
  100	
  bars	
  at	
  all	
  
latitudes.
Magnetosphere
Characterize	
  the	
  three-­‐dimensional	
  
structure	
  of	
  Jupiter's	
  polar	
  magnetosphere	
  
and	
  auroras.
Slide	
  adapted	
  from	
  Orton
Probing	
  the	
  deep	
  interior	
  from	
  orbit
Juno	
  maps	
  Jupiter	
  from	
  the	
  deepest	
  interior	
  to	
  the	
  atmosphere	
  
using	
  microwaves,	
  and	
  magnetic	
  and	
  gravity	
  fields.
Slide	
  adapted	
  from	
  Orton
Mapping	
  Jupiter’s	
  gravity
Tracking	
  changes	
  in	
  Juno’s	
  
velocity	
  reveals	
  Jupiter’s	
  
gravity	
  (and	
  how	
  the	
  planet	
  
is	
  arranged	
  on	
  the	
  inside).
Precise	
  Doppler	
  measurements	
  of	
  
spacecraft	
  motion	
  reveal	
  the	
  gravity	
  
field.
Slide	
  adapted	
  from	
  Orton
Juno’s  Microwave  Radiometer  
measures  thermal  radiation  from  
the  atmosphere  to  as  deep  as  a  
few  100  bar  pressure  (few  100  km  
below  the  visible  cloud  tops).    
Sensing	
  the	
  deep	
  atmosphere	
  
Goal:  to  determine  the  3D  
H2O  and  NH3 abundances.
Sensing	
  the	
  deep	
  atmosphere	
  
At	
  wavelengths	
  >	
  6	
  cm	
  (freqs<	
  4	
  GHz)	
  Jupiter’s	
  
synchrotron	
  radiation	
  makes	
  it	
  very	
  difficult	
  to	
  
map	
  the	
  atmosphere	
  from	
  the	
  Earth.	
  Juno	
  flies	
  
inside	
  the	
  radiation	
  belts.	
  	
  VLA	
  map	
  at	
  21	
  cm;	
  
de	
  Pater	
  et	
  al.,	
  1997
Juno’s	
  field	
  of	
  view	
  is	
  tiny	
  à need	
  context	
  maps.
Slide	
  adapted	
  from	
  Bagenal
Mapping	
  Jupiter’s	
  magnetic	
  field	
  and	
  aurora
HST/NASA
Ground-­‐based	
  observing	
  campaign	
  to	
  support	
  Juno
• Dedicated	
  network	
  of	
  amateur	
  astronomers.	
  
• Many	
  telescopes	
  allocated	
  time,	
  from	
  X-­‐rays	
  to	
  uv-­‐visible,	
  near-­‐
and	
  mid-­‐infrared,	
  and	
  radio	
  from	
  cm—m	
  wavelengths.
• Unique	
  opportunity	
  to	
  characterize	
  Jupiter’s	
  atmosphere	
  from	
  
the	
  stratosphere	
  down	
  to	
  100’s	
  of	
  bars.	
  Time	
  variability	
  
mandates	
  simultaneous	
  data	
  to	
  fully	
  characterize	
  the	
  planet.
• Synergy	
  VLA	
  &	
  Juno:	
  VLA	
  provides	
  context	
  maps	
  to	
  put	
  Juno	
  
MWR	
  data	
  in	
  perspective;	
  Juno	
  extends	
  the	
  information	
  to	
  
much	
  deeper	
  levels.	
  Juno	
  also	
  has	
  a	
  superb	
  view	
  of	
  the	
  poles.

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Galaxy Forum USA 2016 - Prof Imke de Pater, UC Berkeley

  • 1. Imke  de  Pater  (UC  Berkeley)   Outline • Jupiter:  the  planet • Why  study  Jupiter?  Origin  of    our  Solar  System • Recent  work  by  our  group • The  Juno  Mission HST/NASA
  • 2. • Largest  planet  in  our  SS • ~12  x  larger  than  Earth • ~300  times  more  mass • ~85%  H2,  15%  He • trace  amounts  CH4,  NH3,   H2O,  H2S  (on  Sun:  C,N,O,S) Cassini,  Oct.  31  – Nov.  9,  2000 HST/NASA
  • 3. Cassini,  Oct.  31  – Nov.  9,  2000 HST/NASA So,  Why  study  Jupiter?
  • 4. • Composition  and  internal   structure  Jupiter  à information  on  conditions   of  our  solar  nebula  during   the  time  the  Sun  and   planets  formed. Fundamental  Question:   How  did  our  Solar  System  Form? Composition  of  a  planet  can  be  determined   through  remote  sensing  or  in  situ  (probe)
  • 5. IRTF 20 0 titude o o a b c Visible    (HST)                                      5  µm  (IRTF)                            2  cm  (VLA) 1995-­‐1996:  Galileo  Probe  entry Determine  composition  through   observations  at  different  wavelengths Beebe   Ortiz  et  al.,  1998 de  Pater  et  al.  2001
  • 6. IRTF 20 0 titude o o a b c Visible    (HST)                                      5  µm  (IRTF)                            2  cm  (VLA) 1995-­‐1996:  Galileo  Probe  entry Radio: clouds  are  transparant;   Most  of  the  opacity  is  caused   by  NH3 gas.  At  longer   wavelengths  radiation  is   received  from  deeper  levels   in  the  atmosphere.  à NH3 abundance  very  similar  to   solar  N  value.   Beebe   Ortiz  et  al.,  1998 de  Pater  et  al.  2001
  • 7. Two  questions  surface:   • What  is  the  H2O  abundance  in  Jupiter’s  deep  atmosphere? • How  to  reconcile  the  groundbased (radio)  measurement   of  NH3 with  the  Galileo  Probe  data? Owen  et  al.  1999
  • 8. How  can  we  “loose”  NH3 gas  between  4 and  8  bar? • Chemistry;  perhaps  H2S  binds  with  more  than  1  NH3 molecules?  Or  the  water  cloud  takes  up  more  NH3  than   hitherto  assumed?  Lab  work  ongoing • Dynamics:  updrafts,  downdrafts,  drying  out  air,  as  the   zone-­‐belt  generic  picture. 10–16 10–14 10–12 10–10 10–8 Cloud density rate Rx (g cm–3 cm–1 ) 300 250 200 150 Temperature(K) 7.0 5.0 4.0 3.0 2.0 1.5 1.0 0.5 0.75 Pressure(bar) Water solution Water ice NH4 SH solid NH3 ice Wong  et  al.,  2014
  • 9. In  order  to  solve  the  NH3 and  H2O  questions,  we   obtained  data  to  probe  below  Jupiter’s  clouds: • Spectroscopic  data  at  5  µm • Maps  at  radio  wavelengths  at  2-­‐6  cm  (4-­‐18  GHz)   De  Pater  et  al.,  2011 5-­‐µm  image  of  Jupiter’s   northern  hemisphere. In  hot  regions  (hot   spots,  5-­‐µm  rings   around  vortices)  we   probe  down  to  5-­‐7  bar
  • 10. Bjoraker et  al.,  2015 Zones  exhibit  narrow  CH3D  line   profiles.  Modeling  indicates  the   presence  of  a  cloud  at  ~4  bars,  which   must  be  a  water  cloud. à Consistent  with  historical  picture  of   rising  air  in  zones,  sinking  in  belts;  H2O   must  be  >1.2  x  solar  O. Hot  Spots,  Belts,   and  high-­‐latitude   regions  exhibit   broad  CH3D  line   profiles   àprobing  ~7  bar   àNo  opaque  H2O   clouds. 5-­‐µm  Spectra
  • 11. de  Pater  et  al.,  2016 Radio  observations  at  2  -­‐ 6  cm  (or  4  – 18  GHz)   NH3 Solution H2 O NH4 SH Equilibrium NH3 (Fig. 3A, profile a) Depleted NH3 (Fig. 3A, profile e) 17.4 GHz 4.42 GHz 7.45 GHz 11.5 GHz 14.2 GHz 1.46 GHz 17.4 GHz 4.42 GHz 7.45 GHz 11.5 GHz 14.2 GHz 1.46 GHz A B Fig. 1 0 10 1 0.1 10 1 0.1 0.5 1 1.5 100 200 300 400 Normalized contribution functions Pressure(bar) Pressure(bar) Temperature (K) 0 0.5 1 1.5 100 200 300 400 Normalized contribution functions Temperature (K)
  • 12. JUPITER: Radio spectrum Temperature (K) De  Pater  et  al.,  2016 NH4SH  à NH3-­‐ice  à
  • 13. brg c Temperature (K) TP profile de  Pater  et  al.,  2016
  • 14. de  Pater  et  al.,  2016 2  cm 2  cm 6 cm 3.5  cm
  • 15. de  Pater  et  al.,  2016
  • 16. SUMMARY:   • Microwave  maps  show  spatial   variations  in  Tb,  resembling   visible  light  maps.   • Radio-­‐hot  belt  at  ~8  deg N • Localized  NH3 depletions   (hot  spots)  down  to  >  8  bar • Localized  upwellings (plumes)  from  P  >  8  bar:  planetary   wave,  connecting  the  5-­‐µm hot  spots  and  plumes. • Plumes  explain  radio  – Galileo  conundrum
  • 17. NASA’s  Juno  Mission • Launch  Aug  5th 2011. • Arrival  July  4th 2016   • 2700  miles  above  the  jovian cloud  tops  in  a  polar  orbit • Key  goals: – Gravity  field  mapping  to   detect  the  presence  of  a   core.   – Microwave  mapping  to   peer  beneath  the  clouds,   constrain  oxygen. • 32  orbits:    1-­‐8  for  remote   sensing  and  microwave. • 9-­‐32  for  gravity  mapping • De-­‐orbit  March  2018. Slide  adapted  from  Orton
  • 18. 26 Juno’s    Specific  Science  Objectives Origin Determine  water  abundance  and  constrain   core  mass  to  decide  among  alternative   theories  of  origin. Interior Understand  Jupiter's  interior  structure  and   dynamical  properties  by  mapping  its   gravitational  and  magnetic  fields Atmosphere Map  variations  in  atmospheric   composition,  cloud  opacity  and  dynamics   to  depths  greater  than  100  bars  at  all   latitudes. Magnetosphere Characterize  the  three-­‐dimensional   structure  of  Jupiter's  polar  magnetosphere   and  auroras. Slide  adapted  from  Orton
  • 19. Probing  the  deep  interior  from  orbit Juno  maps  Jupiter  from  the  deepest  interior  to  the  atmosphere   using  microwaves,  and  magnetic  and  gravity  fields. Slide  adapted  from  Orton
  • 20. Mapping  Jupiter’s  gravity Tracking  changes  in  Juno’s   velocity  reveals  Jupiter’s   gravity  (and  how  the  planet   is  arranged  on  the  inside). Precise  Doppler  measurements  of   spacecraft  motion  reveal  the  gravity   field. Slide  adapted  from  Orton
  • 21. Juno’s  Microwave  Radiometer   measures  thermal  radiation  from   the  atmosphere  to  as  deep  as  a   few  100  bar  pressure  (few  100  km   below  the  visible  cloud  tops).     Sensing  the  deep  atmosphere   Goal:  to  determine  the  3D   H2O  and  NH3 abundances.
  • 22. Sensing  the  deep  atmosphere   At  wavelengths  >  6  cm  (freqs<  4  GHz)  Jupiter’s   synchrotron  radiation  makes  it  very  difficult  to   map  the  atmosphere  from  the  Earth.  Juno  flies   inside  the  radiation  belts.    VLA  map  at  21  cm;   de  Pater  et  al.,  1997 Juno’s  field  of  view  is  tiny  à need  context  maps.
  • 23. Slide  adapted  from  Bagenal Mapping  Jupiter’s  magnetic  field  and  aurora HST/NASA
  • 24. Ground-­‐based  observing  campaign  to  support  Juno • Dedicated  network  of  amateur  astronomers.   • Many  telescopes  allocated  time,  from  X-­‐rays  to  uv-­‐visible,  near-­‐ and  mid-­‐infrared,  and  radio  from  cm—m  wavelengths. • Unique  opportunity  to  characterize  Jupiter’s  atmosphere  from   the  stratosphere  down  to  100’s  of  bars.  Time  variability   mandates  simultaneous  data  to  fully  characterize  the  planet. • Synergy  VLA  &  Juno:  VLA  provides  context  maps  to  put  Juno   MWR  data  in  perspective;  Juno  extends  the  information  to   much  deeper  levels.  Juno  also  has  a  superb  view  of  the  poles.