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Io’s plasma interac0ons: 101 P. A. Delamere University of Colorado

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Page 1: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Io’s  plasma  interac0ons:  101  

P.  A.  Delamere  University  of  Colorado  

Page 2: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Issues  for  plasma  interac0ons  •  Energy  input  for  neutral  escape  (forma4on  of  corona  and  extended  neutral  clouds)    

•  Diagnos4c  of  atmospheric  composi4on,  distribu4on,  and  possible  asymmetry  

•  Io’s  aurora…diagnos4c  of  Io’s  atmosphere  

•  Torus  variability  linked  to  volcanic  ac4vity  (JAXA  EXCEED  mission)  

Steffl  et  al.,  2008  

Delamere  et  al.,  2004  

Page 3: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Types  of  interac0ons  •  Magne4zed  (internally  generated  magne4c  field)  – Mini-­‐magnetosphere  (Ganymede)  

•  Non-­‐magne4zed  –  Inert,  no  induced  magne4c  field  and  no  neutral  source  (e.g.  moon).    

–  Induced  magne4c  field  due  to  4me-­‐varying  external  magne4c  field  (e.g.  Europa  and  Io)  

– Magne4c  perturba4on  due  to  interac4on  with  neutral  source  (.e.g.  Io,  Enceladus)  

Page 4: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Pickup=source of energy

(at 60 km/s)

Tpu(O+)=270 eV

Tpu(S+)=540 eV

Tpu(SO2+)= 1080 eV

Interac0on  processes  

Page 5: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Momentum  loading  (pickup)  •  Ioniza4on  

•  Charge  exchange  

–  Ioniza4on  adds  mass  –  Charge  exchange  does  not  add  mass  (usually)  –  Pickup  involves  two  parts:  

•  Accelera4on  to  corota4on  speed  •  Hea4ng  at  local  flow  speed  (on  4me  scale  of  gyromo4on)  

–  Both  transfer  momentum  from  ambient  plasma  to  new  ions  

Page 6: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Ioniza0on  and  Charge  Exchange  

•  .CharCharge  

Ioniza4on  limited  by  electron  temperature  [Saur  et  al.,  1999;  Dols  et  al.,  2008]  

Charge  exchange  amplified  by  “seed”    ioniza4on.    Results  in  an  avalanche  of    reac4ons  [Fleshman  et  al.,  2011]  

Page 7: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Io’s  (par0al)  neutral  torus    

M.  Burger  

Page 8: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Electrodynamic  consequences  

•  Momentum  loading  generates  currents  

M•v = J ×BdV∫

J =∇ ×B

µo

Ioniza4on  +  charge  exchange  

Page 9: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Flow  around  a  conduc0ng  obstacle  

Dols  et  al.,  2008  

Page 10: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Ring  Beam  (pickup)  distribu0on  

B  

Page 11: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Momentum  transfer  •  Magne4c  field  perturba4on  due  to  “pick  up”  (e.g.  ioniza4on  and  charge  exchange)  

 •  Alfven  characteris4c  determined  plasma  mass  density  and  magne4c  field.  

vcor  

vA  

vcorvA

=δBx

Bz

Page 12: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Momentum  transfer  

•  Alfven  wing  magne4c  field  topology  results  in  forces  on  charged  par4cles  via  Maxwell  stresses.  – Accelera4on  of  iogenic  plasma  at  the  expense  of  torus  plasma.  

– Ul4mately,  Jupiter’s  atmospheric  is  the  source  of  momentum  and  energy.  

Page 13: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Es0mate  of  momentum  loading    •  Maxwell  stress    

•  Plasma  mass  coupling  rate  

•  Momentum  balance  requires  (ignoring  upstream  input,  chemical  processes)    

dpxdt

= 2(δBx )BzA /µo = (2ρtorusvAA)vx

MAlfven = 2ρtorusvAA =2PdAMAvcor

MAlfven =•

Mionization +•

Mchex ≈ 300 kg/s  

Page 14: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Momentum  transfer  

MAlfven

Mtorus€

MAlfven

Mionization

Mchex

Mtorus•

MAlfven

<1

Page 15: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Electron Beams

Galileo

Fresh hot ions

Flow

Magnetic field

Galileo  Io  Flyby  -­‐  1995  

Flux

NeV

x (10

10 c

m-2

s-1

)"

Y (RIo)"

Bagenal, [1997]

•  Is the local interaction ionosphere-like (elastic collision dominated), or comet-like (mass loading dominated)? •  Bagenal, [1997]: 200-500 (kg/s) •  Saur et al., [2003]: 50-200 (kg/s)

Y (RIo)

Bagenal, [1997]

Page 16: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona
Page 17: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

I = JA = JπRIo2 = 3×106(A)

V ≈ vB(2RIo) = 400(kV)

P =VI =1.2 ×1012(W)

Energe0cs  

Page 18: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Power  (Alfven  wave)  per  hemisphere:  5x1011  W  

Io  Interac4on:  ~1012  W  

IR+UV  auroral  spots:  109-­‐1010  W  

Io-­‐DAM:  109-­‐1010  W  

Precipita4ng  electrons  (100-­‐1000  eV):  ~1010-­‐1011  W  

Page 19: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

B  

Analysis  of  mass  loaded  systems  

Page 20: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Analysis  of  mass  loaded  systems  

Page 21: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Analysis  of  mass  loaded  systems  

Page 22: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Ion  Cyclotron  Waves  B  

Page 23: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Ion  Cyclotron  Waves  

SO+  SO2

+  

Page 24: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Ion  Cyclotron  Waves  

Russell  and  Kivelson,  2001  

Huddleston  et  al.,  1997  

Page 25: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Galileo  Magnetometer  Data  

0.4 0.6 0.8 10

10

20

30

40

Frequency (Hz)

Pow

er/fr

eque

ncy

(Arb

itrar

y lo

g sc

ale)

32 amu 48 amu 64 amuA

Freq

uenc

y (H

z)

1.3 (C.A.) 2 3 4 RIo 32 amu

48 amu

64 amu

A BA B04:35 04:40 04:450.25

0.50

0.75

1.00

0.4 0.6 0.8 10

10

20

30

40

Frequency (Hz)

Pow

er/fr

eque

ncy

(Arb

itrar

y lo

g sc

ale)

32 amu 48 amu 64 amuB

Page 26: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Analysis  of  plasma  data  in  Io’s  wake  Upstream   Wake  

Frank  and  Paterson,  2002  

Page 27: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Hybrid  Simula0ons    (“synthe0c  par0cle  data”)  

Energy  (e

V)  

Time  

Page 28: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Hybrid  simula0ons  (upstream)  

Page 29: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Hybrid  simula0ons  (wake)  

Page 30: P.#A.#Delamere# University#of#Colorado#con/ioworkshop2012/Program... · 2012. 7. 13. · Issuesfor%plasmainterac0ons • Energy’inputfor’neutral’ escape’(formaon’of’corona

Io’s  electrodynamic  interac0on  with  Jupiter’s  magnetosphere  

•  Complex!  –  Induced  Dipole  – Thermal  plasma  -­‐>  neutral  atmosphere  

•  Ioniza4on  and  Charge  Exchange,  auroral  emissions?  – Electron  beams  from  Alfvenic  interac4on  

•  Ioniza4on,  auroral  emissions?  – Escaping  neutrals  

•  Charge  exchange,  electron  impact  dissocia4on  – Plasma  data  analysis  difficult  due  to  non-­‐Maxwellian  distribu4ons!