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TRANSCRIPT
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Dusty Plasmas in the
Laboratory and Space
Bob Merlino
April 2003 APS Meeting Philadelphia, PA
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Outline
1) Introductionwhat is a dusty plasma and
where are they found
2) the charging of dust in a plasma
3) devices for producing dusty plasmas
4) waves in dusty plasmas
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plasma = electrons + ions Plasma
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What is a dusty
plasma?
D
Debye
shielding
small particle
of solid matter
becomes
negativelycharged
absorbselectrons and
ions
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Dusty Plasma in the Universe
Dust represents much of the
solid matter in the universeand this component oftencoexists with the ionized
matter forming a dustyplasma.
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Importance of Charged Dust
the dust acquires an electrical charge and
thus is subject to electromagnetic as well as
gravitational forces
the charged dust particles participate in the
collective plasma processes
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DUSTY PLASMAS
Solar nebula
planetary rings
interstellar medium
comet tails
noctilucent clouds
lightning
Microelectronic
processing
rocket exhaust
fusion devices
Natural Man-made
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Our solar systemaccumulated out
of a dense cloud of
gas and dust, formingeverything that is now
part of our world.
Rosette Nebula
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Noctilucent Clouds (NLC)
Occur in the summer polar mesosphere (~ 82 km)
50 nm ice crystals
Associated with unusual radar echoes and reductions
in the local ionospheric density
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An early temperature measurement in a dusty plasma.
A flame is a very weakly ionized plasma
that contains soot particles.
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Comet Hale-Bopp
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Spokes in Saturns B Ring
Voyager 2
Nov. 1980
Cassini-
HuygensJuly 2004
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Semiconductor Processing System
dust
silane (SiH4) + Ar + O2 SiO2 particles
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Semiconductor Manufacturing
dustSi
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Physics Today
August 1994
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Dust Charging Processes
electron and ion collection
secondary emission
UV induced photoelectron
emission
Total current to a grain = 0
I = Ie + Ii + Isec + Ipe = 0
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electron
repulsion
ion enhancement
The Charge on a Dust Grain
In typical lab plasmas Isec = Ipe = 0
Electron thermal speed >> ion thermal speed so the grains
charge to a negative potential VS relative to the plasma, until
the condition Ie = Ii is achieved.
a
2
2
1
exp
akT
eV
m
kTenI
a
kT
eV
m
kTenI
i
S
i
iii
e
S
e
eee
Q = (4eoa) VS
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Typical Lab Plasma
For T e = Ti = T in a hydrogen plasma
VS = 2.5 (kT/e)
If T 1 eV and a = 1 m,
Q 2000 e
Mass m 5 1012 mp
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Dust Charge Measurements
0
0.5
1
1.5
2
0 20 40 60 80 100 120
Diameter (micron)2
0
0.5
1
1.5
0 20 40 60 80 100 120 140 160
Electron Energy (eV)
Glass
Graphite
Walch, Horanyi, & Robertson,
Phys. Rev. Lett. 75, 838 (1995)
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Devices for producing
dusty plasmas
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RF Dusty Plasma Devices
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PUMP
ANODEDISK
FIREROD
ROTATING DUSTDISPENSER
PLASMA COLUMN
HOT PLATE
B
VIDEOCAMERA
CONFINEDDUST GRAINS
GAS IN
GAS IN
Equipotential profiles
of an anode doublelayer
anode
Device for studying
the trapping of dust
in a dc glowdischarge
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DUST IN A GLOW DISCHARGE
N2
Vacuum
vessel
PS
+
BAnode
Dust Tray
Anode Glow
Plasma
Dust: kaolin (aluminum silicate)
E
mg
QE
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wavefronts
Dust Acoustic Wave Image
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dust mass
DA Dispersion relation
Monochromatic plane wave solutions
for Te = Ti = T
1
1d
dDA Z
m
kTCf
where = ndo/n+o
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Dust Acoustic Wave
Dispersion Relation
theory
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Shocks in Dusty Plasma
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Shocks in Dusty Plasma- results
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Shocks in dusty plasmas
Conclusions Ion acoustic compress-
ional pulses are observed
to steepen as they travelthrough a dusty plasma
Relevant to astrophysical
contexts where density
disturbances travel
through dust clouds
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Conclusions and Outlook
Only recently have we begun to explore thebehavior of dusty plasmas in the laboratory
-charging mechanisms, waves
Technological applications of dusty plasmas arenow being exploited
-ceramic deposition composites
-growth of nanosize particles-diamond growth and deposition on metals
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Dusty plasmas in space are usually embedded
in magnetic fields. This aspect of dustyplasmas has yet to be studied in the lab
R = Mv/QB >> typical lab plasmas
Dusty plasmas may form strongly coupled
systems known as Coulomb Crystalsa new
area for plasma physics research
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Dusty Plasma
DUST
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RF Dusty Plasma Device