8. electric propulsion an overview - purdue engineering...aae 439 ch8 –2 overview at the beginning...
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AAE 439
Ch8 –1
8. Electric Propulsion An Overview
AAE 439
Ch8 –2
OVERVIEW
At the beginning of last century, Goddard experimented with electric gas discharge tubes recognizing basic concepts for Electric Propulsion.
“Wege zur Raumschiffahrt” by Hermann Oberth, 1929. Since the 1950’s, Electric Propulsion has a well established
research history in government, academia, and industry (US, Soviet Union, Europe, Japan).
Since the mid 1980’s, the propulsion community has seen a boom in Electric Propulsion research.
Since the early 1990’s: all major US communications satellite manufactures (such as
Hughes, SS/LORAL, Lockheed-Martin) have embraced Electric Propulsion.
Earth and Space Science Missions are increasingly baselined with Electric Propulsion (DS-1, EO-1, ST, CNSR, Mars Sample Return, etc.)
AAE 439
Ch8 –3
OVERVIEW
EP Statistics: EP Capability:
East/West and North/South Station Keeping Orbit Transfer Orbit Insertion
US Industry (GEO/LEO): 142 Hydrazine Arcjets ordered or in orbit Over 100 Hydrazine Resistojets in orbit 10 Xenon Ion Thrusters in orbit
Russia: Over 100 Hall Thrusters in orbit
European and Japanese satellite manufacturers increasingly baseline EP into spacecraft design.
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Ch8 –4
Flight History of EP Systems
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Ch8 –5
CHARACTERISTICS
Chemical Propulsion
Payload Propellant Power Thrust
Exhaust (Momentum Flux)
Thruster Powerplant
Payload Propellant Thrust
Exhaust (Momentum Flux)
Engine
Energy Limited Chemical bonding energy Limiting energy release Restricting specific impulse
Low payload fraction Strong but short burns High thrusts and propellant
mass flows Moderate exit velocities Limited final velocity
Electric Propulsion Power Limited
Energy conversion rate Material restrictions
Separate power source Higher energy content supplied
to propellant High specific impulse
High exit velocities Low propellant consumption
Low thrusts and acceleration High final velocities Short travel times
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ELECTRIC PROPULSION BENEFITS
High Fuel Efficiency Enables Missions (High Isp) EP provides 2 to 10 times payload increases compared to
chemical EP reduces trip time up to 3 times for many missions
0 0.1 0.2 0.3 0.4 0.5 0.6
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Chemical Propulsion Electric Propulsion
Courtesy of NASA GRC
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Ch8 –7
FUNDAMENTALS
Definition: Electric propulsion is accomplished by the acceleration of gases by electrical and/or electric and magnetic forces acting on a conducting plasma made up of the propellant gas constituents.
Electrical Energy Used to increase Potential Energy
Potential Energy Converted to Kinetic Energy by Various Methods
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Ch8 –8
CLASSIFICATION
E L E C T R I C S P A C E P R O P U L S I O N
Electrostatic Systems Electromagnetic Systems Electrothermal Systems
Arcjets
Resistojet Thrusters
Microwave-Plasma Thrusters
Radio-Frequency Ion Thruster
Ion Thruster
MagnetoPlasmaDynamic Thrusters
RF Plasma Thrusters
Hall Thruster
Pulsed Inductive Thrusters
VaSIMR
Pulsed Plasma Thrusters
Field Emission Ion Thruster
Contact Ionization Thruster
Kaufman Thruster
Thruster with Anode Layer
Stationary Plasma Thruster
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Ch8 –9
FUNDAMENTALS
Thrust: T = mUex
Specific Impulse: Isp = Thrust/Propellant Flow Rate = Uex/g0
Efficiency: = Exhaust Power/Input Power = mUex/2Pin
•
• 2
• •
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Ch8 –10
FUNDAMENTALS
Thrust/Power Ratio as Function of Spec. Impulse Th
rust
/Pow
er [N
/kW
]
Specific Impulse [s]
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Ch8 –11
EP/POWER SOURCES FOR SPACE MISSIONS M
issi
on E
nerg
y
Ion Hall MPD, PIT, VASIMR
Piloted
Outer Planets Inner System Sample Returns
Inner Planets,Comets, Asteroids
Earth Orbit
Solar
Nuclear Nuclear
Isotope Solar with AeroCap & Chem
Solar
Solar at Earth with Aerocapture & Chemical at Target
Nuclear
Isotope
ION HALL MPD, PIT, VaSIMR
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Ch8 –12
GENERAL SPACECRAFT LAYOUT
Based on Nuclear Power and Electric Propulsion
Spacecraft Bus
Electric Propulsion System
ElectricThruster
PropellantFeed
System
PowerProcessingUnit (PPU)
PropellantTank
Spacecraft SubsystemsC&DH RCSGN&C TCSRF SW
Science Payload
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Ch8 –13
HIGH POWER EP CANDIDATES
Variable Specific Impulse Magnetoplasma Rocket (VaSIMR)
Hall-Ion Thruster
Pulsed Inductive Thruster (PIT)
200 kWe MAI Li- LFA (MPD)
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Ch8 –14
ELECTRO-THERMAL SYSTEMS
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Ch8 –15
ELECTROTHERMAL SYSTEMS
Resistojet Thruster Principle of Operation:
simplest of all EP devices material limitations electric power employed to
resistor energy transfer to propellant hot propellant expanded in
nozzle
Performance Characteristics: Specific Impulse: 200-300 s Thrust: 2-350 mN Efficiency: 65-90 % Power: 10-5000 W Typical Propellant:
Hydrogen Hydrazine
Propellant
Resistors
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EXAMPLES
Concentric Tubular Resistojet: Input Power: 3.0 kW Thrust: 0.176 N Spec. Impulse: 840 s Efficiency: 88% Propellant: H2
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ELECTROTHERMAL SYSTEMS
Arcjet Thruster Principle of Operation:
arc discharge between anode + cathode
direct propellant heating by arc
two heating regions hot propellant expanded in
nozzle sophisticated PPU and PPC
Performance Characteristics: Power: 500-5000 W Thrust: 2-700 mN Specific Impulse: 400-1500 s Efficiency: 40-50 % Typical Propellant:
Hydrogen Hydrazine
Cathode
Propellant
Anode
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EXAMPLES
Regeneratively Cooled Arcjet: Power Input: 30 kW Thrust: 3.35 N Spec. Impulse: 1,010 s Efficiency: 54% Propellant: H2
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EXAMPLES
2-kW Arcjet: Input Power: 2.2 kW Spec. Impulse: 600 s Efficiency: 30%-42% Propellant: Hydrazine
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Ch8 –20
ELECTROTHERMAL SYSTEMS
LA
DA
a q
G
Cathode
Anode/Nozzle
Typical dimensions: LA = 0.25 mm; DA = 0.6 mm; G = 0.6 mm
= 30°; = 20°
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Ch8 –21
ELECTROTHERMAL SYSTEMS
Microwave Plasma Thruster Principle of Operation
microwaves generated in cavity
electromagnetic coupling induces plasma discharge
energy transfer to propellant hot propellant expanded in
nozzle
Performance Characteristics Power: 100-600 W Thrust: 2-20 mN Specific Impulse: 200-400 s Efficiency: 30-60 % Typical Propellant:
Inert Gases Nitrogen Hydrogen
Propellant
ResonantCavity
Microwave-PlasmaDischarge
CoaxialMicrowaveInput
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Ch8 –22
Co-Axial RF Plasma Thruster
Power: RF plasmas are sustained over a very wide power and voltage range. Direct-drive schemes are feasible without the need of exotic voltage
requirements. Target operating conditions: 1-100 W (< 1W) at frequencies of 1-1000
MHz, which is tailored to main bus operating voltages of most microspacecraft (< 10 V).
Mass/Volume: RF components and power sources/processing have seen tremendous
technological advancements in recent years especially with regard to size and efficiency and a significant reduction in mass and volume.
The co-axial geometry of this propulsion device lends itself to further miniaturization.
Lifetime: Preliminary experiments have shown that electrodes are not subject to
erosion and sputtering in RF plasmas at certain conditions (frequency, electrode separation, gas pressure).
A micropropulsion system based on this concept could provide lifetimes currently not exhibited by technologies considered for microspacecraft applications.
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Ch8 –23
Co-Axial RF Plasma Thruster
Attributes: Low power operation suitable for power limited spacecraft (micro/
nano satellite). RF operation eliminates erosion enabling very long lifetimes. Suitable for miniaturization leading to Thruster-on-a-Chip.
Co-axial design philosophy: Integration Issues arising from miniaturization:
Propellant feed, Power feed, Diagnostics.
Operating Principle: Characterized by low-power, RF glow discharge operation. RF power ionizes neutral gas and sustains the plasma. Plasma heats gas and enthalpy of gas increases. Thrust is generated by thermodynamic expansion of gas through nozzle.
Thruster Body Outer Electrode
Inner Electrode
N-Type Connector
Dielectric Separator
Propellant Feed Port
Dielectric Separator
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Ch8 –24
Co-Axial RF Plasma Thruster
Proof of concept experiments accomplished: Plasma operation at < 50 W, Gas temperature depends on frequency and gap distance, No erosion observed when compared to DC mode operation at same operating conditions.
Two different size prototypes exist: RF25-1 RF50-1 Device maintains 50 Ω impedance, Inner Electrode diameter: ¼” ½”
Mass: 113 g 229 g Volume: 55 cm3 85 cm3
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ELECTRO-STATIC SYSTEMS
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Ch8 –26
ION THRUSTER BASICS
Four basic and separable processes occur in an ion thruster:
1.
1. Energetic Electron Production,
2.
2. Ion Production,
3.
3. Ion Extraction and Acceleration,
4.
4. Ion Beam Neutralization.
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Ch8 –27
ELECTROSTATIC SYSTEMS
Ion Thruster Principle of Operation
ion acceleration in electrostatic field
ion neutralization at exit plane thrust generation: momentum
change due to electric body forces
Performance Characteristics Power: 0.5-5 kW (30 kW) Thrust: 1-200 mN Specific Impulse: 1500-5,000 s (15,000s) Efficiency: 40-80 % Typical Propellant:
Inert Gases (Xenon, Krypton) Mercury
Ionization Mechanisms: Bombardment Field Emission, Radio Frequency, Contact
Ionization
Research Initiatives: High-voltage extraction grids Cathodes Wear mechanisms
Participants: NASA GRC/JPL Academia Industry
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OPERATION SCHEMATIC
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Ch8 –29
HOLLOW CATHODE
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Ch8 –30
ION OPTICS
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EXAMPLES
NSTAR 30-cm Ion Thruster: Power Input: 0.5-2.3 kW Thrust: 21-92 mN Spec. Impulse: 2000-3200 s Efficiency: 42%-62% Propellant: Xenon
DEEP SPACE 1: First use of Ion Thruster for Primary Propulsion
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ION THRUSTER
15-cm Ion Engine Slotted, Carbon-Carbon Grids Power Input: 1.25 kW Efficiency: 60% (± 5%) Specific Impulse: 2,500-4,000 s Thrust: 20-30 mN
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SAFE-30 POWER TRAIN
Thermal Energy Kinetic Energy
Qth
Power Conversion
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HALL SYSTEMS
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Ch8 –35
HALL THRUSTER SYSTEMS
Stationary Plasma Thruster (SPT) Thruster with Anode Layer (TAL)
Performance Characteristics Power: 0.5 - 3 kW (50 kW) Thrust: 20-150 mN Specific Impulse: 500-2500 s (4000 s) Efficiency: 40-60 % Typical Propellant:
Xenon Argon
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EXAMPLES
TAL/D-55: Power Input: 1.5 kW Thrust: 38-128 mN Spec. Impulse: 700-1800 s Efficiency: 24%-53% Propellant: Xenon
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EXAMPLES
SPT-100: Input Power: 1.35 kW Thrust: 40-97 mN Spec. Impulse: 1070-1600 s Efficiency: 34%-50% Propellant: Xenon Extensive Flight History (Russia)
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HALL DEVELOPMENT PATH
One kilowatt level systems flight proven (TRL 9) Over 100 thrusters flown on Russian satellites System flown on DOD experimental S/C (STEX)
Five-kilowatt level system flight qualified (TRL 8) NASA/BMDO Express T-160 flight program Air Force/Loral SPT140 qualification program
Ten-kilowatt system prototype demo (TRL 6) 1000 hr test of NASA/ Pratt & Whitney T-220
Fifty-kilowatt breadboard validation (TRL 4) NASA-457M in-house program Russian TM-50 pathfinder experiments
Courtesy of NASA GRC
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ELECTRO-MAGNETIC SYSTEMS
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Ch8 –40
ELECTROMAGNETIC SYSTEMS
Magnetoplasma Dynamic Thruster (MPD) Principle of Operation
arc discharge between anode + cathode self-induced magnetic field thrust generated by interaction of current and magnetic field thermal thrust generation
Performance Characteristics Power: 1-200 kW Thrust: 1-2,000 mN Specific Impulse: 400-8,000 s Efficiency: 30-50 % Typical Propellant:
Inert Gases Cs, Li, Bi, N2
Thruster Types: Self-Induced Magnetic Field External Magnetic Field
Participants: NASA JPL/GRC Princeton
jj j x B
B
ANODE
CACATHODETHODEPLASMANEUTRAL GAS
INJECTION HOLES
INSULATOR BACKPLATE
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Ch8 –41
DEVELOPMENT PATH TO MWE PLASMA THRUSTERS
• Anode Texturing • Heat Pipes
• Lithium Propellant • Active Turbulence Suppression
• Plume Shields • Booms
h = 50% Isp = 4,000 s
200 kWe Steady State
100’s of Hrs at 3,000 A
1 - 5 MWe Steady State
h = 60% Isp ≤ 8000 s
10,000 Hrs at 20,000 A
• Multi-Channel Hollow Cathodes • Barium Addition
0.001
0.01
0.1
1
10
100
1000
Cur
rent
Den
sity
(A
/cm
2 )
4000350030002500200015001000Temperature (K)
PBa = 100 Pa
10 Pa
1 Pa
Pure W (110) Pure Ba Ba-W (110)
4
3
2
1
0
-1
Thru
st Co
effic
ient,
C T
25x103 20151050 Current, J (A)
BP (p)BP (b)
AIF (p)AIF (b)
CT (p)
AOF (b)
Total
200 kWe Lithium-fed Thruster
Ships of Space
10-8 g/cm2s at 0.3 m
10-10 g/cm2s at 30 m
Courtesy of NASA JPL
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Ch8 –42
ELECTROMAGNETIC SYSTEMS
Pulsed Plasma Thruster Principle of Operation
spark plug + capacitor discharge
main discharge ablates + ionizes Teflon
self-induced magnetic field Lorentz force
Performance Characteristics Power: 10-200 W Thrust: 0.05-10 mN Specific Impulse: 200-2000 s Efficiency: 5-30 % Typical Propellant:
Teflon Carbon based Polymers
Anode
Cathode
j
d
B
h
V(t) j x B
Insulator
SwitchI(t)
Q(t)
Capacitor
AAE 439
Ch8 –43
EXAMPLES
58-J Pulsed Plasma Thruster (PPT): Power Input: 5-50 W Thrust: 100-750 N Spec. Impulse: 1200 s Efficiency: 10%
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Ch8 –44
PULSED INDUCTIVE THRUSTER
Operating Principle Characterized by µ-second, MW-power pulsed operation. Nozzle injects propellant covering coil surface, while pulse forming
network triggers discharge of cap bank. Transient high current in coil generates rapidly changing magnetic
field. Magnetic field induces strong azimuthal electric field which breaks down propellant. Cross-product interaction of plasma current and magnetic field in coil accelerates plasma to generate thrust.
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PULSED INDUCTIVE THRUSTER
Performance Characteristics: Propellant: Argon, Hydrazine, Ammonia, Carbon Dioxide Specific Impulse: 2,000 - 8,000 s Efficiency: 20 - 50 % Operation Mode: Single Shot Discharge Voltage: 20 - 30 kV Bank Capacitance: 9 µF
Impulse as a Function of Propellant Mass Efficiency as a Function of Specific Impulse
Ammonia, 16 kV
0
0.05
0.1
0.15
0.2
0 1 2 3 4 5 6 7 8
Impu
lse
[N-s
]
Mass [mg]
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Ch8 –46
PULSED INDUCTIVE THRUSTER
Electric Characteristics: Single Circuit Parameters:
Nine circuits in parallel Initial Rise Time: dI/dt = 30 kA/µs Peak Current: 15 kA Capacitance: 2 µF Charge Voltage: 15 - 20 kV
Current Waveform for one Circuit
-10
-5
0
5
10
15
20
0 2 4 6 8 10 12 14
Cur
rent
[kA
]
Time [µs]
(dI/dt)initial≈ 30 kA/µs
Ipeak≈ 15 kA
Imin≈ 50% I
peak
Technical Challenges: Switch Technology
High repetition rate and extreme long lifetime
High peak currents High and rapid initial current rise
High Power Capacitors Extreme long lifetime Requires space qualification under
extreme operating conditions
Powertrain Architecture Recovery of reflected energy Pulse shape control for optimum
pulse waveform
Participants: NASA MSFC/GRC TRW
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Ch8 –47
VaSIMR
Operating Principle: Propellant gas is ionized at helicon plasma frequency Ionized gas enters central chamber and undergoes ion-cyclotron
resonance heating Hot, ionized plasma is expelled through contoured magnetic nozzle
to provide thrust
gas injection quartz tube
helicon antenna
magnets
ICRH antenna
exhaust region
VX-10 Lab Experiment
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Ch8 –48
VaSIMR DEVELOPMENT PATH
Performance Characteristics: VaSIMR concept scales well with high power Proposed Flight Experiment (VF-10)
Power: 10 kW Specific Impulse: 10,000 s Thrust: 100 mN Propellant: H2, D2
Research Activities: Helicon Development ICRH Development
Participants: NASA JSC/MSFC Academia DOE (LANL, ORNL)
( 1 0 k W
2 0 0 k W
1 0 0 M W
G R O U N D T E S T I N G l e a d s s p a c e t e s t i n g )
3 0 M W M a r s H u m a n
m i s s i o n 2 0 1 6 c a r g o 2 0 1 8 c r e w
3 0 M W M a r s N u c l e a r P a t h f i n d e r
O p e r a t i o n a l 1 M W
d e e p s p a c e n u c l e a r
1 0 0 k W d e m o
R T D M i s s i o n
P o w e r
' 9 6 ' 9 7 ' 9 8 ' 9 9 ' 0 0 ' 0 1 ' 0 3 ' 0 3 ' 0 4 ' 0 5 ' 0 6 ' 0 7 ' 0 8 ' 0 9 ' 1 0 ' 1 1 ' 1 2 ' 1 3 ' 1 4 ' 1 5 ' 1 6 ' 1 7 ' 1 8 ' 1 9 ' 2 0
N u c l e a r
Y e a r
N u c l e a r P o w e r D e v
S o l a r P o w e r D e v S o l a r
S p a c e e x p
2 k W
1 0 M W
1 . 5 M W
3 0 M W
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SUMMARY
Electric Propulsion Capability: Pulsed Microthrusters:
Precision Control Formation Flying
kW-Class Systems: NS/EW-Station Keeping S/C Insertion Maintenance and Deorbit Robotic Planetary
ENABLING ADVANCED EXPLORATION OF SPACE! Exploration to expand understanding of space. Commercial development and utilization of extraterrestrial
resources. Provide potential human and robotic exploration.
5-10 kW-Class Systems: GEO Insertions Large Platform Deorbit Earth and Space Science Missions
500+ kW-Class Systems: Human/Robotic Exploration Development of Space
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CONCLUSIVE REMARKS
Performance is mission enabling Increase in payload fraction, Decrease in launch vehicle size (step down), Reduction in trip time.
Mission benefits arise from electric propulsion technology ION - Auxiliary/Primary propulsion for planetary/deep space
missions, HALL - Auxiliary/Primary propulsion for orbital missions ELECTROMAGNETIC - Primary propulsion for planetary/deep space
missions. In many aspects Electric Propulsion is superior over chemical
propulsion for space applications. New developments in materials, electronics, energy storage and
power processing technology will further advance Electric Propulsion.
Disclaimer: Some pictures are courtesy of colleagues from industry and government.