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NIAC 7th Annual Meeting 
Tucson, Arizona 
October 18th, 2006 
An Architecture of Modular Spacecraft 
with Integrated Structural 
Electrodynamic Propulsion (ISEP) 
Nestor Voronka, Robert Hoyt, 
Brian Gilchrist, Keith Fuhrhop 
TETHERS UNLIMITED, INC. 
11711 N. Creek Pkwy S., Suite D-113 
Bothell, WA 98011 
(425) 486-0100 Fax: (425) 482-9670 voronka@tethers.com
Motivation 
–– Traditional propulsion uses propellant as reaction mass 
–– Advantages (of reaction mass propulsion) 
•• Can move spacecraft center of mass, on-demand, and 
relatively quickly 
•• Multiple thrusters offer independent and complete control of 
spacecraft (6DOF) 
–– Disadvantages 
•• Propellant is a finite and mission limiting resource 
•• Propellant mass requirements increases exponentially with 
mission ΔΔV requirements 
•• Propellant may be a source of contamination for optics and 
solar panels 
–– Current Architectures of NASA’’s Vision of Exploration 
require launching and transporting large masses 
–– Are there innovative alternatives?
Space Propulsion Landscape 
10,000 sec 
2,000 sec 
Isp 
Courtesy Gallimore, A., UMich
Electrodynamic Space Tether Propulsion 
–– In-space propulsion system 
–– PROS: 
•• Converts electrical energy into 
thrust/orbital energy 
•• Little or no consumables are required 
–– CONS: 
•• Long (1-100km) flexible structures 
exhibit complex dynamics, especially in 
higher current/thrust cases 
•• Gravity gradient tethers have constrained 
thrust vector 
•• Relies on ambient plasma to close 
current loop Given a fixed amount of power available 
and fixed conductor mass, thrust 
efficiency is independent of the length 
of the conductor
Proposed Solution 
–– Multifunctional propulsion-and-structure 
system that utilizes Lorentz forces (F = 
iL x B) generated by current carrying 
booms to generate thrust with little or 
no propellant expenditure 
•• Utilizes same principles as electrodynamic 
tether propulsion 
–– Utilize relatively short (≈≈100 meter), 
rigid booms with integrated conductors 
capable of carrying large currents, that 
have plasma contactors at the ends 
•• Space Tether Electrodynamic Propulsion 
–– Ex: 10km conductor, 1Ampere in LEO 
•• Thrust |iLxB| ≈≈ 0.3 Newtons 
–– Proposed Integrated Structural 
Propulsion 
•• Ex: 100m conductor, 100 Ampere (!) in 
LEO 
–– Thrust |iLxB| ≈≈ 0.3 Newtons 
–– Torque ≈≈ 750 N· m
Single Boom Concept of Operation 
– Apply potential to overcome motion-induced electric field and drive 
current across magnetic field 
– Current flowing down boom produces thrust force 
– Plasma waves close the electrical circuit
‘‘Structural’’ ED Propulsion 
–– By connecting six booms to a spacecraft along 
orthogonal axes, 4DOF of motion can be 
controlled (translational and rotational)
ISEP Booms 
–– Cold biased, low-resistance 
element to maximize propulsive 
performance 
•• Copper Clad Aluminum (CCA) 
offers low specific resistivity, yes 
remains easy to work with 
–– Ex. 0.01ΩΩ/50 meter boom has a 0.44 
kg/m density 
–– Stiffness dictated by application 
–– Boom ends contain plasma 
contactors & docking sensors 
–– Hemaphroditic high-current 
capacity docking mechanism
100 Ampere Contactors for ISEP 
Emission Device Power Notes 
TC + Electron Gun 2.1 MW 18 emitters, < 1.25 V for SCL 
Electron FEA 5860 W 10 emitters, < 0.4 V for SCL 
Emission 
HC 1250 W to 10 kW Flow Rates & Ion Type 
9 sccm to 40 sccm Xe 
Passive Sphere a 4.7 MW 1 m radius, 6.6E-3 N Drag 
90% Porous – 6.6E-4 N 
Passive Sphere b 1 MW 2.29 m radius, 3.46E-2 N Drag 
90% Porous – 3.46E-3 N 
Passive Plate a 61.3 MW 5 m2 – 5.26E-5 N Drag 
Passive Plate b 1 MW 54.52 m2 – 5.73E-4 N Drag 
Electron 
Collection 
HC 6150 W + 330 W 
(20 A ion prod.) 
280 sccm fuel 
27.35 mg/s Xe+ or 0.21 mg/s H+ 
Ion Emission + Ion 
Gun 
1 MW + 1650 W 
(100 A ion prod.) 83,334 emitters needed 
Ion 
Emission 
HC 1000 W + 1650 W 
(100 A ion prod.) 
1400 sccm fuel 
27.35 mg/s Xe+ or 0.21mg/s H+
ISEP Nodes 
–– Node geometry 
•• Simplest has 6 orthogonal 
mating surfaces 
•• Can also utilize polyhedrons 
with mating surfaces spaced 
45° along the circumference 
–– Node components 
•• Energy storage (flywheels @ 
75 W-hr/kg) 
•• System & Navigation 
Controllers
Modular Spacecraft 
–– By making booms and spacecraft modules 
modular and interconnectable, we create self-assembling 
Tinkertoy® like components for 
space structures and systems
ISEP Applications 
–– Self-Assembling Modular Spacecraft (SAMS) 
–– Self-Assembling Structure for Refueling Station 
•• Integral rail gun for commodity delivery 
–– Self-Assembling Space Tug 
–– Self-Assembling Structure for Large Mirror 
or Antenna Arrays 
–– Formation Flying Space Systems 
•• Terrestrial Planet Finder (TPF)
40000 
35000 
30000 
25000 
20000 
15000 
10000 
5000 
0 
200.0 400.0 600.0 800.0 1000.0 1200.0 
Circular Orbit Altitude (km) 
Delta-V (m/se 
Inclination = 0.0º 
Inclination = 28.5º 
Inclination = 51.6º 
Inclination = 90.0º 
Inclination = 97.0º 
ISEP Performance Analysis 
–– Six 50m orthogonal booms in 300-1100km, 0-97° 
inclination orbits 
–– FEAs for electron emission, HCs for ion emission 
–– Total system mass –– 1000kg with 20kg H consumable 
(approx 3 years full time operation) 
–– Current commanded to 100A continuous for 30 days 
•• System Input power - 6500 Watts 
–– Performance metrics tabulated & averaged 
40000 
35000 
30000 
25000 
20000 
15000 
10000 
5000 
0 
200.0 400.0 600.0 800.0 1000.0 1200.0 
Circular Orbit Altitude (km) 
Delta-V (m/se 
Inclination = 0.0º 
Inclination = 28.5º 
Inclination = 51.6º 
Inclination = 90.0º 
Inclination = 97.0º 
40000 
35000 
30000 
25000 
20000 
15000 
10000 
5000 
0 
200.0 400.0 600.0 800.0 1000.0 1200.0 
Circular Orbit Altitude (km) 
Delta-V (m/se 
Inclination = 0.0º 
Inclination = 28.5º 
Inclination = 51.6º 
Inclination = 90.0º 
Inclination = 97 0º 
Along-track Total ΔV Cross-track Total ΔV Radial TotalΔV
ISEP Performance (cont.) 
–– Thrust magnitude and efficiency 
highly dependent on alignment 
of boom(s) with magnetic field 
–– Torques in the 1-10 N-m range 
as compared to disturbances in 
the 10-8 to 10-1 range 
0.45 
0.4 
0.35 
0.3 
0.25 
0.2 
0.15 
0.1 
0.05 
0 
200.0 400.0 600.0 800.0 1000.0 1200.0 
Circular Orbit Altitude (km) 
Thrust st ( 
Inclination = 0.0º 
Inclination = 28.5º 
Inclination = 51.6º 
Inclination = 90.0º 
Inclination = 97.0º 
Average Along-track Thrust (N) 
200000 
180000 
160000 
140000 
120000 
100000 
80000 
60000 
40000 
20000 
0 
200.0 400.0 600.0 800.0 1000.0 1200.0 
Circular Orbit Altitude (km) 
Specific Impulse (se 
Inclination = 0.0º 
Inclination = 28.5º 
Inclination = 51.6º 
Inclination = 90.0º 
Inclination = 97.0º 
10 
9 
8 
7 
6 
5 
4 
3 
2 
1 
0 
Inclination = 0.0º 
Inclination = 28.5º 
Inclination = 51.6º 
Inclination = 90.0º 
Inclination = 97.0º 
200 400 600 800 1000 1200 
Along-track current torque (N-m) 
200000 
180000 
160000 
140000 
120000 
100000 
80000 
60000 
40000 
20000 
0 
Circular Orbit Altitude (km) 
Inclination = 0.0º 
Inclination = 28.5º 
Inclination = 51.6º 
Inclination = 90.0º 
Inclination = 97.0º 
0 5 10 15 20 25 30 35 
Thrust to Power Ratio (μN/W) 
ISEP boom Torque (N 
Specific Impulse (s 
Average Specific Impulse (Isp) Isp vs. Thrust to Power (uN/w)
ISEP Performance 
–– ISEP is competitive with other EP technologies 
–– In systems where collinear booms are assembled, performance 
improves 
–– For missions where structural elements are required, ISEP’’s dual use 
(propulsive/structural) has significant advantages 
1000000 
100000 
10000 
1000 
100 
10 
1 
Resistojet 
Arcjet 
Pulsed Plasma Thruster 
Hall Effect Thruster 
Ion Thruster 
Integrated Structural EP 
0.001 0.01 0.1 1 
Thrust-to Power (N/kW) 
Specific Impulse (se 
–– KEY TECHNOLOGY CHALLENGE: Power- and Mass- Efficient 
collection and emission of electrons from/to the ambient plasma
Technology Demonstration Experiment 
–– Primary Experiment Objectives 
•• Generate directly detectable torque 
•• Generate directly measurable thrust 
–– Secondary Experiment Objectives 
•• Validate performance of Field Emissive 
Electron device(s) 
•• Validate performance of lightweight 
electron collectors 
–– GOAL: Drive 1 Ampere of current 
through lightweight deployable, 
conductive 10-20 meter booms 
•• 0.2-1.0 second impulses > 0.5 mN
Experimental Method 
–– Picosatellite launched as a secondary 
payload 
–– Target platform –– CubeSat 
•• 1kg –– 10x10x10 cm envelope 
•• Standard initially designed for University class 
experiments and educational purposes 
•• Typically 1-2 launch opportunities a year 
•• Launch costs $40-120K for a 1U CubeSat 
•• Ideal for simple experiments and 
technology demonstrations
Picosat Experiment Contactors 
–– Field Emissive Cathodes 
•• Microfabricated Emitter tips rely on sharp emitter 
tips, and close non-intercepting electrodes to 
generate high field required to enable electrons to 
quantum tunnel out of the material into space 
•• High current densities (5000A/cm2) have been 
demonstrated 
•• Development undergoing to increase total current 
output and reduce environmental constraints 
–– Passive Electron Collector (‘‘Hedgehog’’) 
•• Bundle of conductive yarns 
•• Yarns tied together at root, and when charged will 
form approximately a ‘‘Koosh-ball’’ like spherical 
structure due to electrostatic repulsive forces 
•• 2 meter diameter structure with yarns every 40°, 
and filament every 1° can weigh 10 grams(!)
Experiment Conops 
–– Converted Solar Energy is stored onboard in capacitor bank 
•• Allow for thrust pulse every 4-6 orbits 
–– At desired B-field alignment, discharge capacitor to generate 1Ampere pulse 
–– Measure Thrust with onboard accelerometers 
–– Measure Torque with body attitude rate change
Summary 
–– Proposed Concept IS feasible 
•• Requires small amount of consumables for ion source 
•• 4DOF propulsion–– no thrust in B-field direction 
•• Competitive with tradition Electric Propulsion with added benefit of structural 
elements 
–– Technology Challenges 
•• High Current Plasma Contactors 
–– Devices exist –– robust units with higher efficiencies needed 
•• Plasma Contactor Space Charge Limiting 
–– High current densities may be environmentally limited 
•• Collision proof coordinated control laws for formation flight, and self-assembly 
–– Additional constraints imposed on low-thrust control laws 
–– Experiment in Phase II will demonstrate system feasibility and validate 
component technologies 
–– Potential Applications 
•• Space Tug and Commodity Depot (with integral rail gun?) 
•• Structure for Beamed Power Solar Array/Antenna Fields 
•• Structure for Space Habitats with Integral Drag Makeup

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1386 voronka[1]

  • 1. NIAC 7th Annual Meeting Tucson, Arizona October 18th, 2006 An Architecture of Modular Spacecraft with Integrated Structural Electrodynamic Propulsion (ISEP) Nestor Voronka, Robert Hoyt, Brian Gilchrist, Keith Fuhrhop TETHERS UNLIMITED, INC. 11711 N. Creek Pkwy S., Suite D-113 Bothell, WA 98011 (425) 486-0100 Fax: (425) 482-9670 voronka@tethers.com
  • 2. Motivation –– Traditional propulsion uses propellant as reaction mass –– Advantages (of reaction mass propulsion) •• Can move spacecraft center of mass, on-demand, and relatively quickly •• Multiple thrusters offer independent and complete control of spacecraft (6DOF) –– Disadvantages •• Propellant is a finite and mission limiting resource •• Propellant mass requirements increases exponentially with mission ΔΔV requirements •• Propellant may be a source of contamination for optics and solar panels –– Current Architectures of NASA’’s Vision of Exploration require launching and transporting large masses –– Are there innovative alternatives?
  • 3. Space Propulsion Landscape 10,000 sec 2,000 sec Isp Courtesy Gallimore, A., UMich
  • 4. Electrodynamic Space Tether Propulsion –– In-space propulsion system –– PROS: •• Converts electrical energy into thrust/orbital energy •• Little or no consumables are required –– CONS: •• Long (1-100km) flexible structures exhibit complex dynamics, especially in higher current/thrust cases •• Gravity gradient tethers have constrained thrust vector •• Relies on ambient plasma to close current loop Given a fixed amount of power available and fixed conductor mass, thrust efficiency is independent of the length of the conductor
  • 5. Proposed Solution –– Multifunctional propulsion-and-structure system that utilizes Lorentz forces (F = iL x B) generated by current carrying booms to generate thrust with little or no propellant expenditure •• Utilizes same principles as electrodynamic tether propulsion –– Utilize relatively short (≈≈100 meter), rigid booms with integrated conductors capable of carrying large currents, that have plasma contactors at the ends •• Space Tether Electrodynamic Propulsion –– Ex: 10km conductor, 1Ampere in LEO •• Thrust |iLxB| ≈≈ 0.3 Newtons –– Proposed Integrated Structural Propulsion •• Ex: 100m conductor, 100 Ampere (!) in LEO –– Thrust |iLxB| ≈≈ 0.3 Newtons –– Torque ≈≈ 750 N· m
  • 6. Single Boom Concept of Operation – Apply potential to overcome motion-induced electric field and drive current across magnetic field – Current flowing down boom produces thrust force – Plasma waves close the electrical circuit
  • 7. ‘‘Structural’’ ED Propulsion –– By connecting six booms to a spacecraft along orthogonal axes, 4DOF of motion can be controlled (translational and rotational)
  • 8. ISEP Booms –– Cold biased, low-resistance element to maximize propulsive performance •• Copper Clad Aluminum (CCA) offers low specific resistivity, yes remains easy to work with –– Ex. 0.01ΩΩ/50 meter boom has a 0.44 kg/m density –– Stiffness dictated by application –– Boom ends contain plasma contactors & docking sensors –– Hemaphroditic high-current capacity docking mechanism
  • 9. 100 Ampere Contactors for ISEP Emission Device Power Notes TC + Electron Gun 2.1 MW 18 emitters, < 1.25 V for SCL Electron FEA 5860 W 10 emitters, < 0.4 V for SCL Emission HC 1250 W to 10 kW Flow Rates & Ion Type 9 sccm to 40 sccm Xe Passive Sphere a 4.7 MW 1 m radius, 6.6E-3 N Drag 90% Porous – 6.6E-4 N Passive Sphere b 1 MW 2.29 m radius, 3.46E-2 N Drag 90% Porous – 3.46E-3 N Passive Plate a 61.3 MW 5 m2 – 5.26E-5 N Drag Passive Plate b 1 MW 54.52 m2 – 5.73E-4 N Drag Electron Collection HC 6150 W + 330 W (20 A ion prod.) 280 sccm fuel 27.35 mg/s Xe+ or 0.21 mg/s H+ Ion Emission + Ion Gun 1 MW + 1650 W (100 A ion prod.) 83,334 emitters needed Ion Emission HC 1000 W + 1650 W (100 A ion prod.) 1400 sccm fuel 27.35 mg/s Xe+ or 0.21mg/s H+
  • 10. ISEP Nodes –– Node geometry •• Simplest has 6 orthogonal mating surfaces •• Can also utilize polyhedrons with mating surfaces spaced 45° along the circumference –– Node components •• Energy storage (flywheels @ 75 W-hr/kg) •• System & Navigation Controllers
  • 11. Modular Spacecraft –– By making booms and spacecraft modules modular and interconnectable, we create self-assembling Tinkertoy® like components for space structures and systems
  • 12. ISEP Applications –– Self-Assembling Modular Spacecraft (SAMS) –– Self-Assembling Structure for Refueling Station •• Integral rail gun for commodity delivery –– Self-Assembling Space Tug –– Self-Assembling Structure for Large Mirror or Antenna Arrays –– Formation Flying Space Systems •• Terrestrial Planet Finder (TPF)
  • 13. 40000 35000 30000 25000 20000 15000 10000 5000 0 200.0 400.0 600.0 800.0 1000.0 1200.0 Circular Orbit Altitude (km) Delta-V (m/se Inclination = 0.0º Inclination = 28.5º Inclination = 51.6º Inclination = 90.0º Inclination = 97.0º ISEP Performance Analysis –– Six 50m orthogonal booms in 300-1100km, 0-97° inclination orbits –– FEAs for electron emission, HCs for ion emission –– Total system mass –– 1000kg with 20kg H consumable (approx 3 years full time operation) –– Current commanded to 100A continuous for 30 days •• System Input power - 6500 Watts –– Performance metrics tabulated & averaged 40000 35000 30000 25000 20000 15000 10000 5000 0 200.0 400.0 600.0 800.0 1000.0 1200.0 Circular Orbit Altitude (km) Delta-V (m/se Inclination = 0.0º Inclination = 28.5º Inclination = 51.6º Inclination = 90.0º Inclination = 97.0º 40000 35000 30000 25000 20000 15000 10000 5000 0 200.0 400.0 600.0 800.0 1000.0 1200.0 Circular Orbit Altitude (km) Delta-V (m/se Inclination = 0.0º Inclination = 28.5º Inclination = 51.6º Inclination = 90.0º Inclination = 97 0º Along-track Total ΔV Cross-track Total ΔV Radial TotalΔV
  • 14. ISEP Performance (cont.) –– Thrust magnitude and efficiency highly dependent on alignment of boom(s) with magnetic field –– Torques in the 1-10 N-m range as compared to disturbances in the 10-8 to 10-1 range 0.45 0.4 0.35 0.3 0.25 0.2 0.15 0.1 0.05 0 200.0 400.0 600.0 800.0 1000.0 1200.0 Circular Orbit Altitude (km) Thrust st ( Inclination = 0.0º Inclination = 28.5º Inclination = 51.6º Inclination = 90.0º Inclination = 97.0º Average Along-track Thrust (N) 200000 180000 160000 140000 120000 100000 80000 60000 40000 20000 0 200.0 400.0 600.0 800.0 1000.0 1200.0 Circular Orbit Altitude (km) Specific Impulse (se Inclination = 0.0º Inclination = 28.5º Inclination = 51.6º Inclination = 90.0º Inclination = 97.0º 10 9 8 7 6 5 4 3 2 1 0 Inclination = 0.0º Inclination = 28.5º Inclination = 51.6º Inclination = 90.0º Inclination = 97.0º 200 400 600 800 1000 1200 Along-track current torque (N-m) 200000 180000 160000 140000 120000 100000 80000 60000 40000 20000 0 Circular Orbit Altitude (km) Inclination = 0.0º Inclination = 28.5º Inclination = 51.6º Inclination = 90.0º Inclination = 97.0º 0 5 10 15 20 25 30 35 Thrust to Power Ratio (μN/W) ISEP boom Torque (N Specific Impulse (s Average Specific Impulse (Isp) Isp vs. Thrust to Power (uN/w)
  • 15. ISEP Performance –– ISEP is competitive with other EP technologies –– In systems where collinear booms are assembled, performance improves –– For missions where structural elements are required, ISEP’’s dual use (propulsive/structural) has significant advantages 1000000 100000 10000 1000 100 10 1 Resistojet Arcjet Pulsed Plasma Thruster Hall Effect Thruster Ion Thruster Integrated Structural EP 0.001 0.01 0.1 1 Thrust-to Power (N/kW) Specific Impulse (se –– KEY TECHNOLOGY CHALLENGE: Power- and Mass- Efficient collection and emission of electrons from/to the ambient plasma
  • 16. Technology Demonstration Experiment –– Primary Experiment Objectives •• Generate directly detectable torque •• Generate directly measurable thrust –– Secondary Experiment Objectives •• Validate performance of Field Emissive Electron device(s) •• Validate performance of lightweight electron collectors –– GOAL: Drive 1 Ampere of current through lightweight deployable, conductive 10-20 meter booms •• 0.2-1.0 second impulses > 0.5 mN
  • 17. Experimental Method –– Picosatellite launched as a secondary payload –– Target platform –– CubeSat •• 1kg –– 10x10x10 cm envelope •• Standard initially designed for University class experiments and educational purposes •• Typically 1-2 launch opportunities a year •• Launch costs $40-120K for a 1U CubeSat •• Ideal for simple experiments and technology demonstrations
  • 18. Picosat Experiment Contactors –– Field Emissive Cathodes •• Microfabricated Emitter tips rely on sharp emitter tips, and close non-intercepting electrodes to generate high field required to enable electrons to quantum tunnel out of the material into space •• High current densities (5000A/cm2) have been demonstrated •• Development undergoing to increase total current output and reduce environmental constraints –– Passive Electron Collector (‘‘Hedgehog’’) •• Bundle of conductive yarns •• Yarns tied together at root, and when charged will form approximately a ‘‘Koosh-ball’’ like spherical structure due to electrostatic repulsive forces •• 2 meter diameter structure with yarns every 40°, and filament every 1° can weigh 10 grams(!)
  • 19. Experiment Conops –– Converted Solar Energy is stored onboard in capacitor bank •• Allow for thrust pulse every 4-6 orbits –– At desired B-field alignment, discharge capacitor to generate 1Ampere pulse –– Measure Thrust with onboard accelerometers –– Measure Torque with body attitude rate change
  • 20. Summary –– Proposed Concept IS feasible •• Requires small amount of consumables for ion source •• 4DOF propulsion–– no thrust in B-field direction •• Competitive with tradition Electric Propulsion with added benefit of structural elements –– Technology Challenges •• High Current Plasma Contactors –– Devices exist –– robust units with higher efficiencies needed •• Plasma Contactor Space Charge Limiting –– High current densities may be environmentally limited •• Collision proof coordinated control laws for formation flight, and self-assembly –– Additional constraints imposed on low-thrust control laws –– Experiment in Phase II will demonstrate system feasibility and validate component technologies –– Potential Applications •• Space Tug and Commodity Depot (with integral rail gun?) •• Structure for Beamed Power Solar Array/Antenna Fields •• Structure for Space Habitats with Integral Drag Makeup