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Andrew Petro Advanced Space Propulsion Laboratory  NASA JSC Houston, Texas May 2002 VASIMR Plasma Rocket Technology

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Andrew PetroAdvanced Space Propulsion Laboratory

 NASA JSC Houston, Texas

May 2002

VASIMR Plasma Rocket

Technology

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

OUTLINE

• Introduction

• Development Roadmap

• Flight Demonstration Concepts

• Mission Applications

• Experimentation

• Source, ICRF, Nozzle

• Theoretical Studies

• Source, ICRF, Nozzle

Andrew Petro

Andrew Ilin

VASIMR Plasma Rocket Technology

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

• A high-Isp plasma rocket for space explorationand commercial applications• short trip times• high payload capacity• mission flexibility and abort capability• high-efficiency orbit transfer

• Potential drag compensation for the ISS

•Variable specific impulse to improve trajectory optimization• higher thrust for escape from planetary orbits• higher efficiency for interplanetary cruise

• Magnetoplasma technology is relevantto more advanced systems (including fusion)

• No moving parts, no combustion, no electrodes

• Hydrogen propellant: plentiful, inexpensive, andthe best known radiation shield

Variable Specific Impulse Magnetoplasma Rocket

Benefits of VASIMR Propulsion

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

Propellant

feed Ionizing antenna

(helicon)

Magnetic

field lines

Exhaust

Heating antenna

(ICRF)

Plasma

Magnet coils

RF generators

POWER 

POWER 

Thrust

Simplified Diagram of VASIMR Thruster

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

Development &

Ground Testing

2000 2005 2010 2015 2020 2025 2030

20-50 kW

100 kW

1 MW

10 kW

50 kW

100 kW

1 MW

100 MW

SOLAR 

POWER 

NUCLEAR 

POWER 

Space Demonstration &

Applications

100 MW

Development Roadmap

ISS Demo

Satellite

Demo

Deep Space

Science Missions

Exploration

Missions

Laboratory

A variety of demonstrations and applications of increasing capability are envisioned

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

Thruster

Core

RF Amplifier Set

(1 of 4)

Radiator

Rechargeable

Batteries

Propellant

Tanks

Approximate Dimensions

of Thruster Core:

Diameter < 0.5 m

Length < 1 m

Proposed VASIMR Experiment on ISS

Initial Experiment• Near-term, low-cost, minimuminterfaces with ISS

• Periodic operation with stored power(25 kW)

• 0.2 N thrust, 10,000 sec Isp• 0.5 N thrust, 5400 sec Isp

• Gaseous hydrogen propellant

Eventual Operations• Continuous power• Demonstrate VASIMR and otherelectric propulsion

• Reduce propellant for reboost• Extremely high Isp• Waste gas usage

• Improve ?g environment

• Serve as plasma contactor • ISS becomes advanced technologytest bed

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

POTENTIAL ISS LOCATION

Attachment at external payload siteon P3 (or S3) truss segment shown

Proposed VASIMR Experiment on ISS

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

Plasma in labexperiment

Prototype RF amplifier 

Universal Mini-Controller 

MMU propellant tank 

Superconducting magnet

ICRF antenna

Flight-like Component Development and Testing

 NiCd Batteriesdeveloped for X-38

Standard payloadinterface

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

- Demonstrate advanced space propulsion technology

- Measure natural radiation environment from low to high Earth orbit

• Deploy from Shuttle and

climb to high Earth orbit

• Solar Power: 10-12 kW

• Demonstrate two different propulsion

systems

•VASIMR •Hall thruster

• Operate scientific instruments on spacecraft

and on deployed microsatellites

Free-Flying Space Demonstration

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

10 Kilowatt Thruster Design

For Free-Flyer Mission

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

Nuclear Electric Europa Mission Concept

VASIMR Propulsion

with 50 kW nuclear power generator

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

   T   h  r  u  s   t

   (   N   )

  n   (  m  -   3   )

Earth-to-Mars Thrust Vector

Isp Profile

VASIMR Performance

Piloted Mars Mission

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

Piloted Mars Mission

Crew Lander (60.8 mt Payload)31.0 mt Habitat

13.5 mt Aeroshell16.3 mt Descent System

Departing LEO May 6, 2018

188 mt IMLEO, 12 MW power plant, ? = 4 kg/kW

30 Day Spiral 85 Day Heliocentric Transfer

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

Mars Mission Abort Capability

Aborts due to loss of propellant

Aborts deep into the mission due to non

 propulsion system failures

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

Radiation Shielding with Hydrogen Propellant

Depth, g/cm20 10 20 30 40 50

   G   C   R   D  o  s  e ,  m   S  v   /   d  a  y

0.0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

Aluminum

Water 

Polyethylene

Liquid hydrogen

LH 2 propellant provides

crew shielding 

Hydrogen is the best material for shielding

humans from radiation in space.

VASIMR propellant can provide effective

radiation protection for the entire trip.

The graph shows radiation shielding

capability for various materials.

Two Mars Vehicle Concepts

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

0

1000

2000

3000

4000

Mass

(metric tons)

1Propulsion Type

Initial Mass for One-Year Round Trip to Mars

Chemical

Tether/Chemical

Nuclear Thermal

Nuclear Electric -

VASIMR

OUTBOUND CREW SHIP FOR ONE-YEAR ROUND TRIP MISSIONSIZE COMPARISON TO SPACE SHUTTLE ORBITER 

Comparative Study of One-Year Round-Trip Mission to Mars

Crew of Four

Fast Human Mars Missions

From MSFC/SAIC Study July 2000

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

200MW Earth to Mars Missions

? = 0.5

Maximal Isp = 30,000

Payload Mass = 22 mt

Total Initial Spiraling around Earth Heliocentric trajectory Final relative Total trip

Mass (mt) fuel (mt) time (days) fuel (mt) time (days) velocity (km/s) time (days)

600 180 7 298 34 0 41

350 117 5 111 42 0 47

250 88 4 40 49 0 53

600 152 8 324 31 6.8 39

Higher Power Dramatically Reduces Trip Time

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

Summary

• Power-rich architectures offer the most robust systems forspace exploration

• High power electric propulsion with variable thrust and Ispreduces risk and provides mission flexibility

• High-Isp propulsion systems have potential in near-Earthapplications

• The ISS can become an important facility for demonstratingadvanced propulsion and power technology and those testoperations can directly benefit the ISS.

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

Backup Charts

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

Main DOE and University Collaborators

• Oak Ridge National Laboratory, Fusion Energy Division: Dr. Stanley Milora, Director 

 – Dr. Wally Baity, RF systems (team lead)

 – Dr. Mark Carter, RF systems, plasma theory, magnetic system design

 – Dr. Rick Goulding, experimental plasma generation and heating

 – Dr. William Schwenterly, superconducting magnet design• Los Alamos National Laboratory :

 – Drs. Pat Colestock and Max Light, helicon physics and wave diagnostics

• MSE Technology Inc.(former DOE facility:) Mr. David Micheletti, Program Manager 

 – Dr. Jean Luc Cambier, plasma fluid (MHD) simulation

• University of Texas, Austin, Fusion Research Center:

 – Dr. Roger Bengtson, experimental plasma physics and diagnostics (team lead)

 – Dr. Boris Breizman, plasma theory and system scaling

• University of Maryland, Dept. of Physics/East West Space Science Center: Dr. Roald Sagdeev, Director 

 – Dr. Konstantinos Karavasilis, trajectory simulation and optimization

 – Dr. Sergei Novakovski, plasma fluid (MHD) simulation

• Rice University, Dept. of Physics and Astronomy: Dr. Patricia Reiff, Dept. Chair 

 – Dr. Anthony Chan, plasma theory (team lead)

 – Dr. Carter Kittrell, experimental plasma spectroscopy

• University of Houston, Dept. of Physics:

 – Dr. Edgar Bering, experimental plasma physics and ion diagnostics

• MIT, Dept. of Nuclear Engineering: Dr. Jeffrey Fryberg, Dept. Chair 

 – Dr. Oleg Batischev, plasma non-linear theory and simulation

• MIT, Plasma Science and Fusion Center: Dr. Miklos Porkolab, Director 

 – Dr. Joseph Minervinni (team lead) superconducting magnet design

 – Dr. Joel Schultz, Superconducting magnet design

• Princeton Plasma Physics Laboratory :

 – Dr. Samuel Cohen, Magnetic nozzle and plasma diagnostics

• University of Michigan:

 – Dr. Brian Gilchrist, plasma interferometry

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

0 0.2 0.4 0.6 0.8 1 1.2 1.4

-0.4

-0.3

-0.2

-0.1

0

0.1

0.2

0.3

0.4

Magnetic Field Lines

meters

meters

24 kW VASIMR 

50 MA/m2 current

Four coils

Magnet mass: 37 kg

Andrew Ilin

HELICONICRF

M1M2

M3

M4

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

Physics of the VASIMR 

Charged particles (protons and

electrons) move in helical orbits

at their cyclotron frequency.

When particles see an expanding

magnetic field, they are

accelerated axially at the expense

of their rotational motion.

Magnetic Mirror

Magnetic Nozzle

Both ions and electrons

leave at the same rate!

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

Thermal Studies

Helicon

tube watts 

Thermal envir onment of enti re

system 

Thermal control of

superconductor 

Thermal envir onment

of heli con tube.

0.5oK 

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

VX-10 Development &Testing

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

5 kg superconducting magnet will replace

150 kg conventional LN2-cooled magnet

A vacuum chamber has been assembled for

thermal testing of the superconducting

magnet and cryocooler prior to integration

into the VASIMR experiment.

Superconducting Magnet Technology

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

Definitions

• Plasma: A super heated gas of electrically charged particles at temperatures

greater than 10,000o

K. A magnetic field is used to guide and control the plasma (magnetoplasma.)

• VASIMR:Variable Specific Impulse Magnetoplasma Rocket.

• RF: radio frequency power used to create and heat the plasma in the

VASIMR.

• Helicon: 1st stage of VASIMR, is a high density plasma source, working

with RF power to breakdown the propellant gas and produce the plasma.

• ICRH: ion cyclotron resonance heating, is the mechanism by which RF

waves further heat the plasma in the VASIMR 2nd stage. They do so by

resonating with the natural cyclotron motion of the ions in the magnetic

field.

• Bekuo: means “Star or Shooting Star” in the language of the Bri-Bri Indians

of Costa Rica, descendants of the Maya. The name honors the native

American civilizations, our earliest scientists and astronomers.

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 NASA Johnson Space Center, Advanced Space Propulsion Laboratory

VASIMR Primer

The VASIMR system is a high power, electrothermal plasma rocket featuring a very

high specific impulse (Isp) and a variable exhaust. Its unique architecture allows in-

flight mission-optimization of thrust and Isp to enhance performance and reduce triptime. VASIMR consists of three major magnetic stages where plasma is respectively

injected, heated and expanded in a magnetic nozzle. The magnetic configuration is

called an asymmetric mirror. The 1st stage handles the main injection of propellant gas

and the ionization subsystem; the 2nd stage acts as an amplifier to further heat the

 plasma. The 3rd stage is a magnetic nozzle which converts the plasma energy into

directed momentum. The magnetic field insulates nearby structures from the high

 plasma temperature (>1,000,000 oK.) It is produced by high temperature

superconductors cooled mainly by radiation to deep space. Some supplemental cooling

from the cryogenic propellants ( hydrogen, deuterium, helium or mixtures of these)

may also be used.

The system is capable of high power density, as the plasma energy is delivered by

wave action, making it electrodeless and less susceptible to component erosion.

Plasma production is done in the 1st

stage by a helicon discharge, while additional plasma heating is accomplished in the 2nd stage by the process of ion cyclotron

resonance.