Z Pinch
description
Transcript of Z Pinch
-
1Conceptual Design of a Z-Pinch Fusion
Propulsion System
Advanced Concepts Office
George C. Marshall Space Flight Center
National Aeronautics and Space Administration
Robert Adams, Ph.D.
-
2Team Members
Polsgrove T., Fincher, S., Adams, R. NASA (MSFC)
Fabisinski, L. - International Space Systems, Inc.
Maples, C. - Qualis Corporation
Miernik, J., Statham, G. - ERC, Inc.
Cassibry, J., Cortez, R., Turner, M. - UAHuntsville
Santarius, J. - University of Wisconsin
Percy, T. - SAIC, Inc.
National Aeronautics and Space Administration
George C. Marshall Space Flight Center
ED04/Advanced Concepts Office
-
3Z-Pinch Fusion: Background
Nuclear weapon x-rays are simulated through Z-Pinch phenomena.
New developments in multi-keV plasma radiation sources are progressing to thermonuclear fusion
temperatures*
Such technology could be applied to develop advanced thruster designs that promise high thrust/high specific
impulse propulsion
This project would develop a conceptual design for such a thruster.
*Velikovich, A. L., R. W. Clark, J. Davis, Y. K. Chong, C. Deeney, C. A. Coverdale, C. L. Ruiz, et al. 2007, Z-pinch plasma neutron sources,
Physics of Plasmas 14, no. 2: 022701. doi:10.1063/1.2435322.
-
4Operation of a Z Pinch
Cathode
Anode
Hypersonic Nozzle
I
Gas Cylinder
Evacuated Chamber
-
5High Current Generates Intense
Magnetic Fields
I
B, Magnetic Flux
-
6Magnetic Fields Compress the
Plasma to X-Ray Temperatures
Ion Motion B
X-rays
-
7Plasma Instability
Rayleigh-Taylor is most deleterious effect
preventing success,
can be overcome with
tailored density profile*
*Velikovich, Cochran, and Davis, Phys. Rev. Let. 77(5) 1996.
-
8Electrode Erosion
Coupling electrical energy to plasma Directly coupled devices lead to erosion
All susceptible to x-ray radiation and neutron damage
Potential workarounds Allow electrodes to erode!
Consider inductively coupled techniques
-
9Thruster Concept
Hypersonic NozzlesCathode
Anode
Z-Pinch
D-T Fuel
Secondary Fuel
And Radiation
Shield
MHD Generator
-
10
Z-pinch Design
Annular nozzles with Deuterium-
Tritium (D-T) fuel in
the innermost
nozzle
Lithium mixture containing Lithium-
6/7 in the outermost
nozzle.
The D-T fuel and Lithium-6/7 mixture
acts as a cathode
-
11
Z-pinch modeling
Treat Z-pinch as Otto cycle
Process 1-2: Isentropic compression
Process 2-3: Constant volume heat addition
Process 3-4: Isentropic expansion
Process 4-1: Constant volume heat rejection
-
12
Engine Performance
Engine Performance as a function of liner mass
Design point picked based on mission needs
-
13
Nozzle Performance
Particle trajectory modeling required to estimate performance and correctly size nozzle.
National Aeronautics and Space Administration
George C. Marshall Space Flight Center
ED04/Advanced Concepts Office
-
14
0.0%
5.0%
10.0%
15.0%
20.0%
25.0%
30.0%
35.0%
40.0%
45.0%
50.0%
0 20000 40000 60000 80000 100000 120000
Mission Delta-V (m/s)
Paylo
ad
% (
Paylo
ad
Mass /
IM
LE
O)
Mars Round Trip (90 Days One Way)
Mars Round Trip (30 Days One Way)
Jupiter Round Trip
One Way Trip to Mars (180 Days One Way)
One Way Trip to Mars (90 Days One Way)
Traditional Chemical
Propulsion
Z-Pinch Fusion
Propulsion
Missions to Mars, Jupiter, and Beyond can be achieved
with significantly reduced trip times when
compared to state of the art chemical propulsion
90 day transfer
from Earth to
Mars
Missions Enabled
-
15
Mission Analysis
Mars 90 Mars 30 Jupiter 550 AU
Outbound Trip Time (days) 90.2 39.5 456.8 12936
Return Trip Time (days) 87.4 33.1 521.8 n/a
Total Burn Time (days) 5.0 20.2 6.7 11.2
Propellant Burned (mT) 86.3 350.4 115.7 194.4
Equivalent DV (km/s) 27.5 93.2 36.1 57.2
National Aeronautics and Space Administration
George C. Marshall Space Flight Center
ED04/Advanced Concepts Office
Figure 4.1 Mars 90 Day Transfer Trajectories
Mars Orbit
Earth Orbit
Transfer Traj Orbit
Transfer Trajectory
Mars Orbit
Earth Orbit
Transfer Traj Orbit
Transfer Trajectory
-
16
Vehicle Configuration
Subsystem Mass (kg)
Payload 150,000
Structures 54,600
Main Propulsion 95,138
RCS 586
Thermal 77,164
Power 16,480
Avionics 389
Total Dry Mass 394357
30% MGA 73,307
Total Mass 467,664
-
17
Thrust Coil Configuration
FLiBe protects thrust and seed coils from thermal flux and other radiation.
National Aeronautics and Space Administration
George C. Marshall Space Flight Center
ED04/Advanced Concepts Office
Seed Field
Superconductor
and LN2
coolant channelKapton
Insulator
Seed Coil
Load
Structure
Radiant Heat
Shield
Seed Field
Coil Housing
Evacuated
Region Molten mixture of lithium fluoride
(LiF) and beryllium fluoride (BeF2)
[FLiBe].
Thrust Coil
Load
Structure
Thrust Coil
Conductor
Diagram intended to illustrate the general
composition of the rings that comprise the nozzle.
Dimensions and aspect ratio to be determined
after detailed structural analysis.
Neutron
protection/cooling
channelZirconium diboride
(ZrB2) ceramic shell
Direction
of Fusion
-
18
Power Management System
National Aeronautics and Space Administration
George C. Marshall Space Flight Center
ED04/Advanced Concepts Office
Recharging for next pulse one of the major
technical challenges for pulsed fusion
-
19
Structural Analysis of Magnetic
Nozzle
Structural truss can handles stresses from pulsed fusion indefinitely.
National Aeronautics and Space Administration
George C. Marshall Space Flight Center
ED04/Advanced Concepts Office
Focal point of nozzle
-
20
Thermal Management System
Radiators operate at 300 K, 800 K and 1400 K.
National Aeronautics and Space Administration
George C. Marshall Space Flight Center
ED04/Advanced Concepts Office
-
21
Avionics Suite
National Aeronautics and Space Administration
George C. Marshall Space Flight Center
ED04/Advanced Concepts Office
-
22
DECADE Module II
500 kJ pulsed power facility
Last prototype built before DECADE construction
Defense Threat Reduction Agency Nuclear Weapons Effects (NWE)
Plasma Radiation Sources (PRS)
Good working order
Capable of >1 TW instantaneous power (about 6% of world's
electrical power consumption)
-
23
Pulsed Fusion Facility
DM2 Utilization Arrangements L3 Communications, Pulsed Science Division
Boeing
Oak Ridge National Labs
Other fusion collaborations LANL
HyperV Corp.
Univ. of New Mexico
Expected Capabilities 500 ns pulse, 2 MA current
1 keV, 1025 /m3 plasma state
Effective dwell time of ~100 nsAerophysics
lab
-
24
Summary
No showstoppers found for this technology Preliminary analytical results are promising
The technology development required for this propulsion system is achievable on a reasonable timescale given sufficient resources.
Z-pinch has potential for a number of missions of interest Reusable vehicle that recaptures in Earth Orbit does round trips to Mars
Interstellar precursor missions
Crewed Missions to other solar system targets
Opportunity to create new facility to explore z-pinch and other pulsed fusion concepts Looking for funding to move module to MSFC for installation
Completed facility would allow proof of principle experiments on pulsed fusion concepts.
Our team thanks the NASA Innovative Programs and Partnerships Program for funding this work
National Aeronautics and Space Administration
George C. Marshall Space Flight Center
ED04/Advanced Concepts Office