Title: A Comparison of Nuclear Thermal to Nuclear Electric Propulsion for Interplanetary Missions
1A Comparison of Nuclear Thermal to Nuclear
Electric Propulsion for Interplanetary Missions
- Mike Osenar
- Mentor LtCol Lawrence
2Overview
- Introduction
- Objective
- Establish parameters
- NTR Design
- NEP Design
- Discussion and Conclusion
3Introduction
- NASA is developing Nuclear Electric Propulsion
(NEP) systems for Project Prometheus, a series of
interplanetary missions - What happened to Nuclear Thermal Rocket (NTR)
systems? Should NASA only invest in NEP systems?
4Objectives
- Prove the feasibility of different nuclear
propulsion systems for interplanetary missions
which fit in a single launch vehicle - Compare NTR and NEP system designs for given
missions - Method take a set of inputs, use a series of
calculations and SPAD process along with
reasonable design assumptions to design a
spacecraft to reach a given ?V
5Establish Parameters
- Establish ?Vs and flight times for both NEP and
NTR systems to Jupiter and Pluto - Determine launch vehicle payload restrictions
- Obtain design points inert mass fractions based
on thruster specific impulses
6Establish Parameters
NTR ?V (km/sec) NEP ?V (km/sec) NTR TOF (years) NEP TOF (years)
Jupiter 3.83 7.66 4.13 4.13
Pluto 6.70 13.40 19.00 19.00
- NEP ?Vs and flight times based on AIAA 2002-4729
low thrust gravity assist trajectories - NTR data derived from NEP data
7Establish Parameters
- Relationship between NEP ?V/TOF and NTR ?V/TOF
- Table shows that NTR has same TOF for 50 of the
?V - NTR numbers based on AIAA 1992-3778
Mission ?V (km/s) TOF (yrs)
Pluto NEP 13.4 19
Pluto NTR 6.52 16
Pluto NTR 12.9 10
8Establish Parameters
- Ariane 5 Payload Specifications
Mass to orbit (kg) 18000
Height (m) 12.5
Diameter (m) 4.5
9Establish Parameters
10Establish Parameters
- Design points established from Dumbkopff charts
Design Isp (sec) ?V (km/sec) f-inert
Jupiter NTR 1000 3.83 0.65
Jupiter NEP (Ion) 3500 7.66 0.80
Jupiter NEP (Hall) 1500 7.66 0.60
Pluto NTR 1000 6.70 0.50
Pluto NEP (Ion) 3500 13.40 0.65
Pluto NEP (Hall) 1500 13.40 0.32
11NTR Design
- Size system so that it meets 3 specifications
- Under max payload mass
- Fits in payload fairing
- Reaches required ?V
12NTR Design
- Inputs from Dumbkopff finert, ?V
- Assumptions
- Po 7 MPa
- Isp 1000 s hydrogen
- Tc 3200 K
- T/W .3 experimented, balance between high
thrust short burn time and low reactor mass (low
power)
13NTR Design
- Equations for basic parameters
14NTR Design
- Subsystem Sizing (note volume constraint
?height) - Payload
- 1000 kg to Jupiter, 500 to Pluto
- based on densities of actual space mission
- sized as 2 m tall cylinder
- Tank
- biggest part hydrogen has low density
15NTR Design
- Turbo Pump Feed System
- Nuclear Reactor
- Radiation Shield
- standard SPAD design 18 cm Be, 5 cm W, 5 cm
LiH2 -
16NTR Design
- Nozzle
- Columbium, designed to be ideally expanded in
space (e100) - Miscellaneous
- Avionics
- Reactor containment vessel
- Attitude thrusters
- Structural mass
17NTR Design
- Achievable ?V verified with Rocket Equation
- Vehicle height determined by stacking parts
according to Figure
18NTR Design
- Final Results of NTR Design
?V (km/s) f-inert Initial Mass (kg) Height (m) Power (MWe) TOF (years)
Jupiter NTR 4.191 0.6094 9100.41 7.23 281.23 4.13
Pluto NTR 8.103 0.4182 14853.83 12.29 281.23 19.00
19NEP Design
- Size system so that it meets 2 specifications
- Under max payload mass
- Reaches required ?V
- No size requirement analysis showed that NEP
systems would violate mass constraints before
volume no low-density hydrogen propellant
20NEP Design
- Power Source
- Nuclear Reactors (Pgt6 kWe)
- Critical reactors designed as small as 6 kWe
- Radioisotope Thermoelectric Generators (RTG) (Plt6
kWe) - Solar?
21NEP Design
- Solar Power proportional to inverse square of
distance from sun - to receive power equal to 1 m2 solar panel in
earth orbit, would need 27 m2 panel at Jupiter
and 1562 m2 panel at Pluto - does not factor in degradation significant for
long lifetimes - engineering, GNC concerns with huge solar array
- mass too much
22NEP Design
- Thrusters based on actual designed thrusters from
SPAD - Baselines used T6, XIPS-25, RIT-XT
- Design allowed thrusters to be clustered in
groups of up to 3 proven to work, increases
force and power appropriately
23NEP Design
- Use NTR equations for propellant mass, thrust,
mass flow and power - NEP equations
24NEP Design
- Subsystem Design
- Power system
- Propellant tank
- Thruster mass
- Power conditioning mass
- Other mass (structural, feed systems, avionics,
etc.)
25NEP Design
?V (km/s) f-inert Initial Mass (kg) TOF (years) Power (kWe) of thrusters
Jupiter (Kaufman) 15.860 0.5266 4068.58 4.13 10.258 2
Jupiter (MESC) 14.051 0.5685 3673.06 4.13 8.425 2
Jupiter (RIT) 15.433 0.5622 3768.34 4.13 9.555 2
Jupiter (Hall) 12.242 0.3351 6645.87 4.18 6.180 3
Pluto (Kaufman) 42.725 0.2656 9495.62 18.79 10.258 2
Pluto (MESC) 41.420 0.2849 8079.27 19.40 8.425 2
Pluto (RIT) 44.626 0.2826 8352.61 19.19 9.555 2
Pluto (Hall) 13.771 0.3433 6719 19.02 1.471 1
26Discussion and Conclusion
- Overall, ?Vs were low real science mission
would need higher ?V to capture orbit of planet,
maneuver - Accurate data on EP trajectories was desired over
?Vs for realistic missions
27Discussion and Conclusion
- NTR Design
- Almost failed Pluto design tank volume
- High thrust, impulsive burn more reliable
operates for short time - Much less efficient then NEP
- Other applications? launch vehicle, human Mars
exploration
28Discussion and Conclusion
- NEP Design
- Low thrust, long trip times
- Lifetime analysis electric thrusters tested to
3.5 years less than Jupiter TOF - Space Nuclear reactors require extensive testing
29Discussion and Conclusion
- Testing extensive testing needed for either
system facilities, money needed to test for
operational lifetime - Safety perennial concern with nuclear systems,
real hazards to be considered - Radiological hazard higher with NEP (low power
but long burn time), must be addressed for either
system
30Discussion and Conclusion
- NASA probably right to go with NEP for
interplanetary missions - Much stands between now and operational nuclear
propulsion system - Much to be gained from nuclear propulsion
technology
31Discussion and Conclusion