A Comparison of Nuclear Thermal to Nuclear Electric Propulsion for Interplanetary Missions - PowerPoint PPT Presentation

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A Comparison of Nuclear Thermal to Nuclear Electric Propulsion for Interplanetary Missions

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A Comparison of Nuclear Thermal to Nuclear Electric Propulsion ... Fits in payload fairing. Reaches required ?V. NTR Design. Inputs from Dumbkopff: finert, ?V ... – PowerPoint PPT presentation

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Title: A Comparison of Nuclear Thermal to Nuclear Electric Propulsion for Interplanetary Missions


1
A Comparison of Nuclear Thermal to Nuclear
Electric Propulsion for Interplanetary Missions
  • Mike Osenar
  • Mentor LtCol Lawrence

2
Overview
  • Introduction
  • Objective
  • Establish parameters
  • NTR Design
  • NEP Design
  • Discussion and Conclusion

3
Introduction
  • 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?

4
Objectives
  • 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

5
Establish 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

6
Establish 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

7
Establish 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
8
Establish Parameters
  • Ariane 5 Payload Specifications

Mass to orbit (kg) 18000
Height (m) 12.5
Diameter (m) 4.5
9
Establish Parameters
10
Establish 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
11
NTR Design
  • Size system so that it meets 3 specifications
  • Under max payload mass
  • Fits in payload fairing
  • Reaches required ?V

12
NTR 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)

13
NTR Design
  • Equations for basic parameters

14
NTR 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

15
NTR Design
  • Turbo Pump Feed System
  • Nuclear Reactor
  • Radiation Shield
  • standard SPAD design 18 cm Be, 5 cm W, 5 cm
    LiH2

16
NTR Design
  • Nozzle
  • Columbium, designed to be ideally expanded in
    space (e100)
  • Miscellaneous
  • Avionics
  • Reactor containment vessel
  • Attitude thrusters
  • Structural mass

17
NTR Design
  • Achievable ?V verified with Rocket Equation
  • Vehicle height determined by stacking parts
    according to Figure

18
NTR 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
19
NEP 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

20
NEP Design
  • Power Source
  • Nuclear Reactors (Pgt6 kWe)
  • Critical reactors designed as small as 6 kWe
  • Radioisotope Thermoelectric Generators (RTG) (Plt6
    kWe)
  • Solar?

21
NEP 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

22
NEP 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

23
NEP Design
  • Use NTR equations for propellant mass, thrust,
    mass flow and power
  • NEP equations

24
NEP Design
  • Subsystem Design
  • Power system
  • Propellant tank
  • Thruster mass
  • Power conditioning mass
  • Other mass (structural, feed systems, avionics,
    etc.)

25
NEP Design
  • NEP Design Results

?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
26
Discussion 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

27
Discussion 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

28
Discussion 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

29
Discussion 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

30
Discussion 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

31
Discussion and Conclusion
  • Questions?
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