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Enabling outer planet exploration: performance and feasibility of nuclear thermal propulsion for rendezvous missions

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... Finally, the last module of the systems engineering model is cost estimation. In the paper, the mission cost is determined as a function of launch vehicle cost plus spacecraft dry mass using the historical data of NASA's planetary science missions cost versus spacecraft dry mass [28]. Considering that the NTP system is currently in the development phase, the cost estimate of the propulsion system is beyond the scope of this study. ...
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Nuclear thermal propulsion (NTP) has emerged as a promising technology for enhancing the capabilities of robotic missions in space exploration. This paper investigates and analyzes the tradeoffs and sensitivity associated with utilizing NTP systems for robotic missions to the outer planets. The engine trade results for Jupiter and Neptune rendezvous missions using expendable configuration have demonstrated that the thrust range of 12.5–15 k-lbf (55.6–66.7 kN) can enable new frontiers and flagship-class missions with minimum initial mass in low Earth orbit. The specific impulse sensitivity analysis has shown that using a 13 k-lbf (57.8 kN) engine with an [Formula: see text] as low as 850 s can enable flagship-class missions to the gas giants in a direct transfer trajectory.
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Full-text available
Nuclear thermal propulsion (NTP) has emerged as a promising technology for enhancing the capabilities of robotic missions in space exploration. This paper investigates and analyzes the tradeoffs and sensitivity associated with utilizing NTP systems for robotic missions to the outer planets. The engine trade results for Jupiter and Neptune rendezvous missions using expendable configuration have demonstrated that the thrust range of 12.5–15 k-lbf (55.6–66.7 kN) can enable new frontiers and flagship-class missions with minimum initial mass in low Earth orbit. The specific impulse sensitivity analysis has shown that using a 13 k-lbf (57.8 kN) engine with an [Formula: see text] as low as 850 s can enable flagship-class missions to the gas giants in a direct transfer trajectory.
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Nuclear Thermal Propulsion (NTP) has emerged as a promising technology for enhancing the capabilities of robotic missions in space exploration. This paper aims to investigate and analyze the trade-offs and sensitivity associated with utilizing NTP systems for robotic missions to the outer planets. The engine trade results for Jupiter and Neptune rendezvous mission using expendable configuration has demonstrated that the thrust range of 12.5 klbf to 15 klbf can enable flagship class missions with minimum IMLEO. The specific impulse sensitivity analysis has shown that using a 13 klbf engine with as low was 850 s can enable flagship class missions to the Gas giants in a direct transfer trajectory.
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NASA has recently identified Nuclear Thermal Propulsion (NTP) as a critical technology for the human exploration of Mars. Recent studies have also demonstrated its unique capabilities towards enabling deep space exploration robotic missions with higher payload mass and/or reduced trip times. This game changing technology can also provide the efficient cargo and crew transportation through cislunar space for sustained human presence on the Moon. The NTP systems capability of generating both high thrust and high specific impulse (over twice of the best chemical propulsion systems) can enable a variety of lunar missions (rendezvous and round-trip) which can play critical role in the next phase of lunar exploration. This paper presents the applications of the NTP for sustainable cislunar exploration and identifies the most efficient architectures and engine thrust class for host of lunar missions.
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Chemical propulsion has been the primary propulsion system from the beginning of space age for interplanetary robotic missions1. However, the chemical propulsion system has shown its limitations towards the exploration of outer planets and beyond due to its low energy density and low specific impulse. An outer planet mission using only chemical propulsion system would not be possible without multiple gravity assists or by utilizing a super heavy lift launch vehicle. On the other hand, the advancements in the Nuclear Thermal Propulsion (NTP) system using Low Enriched Uranium (LEU) NTP engine system design have demonstrated the improved performance towards payload mass and short transit time2. High thrust and high specific impulse (over twice the best chemical propulsion engine) NTP system can enable missions which have been limited due to the large ΔV requirements. An NTP propelled spacecraft with high ΔV would reduce the trip time by up to a factor of two or more when compared with a chemical propulsion system spacecraft requiring multiple gravity assists. This work examines the capability of an NTP powered spacecraft for Jupiter rendezvous mission and discusses the advantages in terms of payload delivery and trip time in comparison to the conventional chemical propulsion powered spacecrafts.
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View Video Presentation: https://doi.org/10.2514/6.2021-3598.vid A model-based approach can enhance the conceptual mission design process for NTP enabled robotic missions. This paper presents the early steps taken on the implementation of Model-Based Systems Engineering (MBSE) application with final goal to have rapid integrated system analysis capability. The paper describes the NTP mission model and process of deriving mission requirement diagrams. The modeling approach has been implemented on a conceptual mission design process of an NTP powered robotic mission to Neptune.
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This paper presents a Jupiter rendezvous mission using nuclear thermal propulsion system which will focus on end-to-end trajectory analysis and highlight the complexities of Earth escape and planetary orbital insertion using finite burn maneuvers. The detailed mission design includes spacecraft design, launch schedule, delta-V requirements and multi body high-fidelity finite thrust trajectory analysis. Spacecraft’s initial low Earth parking orbit is considered to be circular at 1000 km in altitude and at 28 degrees inclination. The high fidelity trajectory analysis of the nuclear thermal propulsion spacecraft for a rendezvous mission has been divided into three phases - Earth escape, coasting and orbit insertion phase.
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The nuclear thermal rocket (NTR) represents the next “evolutionary step” in high performance rocket propulsion. Unlike conventional chemical rockets that produce their energy through combustion, the NTR derives its energy from fission of Uranium-235 atoms contained within fuel elements that comprise the engine's reactor core. Using an “expander” cycle for turbopump drive power, hydrogen propellant is raised to a high pressure and pumped through coolant channels in the fuel elements where it is superheated then expanded out a supersonic nozzle to generate high thrust. By using hydrogen for both the reactor coolant and propellant, the NTR can achieve specific impulse (Isp) values of ~900 seconds (s) or more - twice that of today's best chemical rockets. From 1955-1972, twenty rocket reactors were designed, built and ground tested in the Rover and NERVA (Nuclear Engine for Rocket Vehicle Applications) programs. These programs demonstrated: (1) high temperature carbide-based nuclear fuels; (2) a wide range of thrust levels; (3) sustained engine operation; (4) accumulated lifetime at full power; and (5) restart capability - all the requirements needed for a human Mars mission. Ceramic metal “cermet” fuel was pursued as well, as a backup option. The NTR also has significant “evolution and growth” capability. Configured as a “bimodal” system, it can generate its own electrical power to support spacecraft operational needs. Adding an oxygen “afterburner” nozzle introduces a variable thrust and Isp capability and allows bipropellant operation. In NASA's recent Mars Design Reference Architecture (DRA) 5.0 study, the NTR was selected as the preferred propulsion option because of its proven technology, higher performance, lower launch mass, versatile vehicle design, simple assembly, and growth potential. In contrast to other advanced propulsion options, no l- rge technology scale-ups are required for NTP either. In fact, the smallest engine tested during the Rover program - the 25,000 lbf (25 klbf) “Pewee” engine is sufficient when used in a clustered engine arrangement. The “Copernicus” crewed spacecraft design developed in DRA 5.0 has significant capability and a human exploration strategy is outlined here that uses Copernicus and its key components for precursor near Earth object (NEO) and Mars orbital missions prior to a Mars landing mission. The paper also discusses NASA's current activities and future plans for NTP development that include system-level Technology Demonstrations - specifically ground testing a small, scalable NTR by 2020, with a flight test shortly thereafter.
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The high precision mean element (semianalytic) satellite theory developed at Draper Laboratory is more efficient than conventional numerical methods and more accurate than the current generation of analytic theories. This efficiency, along with its portability to a variety of computing environments makes the semianalytic theory a natural choice for maneuver planning applications. These applications will become more important in the future as the capability of individual platforms to maneuver, the number of platforms in space, and the requirements for rapid response to requests for data all increase. The application of semianalytic satellite theory to an Earth Observation satellite in an orbit similar to that expected for LANDSAT 6 is investigated. Orbit constraints such as sun synchronous, repeat ground track, frozen orbit, and non-impulsive maneuver capabilities are included in this analysis. Applications of maneuver planning to past and future satellite missions that include at least two of the listed orbit constraints are discussed. Since atmospheric drag is the primary uncertain disturbing acceleration to the nominal satellite orbit, upper and lower limits of a density confidence interval were determined. Two methods were analyzed; it was found that using forecast and actual solar flux and geomagnetic activity data from the years 1986-1990 resulted in a conservative but realistic confidence interval. The upper limit is utilized to compute the time of the orbit adjust burn and the lower limit of the density is used to calculate the magnitude of the orbit adjust burn. These limits are necessary so that the ground track boundaries are not exceeded.
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We have conducted studies of a revolutionary new concept for conducting a Europa Sample Return Mission. Robotic spacecraft exploration of the Solar System has been severely constrained by the large energy requirements of interplanetary trajectories and the inherent delta V limitations of chemical rockets. Current missions use gravitational assists from intermediate planets to achieve these high-energy trajectories restricting payload size and increasing flight times. We propose a 6-year Europa Sample Return mission with very modest launch requirements enabled by MITEE. A new nuclear thermal propulsion engine design, termed MITEE (MIniature reacTor EnginE), has over twice the delta V capability of H2/O2 rockets (and much greater when refueled with H2 propellant from indigenous extraterrestrial resources) enabling unique missions that are not feasible with chemical propulsion. The MITEE engine is a compact, ultra-lightweight, thermal nuclear rocket that uses hydrogen as the propellant. MITEE, with its small size (50 cm O.D.), low mass (200 kg), and high specific impulse (~1000 sec), can provide a quantum leap in the capability for space science and exploration missions. The Robotic Europa Explorer (REE) spacecraft has a two-year outbound direct trajectory and lands on the satellite surface for an approximate 9 month stay. During this time, the vehicle is refueled with H2 propellant derived from Europa ice by the Autonomous Propellant Producer (APP), while collecting samples and searching for life. A small nuclear-heated submarine probe, the Autonomous Submarine Vehicle (ASV), based on MITEE technology, would melt through the ice and explore the undersea realm. The spacecraft has approximately a three year return to Earth after departure from Europa with samples onboard. Spacecraft payload is 430 kg at the start of the mission and can be launched with a single, conventional medium-sized Delta III booster. The spacecraft can bring back 25 kg of samples from Europa. Europa, in the Jovian system, is a high priority target for an outer Solar System exploration mission. More than a decade ago the Voyager spacecraft revealed Europa as a world swathed in ice and geologically young. NASA's Galileo spacecraft passed approximately 500 miles above the surface and provided detailed images of Europa's terrain marked by a dynamic topology that appeared to be remnants of ice volcanoes or geysers. The surface temperature averages a chilly -200° C. The pictures appear to show a relatively young surface of ice, possibly only 1 km thick in some places. Internal heating of Europa from Jupiter's tidal pull could form an ocean of liquid water beneath the surface. More recently, Ganymede and Callisto are believed to be ocean-bearing Jovian moons based on magnetometer measurements from the Galileo spacecraft. If liquid water exists, life may also. NASA plans to send an orbiting spacecraft to Europa to measure the thickness of the ice and to detect if an underlying liquid ocean exists. This mission would precede the proposed Europa Sample Return mission, which includes dispatching an autonomous submarine-like vehicle that could melt through the ice and explore the undersea realm. Because of the large energy requirements typical of these ambitious solar system science missions, use of chemical rockets results in interplanetary spacecraft that are prohibitive in terms of Initial Mass in Low- Earth Orbit (IMLEO) and cost. For example, using chemical rockets to return samples from Europa appears to be technically impractical, as it would require large delta V and launch vehicle capabilities. On the other hand, use of nuclear thermal rockets will significantly reduce IMLEO and, subsequently, costs. Moreover, nuclear thermal rockets can utilize extraterrestrial resources as propellants, an option not practical with chemical rockets. This "refueling" capability would enable nuclear rockets to carry out very high-energy missions, such as the return of large amounts of extraterrestrial material to Earth. The Europa missions considered in this proposal will be restricted to starting from LEO only after being placed in a stable orbit by a launch vehicle. This simplifies and eases the safety issues and mitigates political concerns. High propulsive efficiency of the MITEE engine yields the benefits of reduced transit time and a smaller launch vehicle.
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Several topics are presented in viewgraph form which together encompass the preliminary assessment of nuclear thermal rocket engine clustering. The study objectives, schedule, flow, and groundrules are covered. This is followed by the NASA groundrules mission and our interpretation of the associated operational scenario. The NASA reference vehicle is illustrated, then the four propulsion system options are examined. Each propulsion system's preliminary design, fluid systems, operating characteristics, thrust structure, dimensions, and mass properties are detailed as well as the associated key propulsion system/vehicle interfaces. A brief series of systems analysis is also covered including: thrust vector control requirements, engine out possibilities, propulsion system failure modes, surviving system requirements, and technology requirements. An assessment of vehicle/propulsion system impacts due to the lessons learned are presented.
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The parallel special perturbation catalog maintenance software "SpecialK" being introduced at Naval Space Command uses an eighth order Gauss-Jackson predictor-corrector for numerical integration. This integrator comes from legacy code which is not extensively documented. A study of the theory upon which the integrator is based and the method by which the integrator is implemented in the software is necessary, to determine if speed or accuracy improvements can be made. This paper presents some results from the study, including a discussion of a variable step size method that had been implemented in the ancestor code that proves to be ineffective.
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An analytical solution is given for the motion of an artifical Earth satellite under the combined influences of gravity and atmospheric drag. The gravitational effects of the zonal harmonicsJ 2,J 3, andJ 4 are included, and the drag effects of any arbitrary dynamic atmosphere are included. By a dynamic atmosphere, we mean any of the modern empirical models which use various observed solar and geophysical parameters as inputs to produce a dynamically varying atmosphere model. The subtleties of using such an atmosphere model with an analytic theory are explored, and real world data is used to determine the optimum implementation. Performance is measured by predictions against real world satellites. As a point of reference, predictions against a special perturbations model are also given.
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A new compact ultra light nuclear reactor engine design termed MITEE (MIniature Reac Tor EnginE) is described. MITEE heats hydrogen propellant to 3000 K, achieving a specific impulse of 1000 seconds and a thrust-to-weight of 10. Total engine mass is 200 kg, including reactor, pump, auxiliaries and a 30% contingency. MITEE enables many types of new and unique missions to the outer solar system not possible with chemical engines. Examples include missions to 100 A.U. in less than 10 years, flybys of Pluto in 5 years, sample return from Pluto and the moons of the outer planets, unlimited ramjet flight in planetary atmospheres, etc. Much of the necessary technology for MITEE already exists as a result of previous nuclear rocket development programs. With some additional development, initial MITEE missions could begin in only 6 years.
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The Nuclear Europa Mobile Ocean (NEMO) mission would land on the surface of Europa, and deploy a small, lightweight melt probe powered by a compact nuclear reactor to melt down through the multi-kilometer ice sheet. After reaching the sub-surface ocean, a small nuclear Autonomous Underwater Vehicle (AUV) would deploy to explore the sub-ice ocean. After exploration and sample collection, the AUV would return to the probe and melt back to the lander. The lander would have replenished its H2 propellant by electrolysis of H2O ice, and then hop to a new site on Europa to repeat the probe/AUV process. After completing the mission, the NEMO spacecraft would return to Earth with its collected samples. The NEMO melt probe and AUV utilize enriched U-235 fuel and conventional water reactor technology. The lander utilizes a compact nuclear thermal propulsion (NTP) engine based on the cermet fuel and high-temperature H2 propellant. The compact nuclear reactors in both the NEMO melt probe and AUV drive a steam power cycle, generating over 10 kW(e) for use in each. Each nuclear reactor's operating lifetime is several years. With its high-mobility and long-duration mission, NEMO provides an ideal platform for life detection experiments.
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The Cassini mission to Saturn will start a second phase in the exploration of the Saturnian system, after the historical Voyager flybys of Saturn in 1980 and 1981. The Cassini primary mission is scheduled to be launched in October 1997 by the Titan IV/Centaur. Cassini uses four planetary gravity-assist flybys to gain the energy necessary to reach Saturn in July 2004. This arrival date at Saturn provides a unique opportunity for a flyby of Saturn's outer satellite Phoebe on the final approach. This paper provides an overview of the processes involved in the interplanetary trajectory design and analysis of the Cassini mission to Saturn.
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A thermally optimized in-space zero boil-off densified cryogen storage system model is developed. The Cryogenic System Design Tool is introduced and is used to model a spherical liquid hydrogen tank with active cooling and passive insulation systems. The model is used to investigate the effects of fluid storage temperature, multilayer insulation (MLI) thickness, and actively cooled shields on the overall storage system mass, cryocooler input power, and system volume. A validation of the Cryogenic System Design Tool is presented. The model predicts that a zero boil-off densified liquid hydrogen storage system minimizes the overall storage system mass and volume for nearly the same cooling input power as that of a normal boiling-point liquid hydrogen storage system.