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Showing papers on "Arcjet rocket published in 1991"


Journal ArticleDOI
TL;DR: In this article, the effect of an arcjet plume on the performance of satellite reflector antennas is studied, and the results show that as the electron density increases, the main beam and sidelobe level gradually degrade.
Abstract: The effect of an arcjet plume on the performance of satellite reflector antennas is studied. The arcjet plume is modeled as a weakly ionized plasma. The spatial permittivity distribution of the plume is approximated using the measured electron density profile and a cold plasma model. Geometrical optics is applied to determine the ray paths as well as the transmitted fields through the inhomogeneous plume. The ray optics results are compared against several exact solutions for scattering from inhomogeneous dielectrics, and good agreement is observed for sufficiently large scatterer size. The far-field antenna patterns of the reflector in the presence of the plume are calculated from the transmitted ray fields using a ray-tube integration scheme. For arcjet prototypes in the 1-kW class, the plume effect on the antenna performance is small. As the electron density increases, the main beam and sidelobe level gradually degrade. The main beam also tends to squint away from the plume region. >

29 citations


Proceedings ArticleDOI
24 Jun 1991

26 citations


Proceedings ArticleDOI
01 Jan 1991
TL;DR: In this paper, both CW and pulsed frequency-doubled dye lasers were used to demonstrate the ability to measure velocity with 10 percent accuracy at rates of 200,000 cm/s in a rarefied flow of Cu atoms seeded in He.
Abstract: Laboratory and field measurements were combined with a modeling effort to explore the feasibility of using atomic copper laser-induced fluorescence to measure velocity, turbulence, and temperature in arcjet flows. Both CW and pulsed frequency-doubled dye lasers were used to demonstrate the ability to measure velocity with 10 percent accuracy at rates of 200,000 cm/s in a rarefied flow of Cu atoms seeded in He. The pulsed laser established a threshold energy for power-broadening of the absorption line at 3.5 x 10 to the -8th J/sq cm. Field measurements at the NASA/JSC 10-MW arcjet facility demonstrated the ability to perform these measurements under actual test conditions. The use of this technique to measure freestream temperatures in the flow was examined for the 0.08/cm linewidth laser used in the NASA/JSC effort. Finally, single-shot turbulence measurements at the USAF/AEDC 35-MW H2 arcjet facility were measured with 4 percent accuracy using the laser/absorption line-overlap technique.

24 citations


Proceedings ArticleDOI
01 Jun 1991
TL;DR: In this paper, the UTSI arcjet model is used to compare the performance of a hydrogen and an ammonia arcjet in the same configuration and at the same electrical power, and the predicted specific impulse is 50 percent higher for the hydrogen propellant.
Abstract: The UTSI arcjet model is used to compare the performance of a hydrogen and an ammonia arcjet in the same configuration and at the same electrical power. The predicted specific impulse is 50 percent higher for the hydrogen propellant. Numerical studies made of the effect of transport properties on the performance of a hydrogen arcjet indicate that diffusive transport is very significant even in the supersonic part of the flow, and that relatively small changes in transport properties can have a significant effect on performance. These studies also show that nonequilibrium recombination chemistry can have a large effect on the transport coefficients. This leads to the conclusion that finite rate chemical calculations are necessary if accurate arcjet performance is to be calculated.

24 citations


Journal ArticleDOI
TL;DR: In this paper, the authors measured the flow velocity of atomic hydrogen in the plume of an ammonia-propelled arcjet thruster using laser-induced fluorescence (LIF).
Abstract: The flow velocity of atomic hydrogen in the plume of an ammonia-propelled arcjet thruster was measured using laser-induced fluorescence (LIF). The velocity was obtained by the Doppler shift of the absorption peak of the Balmer α spectral line. Measurements were made at the nozzle exit, varying the distance from the plume centerline. Results are presented for arcjet operating conditions 13, 20, and 27 kW with a mass flow of 0.31 g/s

19 citations


Proceedings ArticleDOI
01 Jun 1991
TL;DR: In this paper, a hydrogen arcjet was operated at power levels ranging from 5 to 30 kW with three different nozzle geometries, including constrictor diameter, length, and diverging exit angle.
Abstract: A hydrogen arcjet was operated at power levels ranging from 5 to 30 kW with three different nozzle geometries. Test results using all three nozzle geometries are reported and include variations of specific impulse with flow rate, and thrust with power. Geometric variables investigated included constrictor diameter, length, and diverging exit angle. The nozzle with a constrictor diameter of 1.78 mm and divergence angle of 20 deg was found to give the highest performance. A specific impulse of 1460 s was attained with this nozzle at a thrust efficiency of 29.8 percent. The best efficiency measured was 34.4 percent at a specific impulse of 1045 s. Post test examination of the cathode showed erosion after 28 hours of operation to be small, and limited to the conical tip where steady state arc attachment occurred. Each nozzle was tested to destruction.

19 citations


Proceedings ArticleDOI
01 Jun 1991
TL;DR: In this paper, a series of nozzles were operated in modular laboratory thrusters to examine the effects of geometric parameters such as constrictor diameter and nozzle divergence angle on the performance of a hydrogen arcjet.
Abstract: An experimental investigation was performed to evaluate hydrogen arcjet operating characteristics in the range of 1 to 4 kW. A series of nozzles were operated in modular laboratory thrusters to examine the effects of geometric parameters such as constrictor diameter and nozzle divergence angle. Each nozzle was tested over a range of current and mass flow rates to explore stability and performance. In the range of mass flow rates and power levels tested, specific impulse values between 650 and 1250 sec were obtained at efficiencies between 30 and 40 percent. The performance of the two larger half angle (20, 15 deg) nozzles was similar for each of the two constrictor diameters tested. The nozzles with the smallest half angle (10 deg) were difficult to operate. A restrike mode of operation was identified and described. Damage in the form of melting was observed in the constrictor region of all the nozzle inserts tested. Arcjet ignition was also difficult in many tests and a glow discharge mode that prevents starting was identified.

18 citations


Proceedings ArticleDOI
01 Jan 1991
TL;DR: In this article, the performance of water-cooled and radiation cooled arcjet thrusters operating on both 1:2 nitrogen/hydrogen mixtures at 1 to 2 kW and on pure hydrogen at 4 kW were compared.
Abstract: The performance of water-cooled and radiation cooled arcjet thrusters operating on both 1:2 nitrogen/hydrogen mixtures at 1 to 2 kW and on pure hydrogen at 1 to 4 kW are compared. To investigate the effects of test facility background pressure on performance, data were taken for both thruster operating on nitrogen/hydrogen mixtures at facility background pressures nominally at 0.20 Pa and 20 Pa. It is shown that increasing the background pressure decreased the thruster performance, and simple pressure area corrections alone could not account for observed degradation in performance.

16 citations


01 Jan 1991
TL;DR: In this paper, the mass benefits of using advanced chemical propulsion for apogee injection and NSSK functions or electric propulsion (hydrazine arcjets and xenon ion thrusters) for NSSk functions are documented.
Abstract: A model was developed and exercised to allow wet mass comparisons of three axis stabilized communication satellites delivered to geosynchronous transfer orbit. The mass benefits of using advanced chemical propulsion for apogee injection and north-south stationkeeping (NSSK) functions or electric propulsion (hydrazine arcjets and xenon ion thrusters) for NSSK functions are documented. A large derated ion thrusters is proposed which minimizes thruster lifetime concerns and qualification test times when compared to those of smaller ion thrusters planned for NSSK applications. The mass benefits, which depend on the spacecraft mass and mission duration, increase dramatically with arcjet specific impulse in the 500 to 600 s range, but are nearly constant for the derated ion thruster operated in the 2300 to 3000 s range. For a given mission, the mass benefits with an ion system are typically double those of the arcjet system; however, the total thrusting time with arcjets is less than 1/3 that with ion thrusters for the same thruster power. The mass benefits may permit increases in revenue producing payload or reduce launch costs by allowing a move to a smaller launch vehicle.

15 citations


Proceedings ArticleDOI
01 Jun 1991
TL;DR: In this paper, the axial velocity of atomic hydrogen in a 1-kW hydrogen-fueled arcjet thruster was measured using a narrow-band CW ring dye laser.
Abstract: A new diagnostic developed to measure the axial velocity of atomic hydrogen in a 1-kW hydrogen-fueled arcjet thruster is reported. The technique is based on laser-induced fluorescence of the Balmer alpha transition (656 nm) in atomic hydrogen. A narrow-band CW ring dye laser scans the excitation spectrum permitting accurate determination of the absorption line shape and position. The velocity is derived from the Doppler-shifted line position. A spatially resolved velocity profile is presented with a peak velocity of 12.8 km/s at the arcjet centerline near the exit plane.

14 citations


Proceedings ArticleDOI
01 Jan 1991
TL;DR: In this paper, an arcjet power electronics in the 100 to 400 W operating range were developed for future light-weight, low-power spacecraft, and the arcjet integration tests were performed, resulting in successful starts and stable arcjet operation at power levels as low as 240 W with simulated hydrazine propellants.
Abstract: In anticipation of the needs of future light-weight, low-power spacecraft, arcjet power electronics in the 100 to 400 W operating range were developed. Limited spacecraft power and thermal control capacity of these small spacecraft emphasized the need for high efficiency. Power topologies similar to those in the higher 2 kW and 5 to 30 kW power range were implemented, including a four transistor bridge switching circuit, current mode pulse-width modulated control, and an output current averaging inductor with an integral pulse generation winding. Reduction of switching transients was accomplished using a low inductance power distribution network, and no passive snubber circuits were necessary for power switch protection. Phase shift control of the power bridge was accomplished using an improved pulse width modulation to phase shift converter circuit. These features, along with conservative magnetics designs allowed power conversion efficiencies of greater than 92.5 percent to be achieved into resistive loads over the entire operating range of the converter. Electromagnetic compatibility requirements were not considered in this work, and control power for the converter was derived from AC mains. Addition of input filters and control power converters would result in an efficiency of on the order of 90 percent for a flight unit. Due to the developmental nature of arcjet systems at this power level, the exact nature of the thruster/power processor interface was not quantified. Output regulation and current ripple requirements of 1 and 20 percent respectively, as well as starting techniques, were derived from the characteristics of the 2 kW system but an open circuit voltage in excess of 175 V was specified. Arcjet integration tests were performed, resulting in successful starts and stable arcjet operation at power levels as low as 240 W with simulated hydrazine propellants.

01 Jan 1991
TL;DR: In the early 1970's, a substantial research effort was centered on the development of arcjets for space propulsion applications as discussed by the authors, and the majority of the work was at the 30 kW power level with some work at 1-2 kW.
Abstract: During the 1960's, a substantial research effort was centered on the development of arcjets for space propulsion applications. The majority of the work was at the 30 kW power level with some work at 1-2 kW. At the end of the research effort, the hydrogen arcjet had demonstrated over 700 hours of life in a continuous endurance test at 30 kW, at a specific impulse over 1000 s, and at an efficiency of 0.41. Another high power design demonstrated 500 h life with an efficiency of over 0.50 at the same specific impulse and power levels. At lower power levels, a life of 150 hours was demonstrated at 2 kW with an efficiency of 0.31 and a specific impulse of 935 s. Lack of a space power source hindered arcjet acceptance and research ceased. Over three decades after the first research began, renewed interest exists for hydrogen arcjets. The new approach includes concurrent development of the power processing technology with the arcjet thruster. Performance data were recently obtained over a power range of 0.3-30 kW. The 2 kW performance has been repeated; however, the present high power performance is lower than that obtained in the 1960's at 30 kW, and lifetimes of present thrusters have not yet been demonstrated. Laboratory power processing units have been developed and operated with hydrogen arcjets for the 0.1 kW to 5 kW power range. A 10 kW power processing unit is under development and has been operated at design power into a resistive load.

Proceedings ArticleDOI
01 Jul 1991
TL;DR: In this article, a 1 kW-class arcjet thruster was used to simulate fully decomposed hydrazine, and a 0.25 mm diameter hole was drilled into the diverging section of the tungsten thruster nozzle to provide optical access to the internal flow.
Abstract: Emission spectroscopy measurements were made of the plasma flow inside the nozzle of a 1 kW class arcjet thruster. The thruster propellant was a hydrogen-nitrogen mixture used to simulate fully decomposed hydrazine. The 0.25 mm diameter holes were drilled into the diverging section of the tungsten thruster nozzle to provide optical access to the internal flow. Atomic electron excitation, vibrational, and rotational temperatures were determined for the expanding plasma using relative line intensity techniques. The atomic excitation temperatures decreased from 18,000K at a location 3 mm downstream of the constrictor to 9,000K at a location 9 mm from the constrictor, while the molecular vibrational and rotational temperatures decreased from 6,500K to 2,500K and from 8,000K to 3,000K, respectively, between the same locations. The electron density measured using hydrogen H line Stark broadening decreased from about 10(exp 15) cm(-3) to about 2 times 10(exp 14) cm(-3) during the expansion. The results show that the plasma is highly nonequilibrium throughout the nozzle, with most relaxation times equal or exceeding the particle residence time.

Journal ArticleDOI
TL;DR: In this paper, both theoretical and experimental results are presented that demonstrate the effects of electrode geometry on the operation of the magnetoplasmadynamic (MPD) arcjet and describe the * "onset" phenomenon not as a single phenomenon but as two distinct phenomena.
Abstract: In this paper both theoretical and experimental results are presented that demonstrate the effects of electrode geometry on the operation of the magnetoplasmadynamic (MPD) arcjet and describe the * 'onset" phenomenon not as a single phenomenon but as two distinct phenomena—one in which thruster efficiency is drastically reduced due to an anode depletion mechanism and the other when thruster lifetime is decreased due to enhanced erosion Theory and data both show that the electrode current concentrations can be locally changed by varying the channel's interelectrode separation The experiment (conducted on a large radius annular geometry) shows a clear separation between an anode depletion description of onset (caused by the radial component of the thrust vector), indicated by the growth of a large anode voltage drop, and onset indicated by the appearance of unsteady large amplitude voltage oscillations which are attributed to convective motion of large concentrated anode arcs

Journal ArticleDOI
TL;DR: In this article, a magneto-plasmic dynamic (MPD) arcjet was used as both a heat source and an electric current source, and a numerical code was developed which could calculate the melting, the evaporation and the melt layer movement by the centrifugal force and the beam pressure.

Proceedings ArticleDOI
01 Sep 1991
TL;DR: In this paper, an overview of background and information on space propulsion systems on both the programmatic and technical levels is given, and feasibility experimental studies indicate that nondestructive evaluation tools such as ultrasonic, eddy current and x-ray may be successfully used to monitor the life limiting failure mechanisms of space propulsion system.
Abstract: An overview is given of background and information on space propulsion systems on both the programmatic and technical levels. Feasibility experimental studies indicate that nondestructive evaluation tools such as ultrasonic, eddy current and x-ray may be successfully used to monitor the life limiting failure mechanisms of space propulsion systems. Encouraging results were obtained for monitoring the life limiting failure mechanisms for three space propulsion systems; the degradation of tungsten arcjet and magnetoplasmadynamic electrodes; presence and thickness of spallable electrically conducting molybdenum films in ion thrusters; and the degradation of the catalyst in hydrazine thrusters.

01 Jan 1991
TL;DR: In this paper, the effect of the arcjet thruster plume on the performance of an onboard satellite reflector antenna was studied, and a project summary is presented along with sections on plasma and electromagnetic modeling.
Abstract: The objective was to study the effect of the arcjet thruster plume on the performance of an onboard satellite reflector antenna. A project summary is presented along with sections on plasma and electromagnetic modeling. The plasma modeling section includes the following topics: wave propagation; plasma analysis; plume electron density model; and the proposed experimental program. The section on electromagnetic modeling includes new developments in ray modeling and the validation of three dimensional ray results.

Proceedings ArticleDOI
01 Jun 1991
TL;DR: In this article, a series of cold and hot flow static pressure measurements have been made as a function of distance along the principal axis of a 30 kWe arcjet, and it was shown that anode arc attachment points directly coincided with the minimum static pressure points.
Abstract: A series of cold and hot flow static pressure measurements have been made as a function of distance along the principal axis of a 30 kWe arcjet. During these experiments, the background pressure was varied from atmospheric pressure to less than 1 Torr. The experimental arcjet used in these tests had the same constrictor and conical nozzle dimensions as the baseline MOD-1 ammonia arcjet developed at NASA-JPL, but used nitrogen as the propellant gas. Comparison of the measured static pressure profiles with the arc erosion patterns on the anode surface showed that anode arc attachment points directly coincided with the minimum static pressure points. The dual voltage modes commonly observed in 30 kWe class arcjet thrusters are also believed to be caused by the presence of two pressure minima in the arcjet, one at the constrictor entrance and the other in the expansion nozzle. The static pressure profiles also suggest that the sonic flow transition occurs at the entrance to the nozzle, indicating the existence of very thick boundary layers in the arcjet constrictor.


Proceedings ArticleDOI
01 Jun 1991
TL;DR: The throttling capabilities of a 30 kW class ammonia arcjet and its compatibility with a breadboard power conditioning unit (PCU) were tested in two series of tests.
Abstract: The throttling capabilities of a 30 kW class ammonia arcjet and its compatibility with a breadboard power conditioning unit (PCU) were tested in two series of tests. The first series was performed to determine the performance and operating characteristics of the arcjet and the PCU over a range of power levels and propellant flow rates. The power levels for the tests were nominally between 10 and 30 kW, with some operation below 10 kW at the lower flow rates. The ammonia flow rates varied between 0.16 and 0.35 g/s. The second series of tests was an extensive investigation of operation below 12 kW using three cathode spacings. The ammonia flow rates were between 0.115 and 0.335 g/s. Operation of the arcjet from 1.5 kW up to the 30 kW design point was demonstrated with the PCU.

Proceedings ArticleDOI
01 Jan 1991
TL;DR: In this article, the performance of a kW-class laboratory model arcjet thruster was characterized at three mass flow rates of a 2:1 mixture of hydrogen and nitrogen at power levels ranging from 1.0 to 2.0 kW.
Abstract: The first results of a program to expand the operational envelope of low-power arcjets to higher specific impulse and power levels are presented. The performance of a kW-class laboratory model arcjet thruster was characterized at three mass flow rates of a 2:1 mixture of hydrogen and nitrogen at power levels ranging from 1.0 to 2.0 kW. This same thruster was then operated for a total of 300 h at a specific impulse and power level of 550 s and 2.0 kW, respectively, in three continuous 100-h sessions. Thruster operation during the three test segments was stable, and no measurable performance degradation was observed during the test series. Substantial cathode erosion was observed during an inspection following the second 100-h test segment. Most notable was the migration of material from the center of the cathode tip to a ring around a large crater. The anode sustained no significant damage during the endurance test segments. Some difficulty was encountered during start-up after disassembly and inspection following the second 100-h test segment, which caused constrictor erosion. This resulted in a reduced flow restriction and arc chamber pressure, which in turn caused a reduction in the arc impedance.

Journal ArticleDOI
01 Sep 1991
TL;DR: In this paper, an earlier solution procedure is combined with an onset criterion to obtain the onset boundary curves for hydrogen and argon, and it is found that the engine-specific impulse at onset can be increased by increasing the propellant low-temperature electrical conductivity.
Abstract: The phenomenon of onset in MHD arcjets is studied. An earlier solution procedure is combined with an onset criterion to obtain the onset boundary curves for hydrogen and argon. The onset boundary curves are in qualitative agreement with experimental results. It is found that the engine-specific impulse at onset can be increased by increasing the propellant low-temperature electrical conductivity. For plasma temperatures in the range 8000-12000 K, it is predicted that a higher specific impulse at onset should be obtained for hydrogen than for argon.


Journal ArticleDOI
TL;DR: A review of the methods that are applicable to MPD (magnetoplasmadynamic) and arcjet thruster plasmas but that have not been used in space propulsion research can be found in this paper.
Abstract: Diagnostic techniques have recently been developed that permit the determination of the deviation from local thermal equilibrium (LTE) in subatmospheric electric arcs and plasma jets. A review is presented of the methods that are applicable to MPD (magnetoplasmadynamic) and arcjet thruster plasmas but that have not been used in space propulsion research. Appropriate plasma diagnostics can lead to increased thrust, better nozzle design, and improved modeling capabilities. These methods include nonintrusive techniques, and can determine the electron, Te, gas, Tg, and total excitation, Texa< temperatures, as well as the electron and atom densities, without using LTE or partial LTE assumptions. General relations for analysis and experimental results for argon constricted arcs, an arc in a rotating magnetic field, and plasma torch jets are presented. The methods discussed can also be applied to plasma mixtures.



Patent
23 Jan 1991

Proceedings ArticleDOI
01 Jun 1991
TL;DR: In this paper, the effect of swirl and viscosity on low Reynolds number flows is shown by examining integral parameters and flowfield details, and an implicit technique is used to solve the axisymmetric Thin Layer Naiver-Stokes equations.
Abstract: Viscous swirling flow through transonic converging-diverging nozzles (with and without centerbodies) is examined numerically. An implicit technique is used to solve the axisymmetric Thin Layer Naiver-Stokes equations. The effect of swirl and viscosity on low Reynolds number flows is shown by examining integral parameters and flowfield details.

01 Sep 1991
TL;DR: In this paper, the arcjet thruster was mounted 25.4 cm above the solar array, firing along its axis at a 20 degree cant angle, and the effect of having a constricted area exposed to the plume was to increase the current density.
Abstract: : High efficiency arcjet propulsion will be used in the near future for satellite orbit adjustment and eventually for orbit transfer. Testing is currently being conducted to explore spacecraft interface difficulties with this method of propulsion. This thesis looks at one aspect of this interface. Since most earth orbiting spacecraft use solar arrays for power generation, it is of interest to investigate how exposed, biased conducting surfaces will interact with the slightly ionized plume environment of the arcjet thruster. It was found that with the arcjet thruster mounted 25.4 cm above the solar array, firing along its axis at a 20 degree cant angle, electrical currents were indeed collected. The effect of having a constricted area exposed to the plume was to increase the current density. The electron densities at typical solar array distances were found to be 10 to the 10th to 10 to the 12th power/cu.m. An estimate of the total power lost for an array in this configuration showed that 0.05% of the overall power is lost due to collected currents.

01 Dec 1991
Abstract: A 1 kW electronic load was programmed to simulate the nonlinear i-v (volt-ampere) characteristics of an arcjet, both ignited and unignited. The simulator was tested and found to closely resemble an arcjet both for large transients and small perturbances up to about 40 kHz. No attempt was made to simulate the ignition process itself. The dynamic behavior of the arcjet (and the simulator) was shown to differ significantly from that of a resistor bank. Previous research led to the design and construction of a 1 kW arcjet power supply. A high voltage ignition circuit was added to this hardware, and tests on a 1 kW arcjet were performed at NASA-Lewis. All tests were successful and no ignition failures were observed. Circuit documentation and test results are included.