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Dive into the research topics where C.R. Foust is active.

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Featured researches published by C.R. Foust.


Review of Scientific Instruments | 1985

Repeating pneumatic hydrogen pellet injector for plasma fueling

S.K. Combs; S. L. Milora; C.R. Foust; C.A. Foster; D.D. Schuresko

A repeating pneumatic pellet injector has been developed for plasma fueling applications. The repetitive device extends pneumatic injector operation to steady state. The active mechanism consists of an extruder and a gun assembly that are cooled by flowing liquid‐helium refrigerant. The extruder provides a continuous supply of solid hydrogen to the gun assembly, where a reciprocating gun barrel forms and chambers cylindrical pellet from the extrusion; pellets are then accelerated with compressed hydrogen gas (pressures up to 125 bar) to velocities ≤1.9 km/s (1.6 km/s for deuterium pellets). The gun assembly design can accommodate different pellet sizes and barrel lengths. Steady‐state rates of 2 s−1 have been obtained with 2.1‐ , 3.4‐ , and 4.0‐mm‐diameter pellets. The present apparatus operates at higher firing rates in short bursts; for example, a rate of 6 s−1 for 2 s with the larger pellets. These pellet parameters are in the range applicable for fueling large present‐day fusion devices such as the To...


Review of Scientific Instruments | 1986

Fast‐opening magnetic valve for high‐pressure gas injection and applications to hydrogen pellet fueling systems

S. L. Milora; S.K. Combs; C.R. Foust

A fast, magnetically driven gas valve and its application to pneumatic‐based solid hydrogen pellet injectors are described. The valve, which is equipped with a polyimide stem tip (hard seal) and a 5‐mm‐diam orifice, can open against working pressures up to 140 bar (2000 psi). Other unique features of this design include temperature‐ and radiation‐resistant seals, a programmable output pressure pulse, and repetitive operation in excess of 20 Hz. A prototype valve has been used to propel frozen hydrogen isotope pellets to speeds of up to 1900 m/s.


Nuclear Fusion | 2007

Pellet fuelling and control of burning plasmas in ITER

L. R. Baylor; P.B. Parks; T.C. Jernigan; J. B. O. Caughman; S.K. Combs; C.R. Foust; W. A. Houlberg; S. Maruyama; D.A. Rasmussen

Pellet injection from the inner wall is planned for use in ITER as the primary core fuelling system since gas fuelling is expected to be highly inefficient in burning plasmas. Tests of the inner wall guide tube have shown that 5 mm pellets with up to 300 m s−1 speeds can survive intact and provide the necessary core fuelling rate. Modelling and extrapolation of the inner wall pellet injection experiments from present days smaller tokamaks leads to the prediction that this method will provide efficient core fuelling beyond the pedestal region. Using pellets for triggering of frequent small edge localized modes is an attractive additional benefit that the pellet injection system can provide. A description of the ITER pellet injection systems capabilities for fuelling and ELM triggering is presented and performance expectations and fusion power control aspects are discussed.


Nuclear Fusion | 2009

Pellet fuelling, ELM pacing and disruption mitigation technology development for ITER

L. R. Baylor; S.K. Combs; C.R. Foust; T.C. Jernigan; S. J. Meitner; P.B. Parks; J. B. O. Caughman; D. T. Fehling; S. Maruyama; A. L. Qualls; D.A. Rasmussen; C.E. Thomas

Plasma fuelling with pellet injection, pacing of edge localized modes (ELMs) by small frequent pellets and disruption mitigation with gas jets or injected solid material are some of the most important technological capabilities needed for successful operation of ITER. Tools are being developed at the Oak Ridge National Laboratory that can be employed on ITER to provide the necessary core pellet fuelling and the mitigation of ELMs and disruptions. Here we present progress on the development of the technology to provide reliable high throughput inner wall pellet fuelling, pellet ELM pacing with high frequency small pellets and disruption mitigation with gas jets and shattered pellets. Examples of how these tools can be employed on ITER are discussed.


Review of Scientific Instruments | 1989

Performance of a pneumatic hydrogen‐pellet injection system on the Joint European Torus

S.K. Combs; T.C. Jernigan; L. R. Baylor; S. L. Milora; C.R. Foust; P. Kupschus; M. Gadeberg; W. Bailey

A pneumatic‐based, hydrogen isotope pellet injector that was developed at the Oak Ridge National Laboratory (ORNL) has been used in recent plasma fueling experiments on the Joint European Torus (JET). The injector consists of three independent machine‐gun‐like mechanisms (nominal pellet sizes of 2.7, 4.0, and 6.0 mm in diameter) and features repetitive operation (1–5 Hz) for quasi‐steady‐state conditions (>10 s). An extensive set of injector diagnostics permits evaluation of parameters for each pellet shot, including speed, mass, and integrity. Pellet speeds range from 1.0 to 1.5 km/s. Over 3700 pellets have been fired with the equipment at JET, with about 1500 pellets shot for plasma fueling experiments. In recent experiments, the system performance has been outstanding, including excellent reproducibility in pellet speed and mass, and a reliability of >98% in delivery of pellets to the plasma.


Review of Scientific Instruments | 1986

Simple pipe gun for hydrogen pellet injection

S.K. Combs; S. L. Milora; C.R. Foust

A new single‐shot hydrogen pellet injector based on a simple ‘‘pipe gun’’ design is described. In the cryogenic gun block, the 4‐mm‐diam (nominal) pellet is frozen in situ directly from the gaseous hydrogen isotope and then accelerated in the gun barrel with a burst of high‐pressure (≤130‐bar) hydrogen gas to speeds of up to 1680 m/s.


Review of Scientific Instruments | 1987

Eight‐shot pneumatic pellet injection system for the tokamak fusion test reactor

S.K. Combs; S. L. Milora; C.R. Foust; L. R. Baylor; G. C. Barber; R. D. Burris; P.W. Fisher; C.A. Foster; R.V. Lunsford; G. L. Schmidt; D.D. Schuresko; T. Senko; R. C. Shanlever; W. D. Shipley; D. O. Sparks; K. A. Stewart; R.B. Wysor

An eight‐shot pneumatic pellet injection system has been developed for plasma fueling of the tokamak fusion test reactor (TFTR). The active cryogenic mechanisms consist of a solid hydrogen extruder and a rotating pellet wheel that are cooled by flowing liquid‐helium refrigerant. The extruder provides solid hydrogen for stepwise loading of eight holes located circumferentially around the pellet wheel. This design allows for three different pellet diameters: 3.0 mm (three pellets), 3.5 mm (three pellets), and 4.0 mm (two pellets) in the present configuration. Each of the eight pellets can be shot independently. Deuterium pellets are accelerated in 1.0‐m‐long gun barrels with compressed hydrogen gas (at pressures from 70 to 105 bar) to velocities in the range 1.0–1.5 km/s. The pellets are transported to the plasma in an injection line that incorporates two stages of guide tubes with intermediate vacuum pumping stations. A remote, stand‐alone control and data‐acquisition system is used for injector and vacuum...


Nuclear Fusion | 2009

Improved-confinement plasmas at high temperature and high beta in the MST RFP

B.E. Chapman; Joon-Wook Ahn; A. F. Almagri; J. K. Anderson; F. Bonomo; D. L. Brower; D. R. Burke; K.J. Caspary; D.J. Clayton; S.K. Combs; W.A. Cox; D. Craig; B.H. Deng; D.J. Den Hartog; W. X. Ding; F. Ebrahimi; D.A. Ennis; G. Fiksel; Cary Forest; C.R. Foust; P. Franz; S. Gangadhara; J.A. Goetz; M. C. Kaufman; J.G. Kulpin; A. V. Kuritsyn; Richard Magee; M. C. Miller; V.V. Mirnov; Paul Nonn

We have increased substantially the electron and ion temperatures, the electron density, and the total beta in plasmas with improved energy confinement in the Madison Symmetric Torus (MST). The improved confinement is achieved with a well-established current profile control technique for reduction of magnetic tearing and reconnection. A sustained ion temperature >1?keV is achieved with intensified reconnection-based ion heating followed immediately by current profile control. In the same plasmas, the electron temperature reaches 2?keV, and the electron thermal diffusivity drops to about 2?m2?s?1. The global energy confinement time is 12?ms. This and the reported temperatures are the largest values yet achieved in the reversed-field pinch (RFP). These results were attained at a density ~1019?m?3. By combining pellet injection with current profile control, the density has been quadrupled, and total beta has nearly doubled to a record value of about 26%. The Mercier criterion is exceeded in the plasma core, and both pressure-driven interchange and pressure-driven tearing modes are calculated to be linearly unstable, yet energy confinement is still improved. Transient momentum injection with biased probes reveals that global momentum transport is reduced with current profile control. Magnetic reconnection events drive rapid momentum transport related to large Maxwell and Reynolds stresses. Ion heating during reconnection events occurs globally, locally, or not at all, depending on which tearing modes are involved in the reconnection. To potentially augment inductive current profile control, we are conducting initial tests of current drive with lower-hybrid and electron-Bernstein waves.


Fusion Science and Technology | 2009

Development of a Twin-Screw D 2 Extruder for the ITER Pellet Injection System

S. J. Meitner; L. R. Baylor; Juan J. Carbajo; S.K. Combs; D. T. Fehling; C.R. Foust; Marshall T McFee; James M McGill; D.A. Rasmussen; R G Sitterson; D. O. Sparks; A L Qualls

A twin-screw extruder for the ITER pellet injection system is under development at the Oak Ridge National Laboratory. The extruder will provide a stream of solid hydrogen isotopes to a secondary section, where pellets are cut and accelerated with single-stage gas gun into the plasma. A one-fifth ITER scale prototype extruder has been built to produce a continuous solid deuterium extrusion. Deuterium gas is precooled and liquefied before being introduced into the extruder. The precooler consists of a copper vessel containing liquid nitrogen surrounded by a deuterium gas filled copper coil. The liquefier is comprised of a copper cylinder connected to a Cryomech AL330 cryocooler, which is surrounded by a copper coil that the precooled deuterium flows through. The lower extruder barrel is connected to a Cryomech GB-37 cryocooler to solidify the deuterium (at 15 K) before it is forced through the extruder nozzle. A viewport located below the extruder nozzle provides a direct view of the extrusion. A camera is used to document the extrusion quality and duration. A data acquisition system records the extruder temperatures, torque, and speed, upstream, and downstream pressures. This paper will describe the prototype twin-screw extruder and initial extrusion results.


Review of Scientific Instruments | 1995

Small-bore (1. 8-mm), high-firing-rate (10-Hz) version of a repeating pneumatic hydrogen pellet injector

S.K. Combs; C.R. Foust; S. L. Milora

Repeating pneumatic pellet injectors developed at the Oak Ridge National Laboratory (ORNL) were used for plasma fueling experiments on the Tokamak Fusion Test Reactor (TFTR) and the Joint European Torus (JET). For plasma fueling on the DIII–D tokamak, a small‐bore (1.8‐mm) injector has been developed and tested in the laboratory at pellet rates of up to 10 Hz and speeds of ≤1 km/s (for pulse lengths of up to 15 s). This performance represents the smallest pellet size and highest repetition rate demonstrated with an ORNL repeating pneumatic pellet injector. The design has been incorporated in the three‐barrel injector that was previously used on JET; the injection system, equipped with nominal pellet sizes of 1.8‐, 2.7‐, and 4.0‐mm diameter, has been installed on DIII–D and will be used in future plasma fueling experiments.

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S.K. Combs

Oak Ridge National Laboratory

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L. R. Baylor

Oak Ridge National Laboratory

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D. T. Fehling

Oak Ridge National Laboratory

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S. J. Meitner

Oak Ridge National Laboratory

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S. L. Milora

Oak Ridge National Laboratory

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J. B. O. Caughman

Oak Ridge National Laboratory

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T.C. Jernigan

Oak Ridge National Laboratory

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D.A. Rasmussen

Oak Ridge National Laboratory

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M. J. Gouge

Oak Ridge National Laboratory

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P.W. Fisher

Oak Ridge National Laboratory

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