J. Sinnis
Princeton University
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by J. Sinnis.
Journal of Nuclear Materials | 1987
H.F. Dylla; Team Tftr Team; M.G. Bell; W. Blanchard; P. P. Boody; N. Bretz; R.V. Budny; C.E. Bush; Joseph L. Cecchi; S.A. Cohen; S. K. Combs; S. Davis; B.L. Doyle; P.C. Efthimion; A. C. England; H.P. Eubank; R.J. Fonck; E. D. Fredrickson; L R Grisham; R.J. Goldston; B. Grek; R. Groebner; R.J. Hawryluk; D.B. Heifetz; H. W. Hendel; K. W. Hill; S. Hiroe; R. Hulse; D. Johnson; L. C. Johnson
This paper presents a summary of plasma-material interactions which influence the operation of TFTR with high current (≤ 2.2 MA) ohmically heated, and high-power (∼ 10 MW) neutral-beam heated plasmas. The conditioning procedures which are applied routinely to the first-wall hardware are reviewed. Fueling characteristics during gas, pellet, and neutral-beam fueling are described. Recycling coefficients near unity are observed for most gas fueled discharges. Gas fueled discharges after helium discharge conditioning of the toroidal bumper limiter, and discharges fueled by neutral beams and pellets, show R<1. In the vicinity of the gas fueled density limit (at ne = 5–6 × 1019 m−3) values of Zeff are ≦1.5. Increases in Zeff of ≦1 have been observed with neutral beam heating of 10 MW. The primary low Z impurity is carbon with concentrations decreasing from ∼10% to <1% with increasing ne. Oxygen densities tend to increase with ne, and at the ohmic plasma density limit oxygen and carbon concentrations are comparable. Chromium getter experiments and He2+/D+ plasma comparisons indicate that the limiter is the primary source of carbon and that the vessel wall is a significant source of the oxygen impurity. Metallic impurities, consisting of the vacuum vessel metals (Ni, Fe, Cr) have significant (∼10−4 ne) concentrations only at low plasma densities (ne <1019 m−3). The primary source of metallic impurities is most likely ion sputtering from metals deposited on the carbon limiter surface.
Journal of Nuclear Materials | 1984
Joseph L. Cecchi; M.G. Bell; M. Bitter; W. Blanchard; N. Bretz; C.E. Bush; S.A. Cohen; J. Coonrod; S. Davis; D. Dimock; B.L. Doyle; H.F. Dylla; P.C. Efthimion; R.J. Fonck; R.J. Goldston; S. von Goeler; B. Grek; D.J. Grove; R.J. Hawryluk; D.B. Heifetz; H. W. Hendel; K. W. Hill; R. Hulse; J. Isaacson; D. Johnson; L. C. Johnson; R. Kaita; S. Kaye; S.J. Kilpatrick; J. Kiraly
Abstract During the recent ohmic heating experiments on TFTR, the movable limiter array, preliminary inner bumper limiter, and prototype ZrAl alloy bulk getter surface pumping system were brought into operation. This paper summarizes the operational experience and plasma characteristics obtained with these components. The near-term upgrades of these systems are also discussed.
Plasma Physics and Controlled Fusion | 1987
M. Bitter; V. Arunasalam; M.G. Bell; S Bosch; N. Bretz; R.V. Budny; C.E. Bush; D. Dimock; H.F. Dylla; P.C. Efthimion; R.J. Fonck; E. D. Fredrickson; H. P. Furth; G. Gammel; R.J. Goldston; B. Grek; L R Grisham; G. W. Hammett; Ken-ichi Hattori; R.J. Hawryluk; H. W. Hendel; K. W. Hill; E. Hinnov; T Hirayama; R B Howell; R. Hulse; H. Hsuan; K P Jaehnig; D.L. Jassby; F. Jobes
New long-pulse ion sources have been employed to extend the neutral beam pulse on TFTR from 0.5 sec to 2.0 sec. This made it possible to study the long-term evolution of supershots at constant current and to perform experiments in which the plasma current was ramped up during the heating pulse. Experiments were conducted with co and counter injection as well as with nearly balanced injection of deuterium beams up to a total power of 20 MW. The best results, i.e., central ion temperatures Tio > 25 keV and neo τE Tio values of 3 × 1020 keV sec m-3, were obtained with nearly balanced injection. The central toroidal plasma rotation velocity scales in a linear-offset fashion with beam power and density. The scaling of the inferred global momentum confinement time with plasma parameters is inconsistent with the predictions of the neoclassical theory of gyroviscous damping. An interesting plasma regime with properties similar to the H-mode has been observed for limiter plasmas with edge qa just above 3 and 2.5.
Plasma Physics and Controlled Fusion | 1988
K. McGuire; V Arunsalam; Cris W. Barnes; M.G. Bell; M. Bitter; H.S. Bosch; N. Bretz; R.V. Budny; C.E. Bush; A. Cavallo; P. Colestock; S. Davis; D. Dimock; H.F. Dylla; P.C. Efthimion; A Ehrhardt; R.J. Fonck; E. D. Fredrickson; R.J. Goldston; G. J. Greene; B. Grek; L.R. Grisham; G. W. Hammett; R.J. Hawryluk; H. W. Hendel; K. W. Hill; E. Hinnov; R.B. Howell; R. Hulse; H. Hsuan
During the 1987 run, TFTR reached record values of QDD, neutron source strength, and Ti(0). Good confinement together with intense auxiliary heating has resulted in a plasma pressure greater than 3*105 Pascals on axis, which is at the ballooning stability boundary. At the same time improved diagnostics, especially ion temperature profile measurements, have led to increased understanding of tokamak confinement physics. Ion temperature profiles are much more peaked than previously thought, implying that ion thermal diffusivity, even in high ion temperature supershot plasmas, is greater than electron thermal diffusivity. Based on studies of the effect of beam orientation on plasma performance, one of the four neutral beamlines has been re-oriented from injecting co-parallel to counter parallel, which will increase the available balanced neutral injection power from 14 MW to 27 MW. With this increase in balanced beam power, and the addition of 7 MW of ICRF power it is planned to increase the present equivalant QDT of 0.25 to close to break-even conditions in the coming run.
Plasma Physics and Controlled Fusion | 1986
M.G. Bell; V Arunsalam; M. Bitter; W. Blanchard; F Boody; N. Bretz; R.V. Budny; C.E. Bush; J D Callen; Joseph L. Cecchi; S.A. Cohen; R J Colchin; S. K. Combs; J. Coonrod; S. Davis; D. Dimock; H.F. Dylla; P.C. Efthimion; A. C. England; H P Eubank; R.J. Fonck; E. D. Fredrickson; L R Grisham; R.J. Goldston; B. Grek; R.J. Hawryluk; W. W. Heidbrink; H. W. Hendel; K. W. Hill; E. Hinnov
The characteristics of plasma operation on the axisymmetric inner toroidal limiter in TFTR are described. After conditioning, plasmas with low metal content and low zeff are obtained with this limiter. There is no substantial increase in zeff with total input power during neutral beam injection. Compared to operation on the outer blade limiter, additional gas is required to fuel plasmas on the inner limiter. Injection of D pellets increased the plasma density substantially and produced energy confinement times up to 0.5 s in ohmically heated plasmas. The four neutral beam lines have injected up to 13.5 MW total power into the plasma for 0.5 s with up to 90 kV accelerating voltage. The scaling of the plasma stored energy was studied as a function of the input power, plasma current and plasma density. In the range 1.4 to 2.2 MA, the overall and incremental confinement times for both the total and thermal stored energies increase with plasma current at fixed density. There appears to be a weak negative scaling of the total stored energy with density at high injection power.
Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms | 1987
L.R. Grisham; M.G. Bell; W. Blanchard; F Boody; N. Bretz; R.V. Budny; C.E. Bush; Joseph L. Cecchi; S.A. Cohen; S. Davis; H.F. Dylla; P.C. Efthimion; A. C. England; H.P. Eubank; R.J. Fonck; E. D. Fredrickson; R.J. Goldston; B. Grek; R. Groebner; R.J. Hawryluk; D.B. Heifetz; H. W. Hendel; K. W. Hill; R. Hulse; D. Johnson; L. C. Johnson; S.J. Kilpatrick; P. H. LaMarche; R. Little; D. Manos
The neutral beam injection experiment on TFTR has now been underway for over two years, during which time we have injected as much as about 20 MW of beam power at energies up to 110 keV. We have obtained qualitative evidence of direct current drive by the injected beam ions. Recently we have produced plasmas in which the energy confinement time, βp, neutron emission, stored energy (both total and electron), and ion temperature exhibit a pronounced enhancement over previous behavior. Under these conditions we have obtained preliminary indications that significant bootstrap current is being driven. Operation will continue with new sources with which we should be able to increase the beam pulse length fourfold.
Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms | 1989
L.R. Grisham; V Arunsalam; Cris W. Barnes; M.G. Bell; M. Bitter; H.S. Bosch; N. Bretz; C.E. Bush; P. Colestock; S. Davis; D. Dimock; H.F. Dylla; P.C. Efthimion; R.J. Fonck; E. D. Fredrickson; R.J. Goldston; B. Grek; G. W. Hammett; R.J. Hawryluk; H. W. Hendel; K. W. Hill; E. Hinnov; R.B. Howell; R. Hulse; H. Hsuan; K P Jaehnig; D.L. Jassby; F. Jobes; D. Johnson; L. C. Johnson
Abstract The principal heating system for the Tokamak Fusion Test Reactor (TFTR) consists of four beamlines to inject beams of neutral deuterium into the tokamak plasma. We have recently injected beams at total powers up to about 30 MW, and we have achieved ion temperatures in the plasma core of 30 keV and more.
Philosophical Transactions of the Royal Society A | 1987
R.J. Hawryluk; V. Arunasalam; J. D. Bell; M.G. Bell; M. Bitter; W. Blanchard; F Boody; N. Bretz; R.V. Budny; C.E. Bush; J D Callen; Joseph L. Cecchi; Sydney Cohen; R J Colchin; S. K. Combs; J. Coonrod; S. Davis; D. Dimock; H.F. Dylla; P.C. Efthimion; L. C. Emerson; A. C. England; H.P. Eubank; R.J. Fonck; E. D. Fredrickson; R.J. Goldston; L R Grisham; B. Grek; R. Groebner; H. W. Hendel
Recent experiments on TFTR have extended the operating regime of TFTR in both ohmic- and neutral-beam -heated discharges. The TFTR tokamak has reached its original machine-design specifications (Ip = 2.5 MA and BT = 5.2 T). Initial neutral-beam -heating experiments used up to 6.3 MW of deuterium beams. With the recent installation of two additional beamlines, the power has been increased up to 11 MW. A deuterium pellet injector was used to increase the central density to 2.5 x 1020 m-3 in high-current discharges. At the opposite extreme, by operating at low plasm a current (Ip ~ 0.8 MA) and low density (ne~ 1 x 1019 m-3), high ion temperatures (9 + 2 keV) and rotation speeds (7 x 105 m s-1) have been achieved during injection. In addition, plasma-compression experiments have demonstrated acceleration of beam ions from 82 to 150 keV, in accord with expectations. The wide operating range of TFTR, together with an extensive set of diagnostics and a flexible control system, has facilitated transport and scaling studies of both ohmic- and neutral-beam -heated discharges. The result of these confinement studies are presented.
Physical Review Letters | 1981
M. Yamada; H. P. Furth; W. Hsu; A. Janos; S. Jardin; M. Okabayashi; J. Sinnis; T.H. Stix; K. Yamazaki
Plasma Physics and Controlled Fusion | 1986
M. Murakami; V. Arunasalam; J. D. Bell; M.G. Bell; M. Bitter; W. Blanchard; F Boody; N. Bretz; R. V. Budny; C.E. Bush; J D Callen; J. L. Cecchi; S Cohen; R J Colchin; S. K. Combs; J. Coonrod; S. Davis; D. Dimock; H. F. Dylla; P.C. Efthimion; L. C. Emerson; A. C. England; H P Eubank; R.J. Fonck; E. Fredrickson; H. P. Furth; L R Grisham; S. von Goeler; R.J. Goldston; B. Grek