M. P. Petrov
Princeton Plasma Physics Laboratory
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by M. P. Petrov.
Nuclear Fusion | 1995
M. P. Petrov; R.V. Budny; H. Duong; R.K. Fisher; N. N. Gorelenkov; J. McChesney; D.K. Mansfield; S. S. Medley; P.B. Parks; M.H. Redi; A. L. Roquemore
Results from recent DT experiments on TFTR to measure the energy distribution and radial density profile of fast confined alphas with the use of Li pellets and neutral particle analysis are presented. When a pellet is injected into the plasma, a toroidally extended ablation cloud is formed. A small fraction of the fusion alphas incident on the cloud is converted to helium neutrals as a result of electron capture processes. The escaping energetic helium neutrals are analysed and detected by the neutral particle analyser. Radially resolved energy spectra of trapped confined alphas in 0.5-2 MeV range and radial alpha density profiles are presented in this paper. The experimental data are compared with modelling results obtained with the TRANSP Monte Carlo code and with a specially developed Fokker-Planck post-processor (FPP) that uses the alpha source distribution produced by TRANSP. Comparison of the experimental data with TRANSP and FPP shows that the alphas in the plasma core of sawtooth free discharges in TFTR are well confined and slow down classically. The energy and radial profiles distributions outside the plasma core show the influence of stochastic ripple losses on alphas. Measurements for sawtoothing plasmas show a significant outward radial transport of trapped alphas
Review of Scientific Instruments | 1996
S. S. Medley; D.K. Mansfield; A.L. Roquemore; R.K. Fisher; H. Duong; J. McChesney; P.B. Parks; M. P. Petrov; A. V. Khudoleev; N. N. Gorelenkov
Radially resolved energy and density distributions of the confined α particles in D–T experiments on the Tokamak Fusion Test Reactor (TFTR) are being measured with the pellet charge exchange (PCX) diagnostic. Other energetic ion species can be detected as well, such as tritons produced in D–D plasmas and H, He3, or tritium rf‐driven minority ion tails. The ablation cloud formed by injected low‐Z impurity pellets provides the neutralization target for this active charge exchange technique. Because the cloud neutralization efficiency is uncertain, the PCX diagnostic is not absolutely calibrated so only relative density profiles are obtained. A mass and energy resolving E∥B neutral particle analyzer (NPA) is used which has eight energy channels covering the energy range of 0.3–3.7 MeV for α particles with energy resolution ranging from 5.8% to 11.3% and a spatial resolution of ∼5 cm. The PCX diagnostic views deeply trapped ions in a narrow pitch angle range around a mean value of v∥/v=−0.048±10−3. For D–T op...
Physics of Plasmas | 1996
R. Majeski; J. H. Rogers; S. H. Batha; A. Bers; R.V. Budny; D. S. Darrow; H.H. Duong; R. K. Fisher; C. B. Forest; E. D. Fredrickson; B. Grek; K. W. Hill; J. C. Hosea; D. Ignat; B. LeBlanc; F. M. Levinton; S.S. Medley; M. Murakami; M. P. Petrov; C.K. Phillips; A. Ram; A. T. Ramsey; G. Schilling; G. Taylor; J. R. Wilson; M. C. Zarnstorff
Recent experiments in the ion cyclotron range of frequencies (ICRF) in the Tokamak Fusion Test Reactor [Fusion Technol. 21, 13 (1992)] are discussed. These experiments include mode conversion heating and current drive, fast wave current drive, and heating of low (L)‐ mode deuterium–tritium (D–T) plasmas in both the hydrogen minority and second harmonic tritium regimes. In mode conversion heating, a central electron temperature of 10 keV was attained with 3.3 MW of radio‐frequency power. In mode conversion current drive experiments, up to 130 kA of current was noninductively driven, on and off axis, and the current profiles were modified. Fast wave current drive experiments have produced 70–80 kA of noninductively driven current. Heating of L‐mode deuterium and D–T plasmas by hydrogen minority ICRF has been compared. Finally, heating of L‐mode D–T plasmas at the second harmonic of the tritium cyclotron frequency has been demonstrated.
Nuclear Fusion | 2000
C. K. Phillips; M.G. Bell; R.E. Bell; S. Bernabei; M. Bettenhausen; C.E. Bush; D. Clark; D. S. Darrow; E.D. Fredrickson; G. R. Hanson; J. Hosea; Benoit P. Leblanc; R. Majeski; S. S. Medley; R. Nazikian; M. Ono; H. Park; M. P. Petrov; J. H. Rogers; G. Schilling; C.H. Skinner; D.N. Smithe; E. J. Synakowski; Gary Taylor; J. R. Wilson
In fast wave to ion Bernstein wave mode conversion experiments in DT supershot plasmas, localized efficient ion heating rather than electron heating was observed, which was due to Doppler broadened tritium cyclotron resonance overlap into the mode conversion region. The ion temperature heat pulse associated with RF power modulation in this regime could provide a diagnostic tool for measuring the local ion thermal conductivity in various confinement regimes. In direct launch ion Bernstein wave heating experiments, core power coupling was limited by the excitation of parasitic edge modes. However, a sheared poloidal flow was observed that is consistent in both magnitude and direction with theoretical models based on RF driven Reynolds stress. With the modest power coupled to the core (~360 kW), the magnitude of the shear in the observed flow was estimated to be a factor of 3-4 too low to trigger transport barrier formation through localized shear suppression of turbulence.
Physics of Plasmas | 1999
M. P. Petrov; R.E. Bell; R.V. Budny; N.N. Gorelenkov; S. S. Medley; R. B. White; S. J. Zweben
This paper presents studies of the H+ minority ions driven by Ion Cyclotron Radio Frequency (ICRF) heating in the Tokamak Fusion Test Reactor (TFTR) [R. J. Hawryluk et al., Phys. Plasmas 5, 1577 (1998)] deuterium plasmas using primarily passive H° flux detection in the energy range of 0.2–1.0 MeV. The measured passive H+ energy spectra are compared with active (Li pellet charge exchange) results. It is shown that in the passive mode the main donors for the neutralization of H+ ions in this energy range are C5+ ions. The measured effective H+ tail temperatures range from 0.15 MeV at an ICRF power of 2 MW to 0.35 MeV at 6 MW. Radial redistribution of ICRF-driven H+ ions was detected when giant sawtooth crashes occurred during the ICRF heating. The redistribution affected ions with energy below 0.7–0.8 MeV. The sawtooth crashes displaces H+ ions outward along the plasma major radius into the stochastic ripple diffusion domain where those ions are lost in ∼10 msec. These observations are consistent with the m...
Review of Scientific Instruments | 2003
S. S. Medley; R.E. Bell; M. P. Petrov; A.L. Roquemore; E. V. Suvorkin
The neutral particle analyzer (NPA) diagnostic on the National Spherical Torus Experiment (NSTX) utilizes a PPPL-designed E∥B spectrometer which measures the energy spectra of minority H and bulk D species simultaneously with 39 energy channels per mass species and a time resolution of 1 ms. The calibrated energy range is E=0.5–150u2009keV and the energy resolution varies from ΔE/E=3%–7% over the surface of the microchannel plate detector. The NPA measures thermal Maxwellian ion spectra to obtain line integrated ion temperatures, Ti. For line integral electron densities below neL∼3.5×1019u2009m−2, good agreement is observed between the line integrated NPA Ti and the central Ti(0) measured by the spatially localized charge exchange recombination spectroscopy (CHERS) diagnostic. However, with increasingly higher neL the NPA Ti falls below the central Ti(0) measured by CHERS because the charge exchange neutral emissivity weights the line integrated NPA measurement outboard of the plasma core. An analytic neutral ana...
Physics of Plasmas | 1999
M. H. Redi; S. H. Batha; R.V. Budny; D. S. Darrow; F. M. Levinton; D. McCune; S. S. Medley; M. P. Petrov; S. von Goeler; R. B. White; M. C. Zarnstorff; S. J. Zweben; Tftr Team
Neoclassical simulations of alpha particle density profiles in high fusion power plasmas on the Tokamak Fusion Test Reactor [Phys. Plasmas 5, 1577 (1998)] are found to be in good agreement with measurements of the alpha distribution function made with a sensitive active neutral particle diagnostic. The calculations are carried out in Hamiltonian magnetic coordinates with a fast, particle-following Monte Carlo code which includes the neoclassical transport processes, a recent first-principles model for stochastic ripple loss and collisional effects. New calculations show that monotonic shear alpha particles are virtually unaffected by toroidal field ripple. The calculations show that in reversed shear the confinement domain is not empty for trapped alphas at birth and allow an estimate of the actual alpha particle densities measured with the pellet charge exchange diagnostic.
Nuclear Fusion | 1999
B. C. Stratton; R. V. Budny; D. S. Darrow; R.K. Fisher; E.D. Fredrickson; G. Y. Fu; S. S. Medley; R. Nazikian; M. P. Petrov; M. H. Redi; E. Ruskov; Gary Taylor; R. B. White; Stewart J. Zweben
The article reviews the physics of fusion alpha particles and energetic neutral beam ions studied in the final phase of TFTR operation, with an emphasis on observations in reversed magnetic shear (RS) and enhanced reversed shear (ERS) DT plasmas. Energy resolved measurements of the radial profiles of confined, trapped alphas in RS plasmas exhibit reduced core alpha density with increasing alpha energy, in contrast to plasmas with normal monotonic shear. The measured profiles are consistent with predictions of increased alpha loss due to stochastic ripple diffusion and increased first orbit loss in RS plasmas. In experiments in which a short tritium beam pulse is injected into a deuterium RS plasma, the measured DT neutron emission is lower than standard predictions assuming first orbit loss and stochastic ripple diffusion of the beam ions. A microwave reflectometer measured the spatial localization of low toroidal mode number (n), alpha driven toroidal Alfven eigenmodes (TAEs) in DT RS discharges. Although the observed ballooning character of the n = 4 mode is consistent with predictions of a kinetic MHD stability code, the observed antiballooning nature of the n = 2 mode is not. Furthermore, the modelling does not show the observed strong dependence of mode frequency on n. These alpha driven TAEs do not cause measurable alpha loss in TFTR. Other Alfven frequency modes with n = 2-4 seen in both DT and DD ERS and RS discharges are localized to the weak magnetic shear region near qmin. In 10-20% of DT discharges, normal low n MHD activity causes alpha loss at levels above the first orbit loss rate.
Review of Scientific Instruments | 1997
R.K. Fisher; H. Duong; J. McChesney; P.B. Parks; S. S. Medley; R. V. Budny; D.K. Mansfield; A.L. Roquemore; M. P. Petrov; N. N. Gorelenkov
Confinement of alpha particles is essential for fusion ignition and alpha physics studies are a major goal of the TFTR, JET, and ITER DT experiments, but alpha measurements remain one of the most challenging plasma diagnostic tasks. The pellet charge exchange (PCX) diagnostic has successfully measured the radial density profile and energy distribution of fast (0.5–3.5 MeV) confined alpha particles in TFTR. This article describes the diagnostic capabilities of PCX demonstrated on TFTR and discusses the prospects for applying this technique to ITER. Major issues on ITER include the pellet’s perturbation to the plasma and obtaining satisfactory pellet penetration into the plasma.
Archive | 1996
L. C. Johnson; Cris W. Barnes; R.E. Bell; M. Bitter; R.V. Budny; C.E. Bush; D. S. Darrow; Hau Hoang Duong; Philip C. Efthimion; R. K. Fisher; R. J. Fonck; H. W. Herrmann; D. L. Jassby; A. V. Krasilnikov; G. R. McKee; S. S. Medley; M. Osakabe; M. P. Petrov; A.L. Roquemore; M. Sasao; S Sesnic; B. C. Stratton; E. J. Synakowski; S. von Goeler; S. J. Zweben
Since the introduction of tritium into the Tokamak Fusion Test Reactor (TFTR) in December 1993, more than 400 D-T plasmas have been produced, with a total fusion energy of over 900 MJ. Fusion power production in D-T supershots is routinely in the 5–10 MW range, within a factor of ~ 200 of that expected in ITER. Neutron flux at the first wall of TFTR has reached about 10% of values projected for ITER, and central fusion power densities are already at ITER levels. Therefore, experience gained in fusion product measurements during the TFTR D-T experiments is directly relevant to the design of diagnostic systems for ITER.