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Dive into the research topics where Erik Granstedt is active.

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Featured researches published by Erik Granstedt.


Review of Scientific Instruments | 2010

High speed digital holography for density and fluctuation measurements (invited)

Clarence E. Thomas; L. R. Baylor; S.K. Combs; S. J. Meitner; D.A. Rasmussen; Erik Granstedt; R. Majeski; R. Kaita

The state of the art in electro-optics has advanced to the point where digital holographic acquisition of wavefronts is now possible. Holographic wavefront acquisition provides the phase of the wavefront at every measurement point. This can be done with accuracy on the order of a thousandth of a wavelength, given that there is sufficient care in the design of the system. At wave frequencies which are much greater than the plasma frequency, the plasma index of refraction is linearly proportional to the electron density and wavelength, and the measurement of the phase of a wavefront passing through the plasma gives the chord-integrated density directly for all points measured on the wavefront. High-speed infrared cameras (up to ∼40,000 fps at ∼64×4 pixels) with resolutions up to 640×512 pixels suitable for use with a CO(2) laser are readily available, if expensive.


44th AIAA/ASME/SAE/ASEE Joint Propulsion Conference & Exhibit | 2008

Effects of Cathode Electron Emission on Hall Thruster Discharge

Yevgeny Raitses; Erik Granstedt; Artem Smirnov; Enrique Merino; Nathaniel J. Fisch

Low power cylindrical and annular geometry Hall thrusters are operated in a non-selfsustained regime with different thermionic cathode-neutralizers. The enhancement of the electron emission with a keeper current for the hollow cathode and with a wire heating for the filament cathode leads to a significant (up to 30%) narrowing of the plasma plume and increase of the energetic ion fraction. For the cylindrical Hall thruster, the observed variations of the plasma potential, electron temperature, and plasma density with the keeper current suggest that the electron emission from the cathode can affect the electron cross-field transport and the ionization in the thruster channel.


Review of Scientific Instruments | 2014

Digital holography for in situ real-time measurement of plasma-facing-component erosion.

Clarence E. Thomas; Erik Granstedt; T. M. Biewer; L. R. Baylor; S.K. Combs; S. J. Meitner; D. L. Hillis; R. Majeski; R. Kaita

In situ, real time measurement of net plasma-facing-component (PFC) erosion/deposition in a real plasma device is challenging due to the need for good spatial and temporal resolution, sufficient sensitivity, and immunity to fringe-jump errors. Design of a high-sensitivity, potentially high-speed, dual-wavelength CO2 laser digital holography system (nominally immune to fringe jumps) for PFC erosion measurement is discussed.


Journal Name: Propulsion and Power; Conference: 43rd AIAA/ASME/SAE/ASEE Joint Propulsion Conference and Exhibit, 8-11 July 2007, Cincinnati, OH. | 2007

Optimization of Cylindrical Hall Thrusters

Yevgeny Raitses; Artem Smirnov; Erik Granstedt; Nathaniel J. Fisch

The cylindrical Hall thruster features high ionization efficiency, quiet operation, and ion acceleration in a large volume-to-surface ratio channel with performance comparable with the state-of-the-art annular Hall thrusters. These characteristics were demonstrated in low and medium power ranges. Optimization of miniaturized cylindrical thrusters led to performance improvements in the 50-200W input power range, including plume narrowing, increased thruster efficiency, reliable discharge initiation, and stable operation.


Review of Scientific Instruments | 2016

First fast-ion D-alpha (FIDA) measurements and simulations on C-2U

N. Bolte; D. Gupta; L. Stagner; M. Onofri; S. Dettrick; Erik Granstedt; P. Petrov

The first measurements of fast-ion D-alpha (FIDA) radiation have been acquired on C-2U, Tri Alpha Energys advanced, beam-driven field-reversed configuration (FRC). These measurements are also forward modeled by FIDASIM. This is the first measurement and simulation of FIDA carried out on an FRC topology. FIDA measurements are made of Doppler-shifted Balmer-alpha light from neutralized fast ions using a bandpass filter and photomultiplier tube. One adjustable line-of-sight measured signals at eight locations and eight times during the FRC lifetime over 26 discharges. Filtered signals include only the highest energy ions (>6 keV) and share some salient features with the FIDASIM result. Highly Doppler-shifted beam radiation is also measured with a high-speed camera and is spatially well-correlated with FIDASIM.


Review of Scientific Instruments | 2012

Spectral emission measurements of lithium on the lithium tokamak experiment.

T.K. Gray; T. M. Biewer; D.P. Boyle; Erik Granstedt; R. Kaita; R. Maingi; R. Majeski

There has been a long-standing collaboration between ORNL and PPPL on edge and boundary layer physics. As part of this collaboration, ORNL has a large role in the instrumentation and interpretation of edge physics in the lithium tokamak experiment (LTX). In particular, a charge exchange recombination spectroscopy (CHERS) diagnostic is being designed and undergoing staged testing on LTX. Here we present results of passively measured lithium emission at 5166.89 A in LTX in anticipation of active spectroscopy measurements, which will be enabled by the installation of a neutral beam in 2013. Preliminary measurements are made in transient LTX plasmas with plasma current, I(p) < 70 kA, ohmic heating power, P(oh) ∼ 0.3 MW and discharge lifetimes of 10-15 ms. Measurements are made with a short focal length spectrometer and optics similar to the CHERS diagnostics on NSTX [R. E. Bell, Rev. Sci. Instrum. 68(2), 1273-1280 (1997)]. These preliminary measurements suggest that even without the neutral beam for active spectroscopy, there is sufficient passive lithium emission to allow for line-of-sight profile measurements of ion temperature, T(i); toroidal velocity and v(t). Results show peak T(i) = 70 eV and peak v(t) = 45 km/s were reached 10 ms into the discharge.


Review of Scientific Instruments | 2016

Design of a digital holography system for PFC erosion measurements on Proto-MPEX

Clarence E. Thomas; T. M. Biewer; L. R. Baylor; S.K. Combs; S. J. Meitner; J. Rapp; D. L. Hillis; Erik Granstedt; R. Majeski; R. Kaita

A project has been started at ORNL to develop a dual-wavelength digital holography system for plasma facing component erosion measurements on prototype material plasma exposure experiment. Such a system will allow in situ real-time measurements of component erosion. Initially the system will be developed with one laser, and first experimental laboratory measurements will be made with the single laser system. In the second year of development, a second CO2 laser will be added and measurements with the dual wavelength system will begin. Adding the second wavelength allows measurements at a much longer synthetic wavelength.


Fusion Engineering and Design | 2010

Experiments with liquid metal walls: Status of the lithium tokamak experiment

R. Kaita; L. Berzak; D.P. Boyle; T. Gray; Erik Granstedt; G. W. Hammett; C.M. Jacobson; Andrew Jones; Thomas Kozub; H.W. Kugel; Benoit P. Leblanc; Nicholas Logan; M. Lucia; D.P. Lundberg; R. Majeski; D.K. Mansfield; J. Menard; J. Spaleta; Trevor Strickler; J. Timberlake; Jongsoo Yoo; Leonid E. Zakharov; R. Maingi; V. Soukhanovskii; K. Tritz; Sophia Gershman


Fusion Engineering and Design | 2010

The Impact Of Lithium Wall Coatings On NSTX Discharges And The Engineering Of The Lithium Tokamak eXperiment (LTX)

R. Majeski; H.W. Kugel; R. Kaita; S. Avasarala; M.G. Bell; R.E. Bell; L. Berzak; P. Beiersdorfer; S.P. Gerhardt; Erik Granstedt; T. Gray; C.M. Jacobson; J. Kallman; S.M. Kaye; Thomas Kozub; Benoit P. Leblanc; J. Lepson; D.P. Lundberg; R. Maingi; D.K. Mansfield; S. Paul; G. Pereverzev; H. Schneider; V. Soukhanovskii; T. Strickler; D.P. Stotler; J. Timberlake; Leonid E. Zakharov


Archive | 2007

Overrun Discharge Current Operation of Low Power Cylindrical Hall Thrusters

Yevgeny Raitses; Artem Smirnov; Erik Granstedt; Nathaniel J. Fisch

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R. Majeski

Princeton Plasma Physics Laboratory

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R. Kaita

Princeton University

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C.M. Jacobson

Princeton Plasma Physics Laboratory

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D.P. Boyle

Princeton Plasma Physics Laboratory

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R. Maingi

Oak Ridge National Laboratory

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T. M. Biewer

Oak Ridge National Laboratory

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Leonid E. Zakharov

Princeton Plasma Physics Laboratory

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S. J. Meitner

Oak Ridge National Laboratory

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S.K. Combs

Oak Ridge National Laboratory

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J. Timberlake

Princeton Plasma Physics Laboratory

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