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  • 1
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: The receiver of the Joint European Torus (JET) energetic ion and alpha particle collective Thomson scattering diagnostic is calibrated assuming blackbody emission from the torus vacuum vessel (VV) and using electron cyclotron emission (ECE). The 32 receiver channels are absolutely calibrated with a mechanical chopper in the quasioptical arm of the receiver, alternating the receiver view between the torus vacuum at 320 °C and room temperature. This calibration is noisy due to the small difference between torus and room temperatures. A more accurate relative calibration is achieved with the ECE during plasma shots. The intensity of the ECE is found to be a smooth function of frequency, which enables the combination of the ECE calibration with the VV calibration. The accuracy of the absolute VV calibration is hereby improved to nearly the same standard as the relative ECE calibration. ECE signals measured by the calibrated receiver agree well with standard JET ECE diagnostics. Based on mathematical considerations presented here, noise is injected into the receiver final intermediate frequency stage during VV calibrations to provide more bit transitions for accurate analog-to-digital (AD) conversion of the low level calibration signals. This yields a resolution which is better than 1% of an (AD) step. © 1999 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 2
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: Spectral purity of the transmitter source of a collective Thomson scattering (CTS) system is vitally important to insure that measured signals only originate from the plasma and not from stray source light. A number of high power (up to 500 kW), 140 GHz gyrotron tubes used with the Joint European Torus (JET) CTS system have been found to have one or more spurious modes and many harmonics in the output spectrum. The CTS diagnostic receiver system was used to make measurements of the gyrotron spectrum. It was comprised of a homodyne part from MIT for frequency sidebands 〈500 MHz, and a heterodyne part constructed at JET for frequency sidebands from 0.1 to 6 GHz. One tube at high power produced a strong 25 MHz mode and its harmonics to large frequency offsets, unsuitable for CTS measurements. Only at reduced power of approximately 100 kW was this tube's spectrum sufficiently clean for CTS. Another tube at JET operated at 500 kW output power with only low level parasitic modes, indicating that higher power gyrotrons may be available for future alpha particle measurements. The main receiver was tested with a low power test setup which simulated the gyrotron stray source light, the thermal ion feature and plasma electron cyclotron emission. © 1999 American Institute of Physics.
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  • 3
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: A low-power 60 GHz gyrotron collective Thomson scattering diagnostic has been operating on TFTR to test the feasibility of detecting alpha particles when scattering perpendicular to the magnetic field. An enhanced scattered signal is predicted to result from the interaction of the energetic ions with plasma resonances in the lower hybrid frequency range. Millimeter-wave power levels at the plasma were approximately 200 W for typical pulse lengths of 50 ms. Deuterium and possible fusion product ion cyclotron frequencies and their harmonics were observed during neutral beam heating. These spectra are similar to ion cyclotron emission spectra which are detected with radio-frequency probes on TFTR at the plasma edge. Also, ion cyclotron resonance heating fundamental and harmonic fluctuations were observed. However, a signal has not been definitively detected in the lower hybrid frequency range which correlates to alpha particles. Broadband noise was observed during neutral beam heating which is greater than the predicted alpha particle signal. © 1997 American Institute of Physics.
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  • 4
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: A 60 GHz gyrotron collective Thomson scattering alpha particle diagnostic has been implemented for the D-T period on the Tokamak Fusion Test Reactor (TFTR). Gyrotron power of 0.1–1 kW in pulses of up to 1 s can be launched in X mode. Efficient corrugated waveguides are used with antennas and vacuum windows of the TFTR Microwave Scattering system. A multichannel synchronous detector receiver system and spectrum analyzer acquire the scattered signals. A 200 megasample/s digitizer and spectrum analyzer are used to resolve fine structure in the frequency spectrum. By scattering nearly perpendicular to the magnetic field, this experiment will take advantage of an enhancement of the scattered signal which results from the interaction of energetic ions with plasma resonances in the lower hybrid frequency range. Significant enhancements are expected with D-T fusion alpha particles, which should be detectable with gyrotron power of less than 1 kW, while maintaining an acceptable signal-to-noise ratio. This diagnostic will be the first experimental test of recent collective Thomson scattering models and should also provide an indication of the presence of energetic alpha particles in the core of TFTR. © 1995 American Institute of Physics.
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 102 (1995), S. 8378-8384 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Rate coefficients are reported for electronic quenching of OH A 2Σ v'=0 by N2, O2, CO, CO2, NO, Ar, Kr, and Xe measured at high temperatures behind reproducible shock waves. The cross section for quenching by Ar was found to be less than 0.06 A(ring)2. The cross sections for quenching by N2 and Kr were found to be 0.5 and 1.0 A(ring)2, respectively. The cross sections for the remaining species were found to be of order gas kinetic. For all of the species the cross sections were found to be very weak functions of temperature from 1900 to 2300 K. The measured cross sections are compared with previous measurements at lower temperatures. The observed variation with species and with temperature is observed to be consistent with a charge-transfer model for the process. © 1995 American Institute of Physics.
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 9 (1997), S. 3513-3522 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The hypervelocity two-dimensional reacting supersonic mixing layer experiments of Erdos et al. with a H2/air stream have been simulated with model free fine grid calculations on a N–S solver with full and single step chemistry. Response of the flow to fluctuations in the in-flow stream is utilized to examine chemistry fluid flow interactions. A favourable comparison of the computation with experimentally measured wall static pressure and heat transfer data along with flow picture forms the basis for further analysis. Insight into the mean flow thermal and reaction properties is provided from the examination of large scale structures in the flow in which the hydrogen stream is at 103 K flowing at 2.4 km/s (M=3.09) and the air stream is at 2400 K flowing at 3.8 km/s (M=3.99). The chemistry-flow interaction is dominated by large stream kinetic energy and affects the mean properties including the temperature profiles across the mixing layer. Single step chemistry, in comparison to full chemistry, is inadequate to describe ignition and early combustion processes, but seems reasonable for describing mixing and combustion downstream. Fast chemistry approximation coupled with mixture fraction based on hydrogen element seems to predict H2 mean profiles well; but this is shown to be due to the insensitivity of YH2 to progress of the reaction. This approximation under-predicts YO2 though the general shape of the profile is maintained. Mixture fraction variable approach is shown to be inadequate for the prediction of the H2O mass fraction because of the effect of non-normal diffusion. Finite chemistry conditions are shown to prevail throughout the domain of the mixing layer. It appears that use of mixture fraction approach may be inadequate to compute high speed reacting turbulent flows. © 1997 American Institute of Physics.
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Physics of Fluids 7 (1995), S. 1071-1081 
    ISSN: 1089-7666
    Source: AIP Digital Archive
    Topics: Physics
    Notes: An experimental study was conducted of mixing in supersonic axisymmetric shear layers using planar laser-induced fluorescence of seeded nitric oxide. Passive scalar images were obtained at convective Mach numbers (Mc) of 0.35, 0.82, and 1.3. Values of the fraction of mixed fluid (δm/δ1) were obtained at Mc=0.35 and 0.82, using a technique that employs fluorescence quenching to provide a direct measurement of fluid unmixedness. From the unmixedness measurement, an accurate value of the fraction of mixed fluid can be derived, even when the smallest mixing scales are not resolved. The visualizations reveal that at low Mc, the turbulent structures appear primarily as rollers, although the degree of axisymmetry of the rollers could not be determined. At high Mc, the structures were more irregular, and often appeared as the jagged, irregular structures that have been previously documented in planar layers. Concentration fluctuation statistics show that fluctuations are smaller at Mc=0.82 than at Mc=0.35, particularly on the high-speed edge of the layer, but those at Mc=1.3 are comparable to those at Mc=0.35. Using the quenching method, the fraction of mixed fluid, δm/δ 1, was found to be 0.45 and 0.48 at Mc=0.35 and 0.82, respectively. If the effect of the Reynolds number difference is taken into account, then the measured trend is even stronger. One can conclude then that the moderately compressible axisymmetric mixing layer has a slightly greater mixing efficiency than its incompressible counterpart. © 1995 American Institute of Physics.
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