Search results for " coi"

showing 10 items of 326 documents

A new frozen-spin target for 4π particle detection

1999

Abstract A new frozen-spin target has been developed, that allows the detection of emitted particles in an angular acceptance of almost 4π in the laboratory frame. The central part of this new target represents a 3He/4He dilution refrigerator that is installed horizontally along the beam axis. The refrigerator includes an internal superconducting holding coil to maintain the nucleon polarization in the frozen-spin mode longitudinally to the beam. The design of the dilution refrigerator and the use of an internal holding coil enabled for the first time the measurement of a spin-dependent total cross section in combination with a polarized solid state target. This new frozen-spin target was u…

PhysicsNuclear and High Energy Physicsmedia_common.quotation_subjectRefrigerator carPolarization (waves)AsymmetryHelicityNuclear physicsElectromagnetic coilSum rule in quantum mechanicsDilution refrigeratorNucleonInstrumentationmedia_commonNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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The influence of the quarter wave plates in automated photoelasticity

2002

During the last decades, several methods have been proposed to automate photoelastic analyses. Some procedures are based on the circularly polarised light by using quarter wave plates. However, quarter wave plates are typically matched for a specific wavelength, and an error is introduced at different wavelengths. The error of quarter wave plates affects the measurement of isochromatic and isoclinic data. In this paper, the influence of the errors of quarter wave plates in some of the most common automated photoelastic methods is reviewed. The errors in the photoelastic data are given and the procedures to reduce, or eliminate, them are also suggested.

PhysicsPhotoelasticitybusiness.industryMechanical EngineeringWaveplateAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic Materialssymbols.namesakeWavelengthDigital imageFourier transformOpticsData acquisitionsymbolsElectrical and Electronic EngineeringbusinessCircular polarizationQuarter (Canadian coin)
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Plenary talk - non coaxial force and inductance calculations for bitter coils and coils with uniform radial current distributions

2011

Recently the Bessel function approach to calculating the magnetic fields of coils has been used to calculate the mutual inductance and the force between two non coaxial thick cylindrical coils with parallel axes and uniform radial current distributions. This method can also be applied to calculate the force and inductance between an ordinary coil and a Bitter coil, or between two bitter coils, not necessarily coaxial. Bitter coils give a simpler case of the method, and it is possible to solve analytically for the magnetic field of a bitter disk.

PhysicsQuantitative Biology::BiomoleculesCurrent distributionbusiness.industryPhysics::Medical PhysicsElectrical engineeringMechanicsMagnetic fieldInductancesymbols.namesakeElectromagnetic coilCondensed Matter::SuperconductivitysymbolsCoaxialCurrent (fluid)businessBessel functionExcitation2011 International Conference on Applied Superconductivity and Electromagnetic Devices
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Exact solutions for the mutual inductance of circular coils and elliptic coils

2012

An exact solution is presented for the mutual inductance between general noncoaxial thin circular and elliptic coils with parallel axes. The thin coil solution is given as an angular integral of an elliptic integral expression. In addition, for the coaxial case, an exact solution is given for the mutual inductance of a thick circular coil and a thick elliptic coil. The elliptic coil is such that the coil thickness is the same along both elliptic semi-axes. The thick coil solution is given as an integral of an expression involving Bessel and Struve functions. Extensive numerical results for sample geometries are given for both solutions, which are cross checked against each other in the limi…

PhysicsQuantitative Biology::BiomoleculesPhysics::Medical PhysicsMathematical analysisElectronic Optical and Magnetic MaterialsMagnetic fieldInductancesymbols.namesakeExact solutions in general relativityElectromagnetic coilStruve functionsymbolsElliptic integralElectrical and Electronic EngineeringCoaxialBessel functionIEEE Transactions on Magnetics
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Non coaxial force and inductance calculations for bitter coils and coils with uniform radial current distributions

2011

Recently the Bessel function approach to calculating the magnetic fields of coils has been used to calculate the mutual inductance and the force between two non coaxial thick cylindrical coils with parallel axes and uniform radial current distributions. This method can also be applied to calculate the force and inductance between an ordinary coil and a Bitter coil, or between two bitter coils, not necessarily coaxial. Bitter coils give a simpler case of the method, and it is possible to solve analytically for the magnetic field of a bitter disk.

PhysicsQuantitative Biology::Biomoleculesbusiness.industryPhysics::Medical PhysicsElectrical engineeringMechanicsMagnetic fieldInductancesymbols.namesakeElectromagnetic coilCondensed Matter::SuperconductivitysymbolsCurrent (fluid)CoaxialbusinessSuperconducting CoilsBessel functionExcitation2011 International Conference on Applied Superconductivity and Electromagnetic Devices
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Designing spin-spin interactions with one and two dimensional ion crystals in planar micro traps

2011

We discuss the experimental feasibility of quantum simulation with trapped ion crystals, using magnetic field gradients. We describe a micro structured planar ion trap, which contains a central wire loop generating a strong magnetic gradient of about 20 T/m in an ion crystal held about 160 \mu m above the surface. On the theoretical side, we extend a proposal about spin-spin interactions via magnetic gradient induced coupling (MAGIC) [Johanning, et al, J. Phys. B: At. Mol. Opt. Phys. 42 (2009) 154009]. We describe aspects where planar ion traps promise novel physics: Spin-spin coupling strengths of transversal eigenmodes exhibit significant advantages over the coupling schemes in longitudin…

PhysicsQuantum PhysicsCondensed matter physicsmedia_common.quotation_subjectFOS: Physical sciencesFrustrationQuantum simulatorAtomic and Molecular Physics and OpticsSpin magnetic momentIonMagnetic fieldPlanarElectromagnetic coilIon trapQuantum Physics (quant-ph)media_common
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246. Analysis of signal-to-noise ratio for a 2-channels coil developed to enable transcranial Magnetic Resonance-guided Focused Ultrasound Surgery (t…

2018

Abstract Purpose In recent years trans-cranial Magnetic Resonance-guided Focused Ultrasound Surgery (tcMRgFUS) treatments have aroused large scientific and medical interest [1] . Usually, tcMRgFUS systems are integrated with 3 T systems which allow the use of the body RF coil for both real time imaging and MR-thermometry. At University Hospital of Palermo there is the world-first installation of a tcMRgFUS system integrated with a 1.5 T scanner. Here we present the characterization in terms of signal-to-noise ratio (SNR) of a dedicated RF coils suitably developed (by InSightec) to enable tcMRgFUS treatments with 1.5 T MR units. Methods and materials The focused ultrasound equipment (ExAblat…

PhysicsScannerExAblateBiophysicsGeneral Physics and AstronomyGeneral MedicineImaging phantom030218 nuclear medicine & medical imagingMagnetic resonance guided focused ultrasound surgery03 medical and health sciences0302 clinical medicineTransducerSignal-to-noise ratio (imaging)Electromagnetic coil030220 oncology & carcinogenesisRadiology Nuclear Medicine and imagingBiomedical engineeringRadiofrequency coilPhysica Medica
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3-D Shielding Analyses of the Vertical and Mid-Plane Ports in ITER

1996

A three dimensional (3-D) shielding analysis of the International Thermonuclear Experimental Reactor (ITER) has been performed with the aim of calculating the nuclear heating on the magnet system, correlating it to the existing vertical and horizontal ports. When these openings are left unshielded, more than 50 kW are calculated for the upper half of Toroidal Field Coil system and two of the Poloidal Field Coils. A simple plug, with same thickness as of the vacuum vessel can lower the heating to meet the imposed requirements. 5 refs., 6 figs., 4 tabs.

PhysicsThermonuclear fusionNuclear heatingPlane (geometry)020209 energyNuclear engineeringMonte Carlo methodGeneral Engineering02 engineering and technology01 natural sciences010305 fluids & plasmaslaw.inventionNuclear physicsElectromagnetic coillawMagnet0103 physical sciencesElectromagnetic shielding0202 electrical engineering electronic engineering information engineeringSpark plugFusion Technology
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A Ioffe Trap Magnet for the Project 8 Atom Trapping Demonstrator

2020

The goal of the Project 8 experiment (B. Monreal and J. Formaggio, 2009) is to measure the absolute neutrino mass using tritium, which involves precisely measuring the energies of the beta-decay electrons in the high-energy tail of the spectrum (A. A. Esfahani et al. , 2017). The experimental installation of Project 8 Atom Trapping Demonstrator requires a magnet with rather unusual field properties. The magnet has to contain within the cold mass a large volume enclosed by a continuous, uninterrupted boundary higher than 2 T, whereas the field in a substantial volume inside this boundary has to be of the order of 10−4 T or less. A 1-T solenoid field provides the background field necessary fo…

PhysicsToroidMagnetic separationSuperconducting magnetElectronCondensed Matter PhysicsThermal conduction01 natural sciences7. Clean energyElectronic Optical and Magnetic MaterialsElectromagnetic coilMagnet0103 physical sciencesDuct (flow)Electrical and Electronic EngineeringAtomic physics010306 general physics
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Characterization and Error Compensation of a Rogowski Coil in the Presence of Harmonics

2011

This paper reports the results of an experimental study dealing with a commercial Rogowski coil current transducer (RCCT) in the presence of harmonic distortion. The RCCT was observed under two conditions: 1) sinusoidal excitation with frequencies from 50 to 750 Hz and 2) nonsinusoidal excitation using fundamental frequency and one harmonic, with adjustable amplitude and phase shift. The experimental results show only a weak dependence of the harmonic current ratio error and phase displacement on the amplitude and phase shift of the excitation harmonic. The phase displacement is also independent of the conductor position within the Rogowski coil window. An error compensation method, based o…

PhysicsTotal harmonic distortionFrequency responsebusiness.industryAcousticsElectrical engineeringFundamental frequencycurrent transducerRogowski coilCurrent measurement current transducer frequency response harmonic distortion power system harmonics Rogowski coil.harmonic distortionHarmonic analysisAmplitudeHarmonicsHarmonicpower system harmonicElectrical and Electronic EngineeringbusinessInstrumentationSettore ING-INF/07 - Misure Elettriche E ElettronicheRogowski coil
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