Simulation Model for Design of a New Power Supply
Identifieur interne :
000471 ( PascalFrancis/Curation );
précédent :
000470;
suivant :
000472
Simulation Model for Design of a New Power Supply
Auteurs : T. Takayanagi [
Japon] ;
N. Hayashi [
Japon] ;
T. Ueno [
Japon] ;
T. Togashi [
Japon] ;
Y. Irie [
Japon]
Source :
-
IEEE transactions on applied superconductivity [ 1051-8223 ] ; 2012.
RBID : Pascal:13-0011400
Descripteurs français
- Pascal (Inist)
- Simulation système,
Alimentation électrique,
Aimant,
Surface équivalente radar,
Cyclage,
Synchrotron,
Japon,
Accélérateur proton,
Oscillation forcée,
Impédance charge,
Chambre à vide,
Simulation circuit,
Codage,
Structure résonnante,
Schéma équivalent,
Céramique,
Electronique puissance,
2920L.
- Wicri :
English descriptors
- KwdEn :
- Ceramic materials,
Circuit simulation,
Coding,
Cycling,
Equivalent circuit,
Forced oscillation,
Japan,
Load impedance,
Magnet,
Power electronics,
Power supply,
Proton accelerator,
Radar cross section,
Resonant structure,
Synchrotrons,
System simulation,
Vacuum chamber.
Abstract
The simulation model for a new power supply of the injection bump system magnets [1]-[4] of the 3-GeV RCS (Rapid Cycling Synchrotron) in J-PARC (Japan Proton Accelerator Complex) [5], [6] has been constructed. The new power supply requires the reduction of the ripple noise current which will resonate with load and excites a forced beam oscillation at ∼96 kHz in the injection stage. In order to incorporate the load impedance in the simulation model, the impedances of a feeder line and the bump magnet with a ceramic vacuum chamber [7] inside were measured. The RF shield is formed on the ceramic surface along the beam direction. The results were successfully analysed using the OPERA-3D [8] and the circuit simulation code, Micro-Cap [9], and showed a good agreement. It was found the RF shield of a ceramic chamber has a resonant structure corresponding to ∼96 kHz.
| pA |
| A01 | 01 | 1 | | @0 1051-8223 |
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| A03 | | 1 | | @0 IEEE trans. appl. supercond. |
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| A05 | | | | @2 22 |
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| A06 | | | | @2 3 |
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| A08 | 01 | 1 | ENG | @1 Simulation Model for Design of a New Power Supply |
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| A09 | 01 | 1 | ENG | @1 The Twenty-First International Conference on Magnet Technology |
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| A11 | 01 | 1 | | @1 TAKAYANAGI (T.) |
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| A11 | 02 | 1 | | @1 HAYASHI (N.) |
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| A11 | 03 | 1 | | @1 UENO (T.) |
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| A11 | 04 | 1 | | @1 TOGASHI (T.) |
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| A11 | 05 | 1 | | @1 IRIE (Y.) |
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| A14 | 01 | | | @1 JAEA/J-PARC @2 Ibaraki-ken 319-1195 @3 JPN @Z 1 aut. @Z 2 aut. @Z 3 aut. @Z 4 aut. |
|---|
| A14 | 02 | | | @1 KEK @2 Ibaraki-Ken 305-0801 @3 JPN @Z 5 aut. |
|---|
| A18 | 01 | 1 | | @1 IEEE (Institute of Electrical and Electronics Engineers @3 USA @9 org-cong. |
|---|
| A20 | | | | @2 5400704.1-5400704.4 |
|---|
| A21 | | | | @1 2012 |
|---|
| A23 | 01 | | | @0 ENG |
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| A43 | 01 | | | @1 INIST @2 22424 @5 354000506810803660 |
|---|
| A44 | | | | @0 0000 @1 © 2013 INIST-CNRS. All rights reserved. |
|---|
| A45 | | | | @0 13 ref. |
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| A47 | 01 | 1 | | @0 13-0011400 |
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| A60 | | | | @1 P @2 C |
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| A61 | | | | @0 A |
|---|
| A64 | 01 | 1 | | @0 IEEE transactions on applied superconductivity |
|---|
| A66 | 01 | | | @0 USA |
|---|
| C01 | 01 | | ENG | @0 The simulation model for a new power supply of the injection bump system magnets [1]-[4] of the 3-GeV RCS (Rapid Cycling Synchrotron) in J-PARC (Japan Proton Accelerator Complex) [5], [6] has been constructed. The new power supply requires the reduction of the ripple noise current which will resonate with load and excites a forced beam oscillation at ∼96 kHz in the injection stage. In order to incorporate the load impedance in the simulation model, the impedances of a feeder line and the bump magnet with a ceramic vacuum chamber [7] inside were measured. The RF shield is formed on the ceramic surface along the beam direction. The results were successfully analysed using the OPERA-3D [8] and the circuit simulation code, Micro-Cap [9], and showed a good agreement. It was found the RF shield of a ceramic chamber has a resonant structure corresponding to ∼96 kHz. |
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| C02 | 01 | X | | @0 001D03D |
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| C02 | 02 | X | | @0 001D05H |
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| C02 | 03 | X | | @0 001D05G01 |
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| C02 | 04 | X | | @0 001D03G01 |
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| C03 | 01 | X | FRE | @0 Simulation système @5 01 |
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| C03 | 01 | X | ENG | @0 System simulation @5 01 |
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| C03 | 01 | X | SPA | @0 Simulación sistema @5 01 |
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| C03 | 02 | X | FRE | @0 Alimentation électrique @5 02 |
|---|
| C03 | 02 | X | ENG | @0 Power supply @5 02 |
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| C03 | 02 | X | SPA | @0 Alimentación eléctrica @5 02 |
|---|
| C03 | 03 | X | FRE | @0 Aimant @5 03 |
|---|
| C03 | 03 | X | ENG | @0 Magnet @5 03 |
|---|
| C03 | 03 | X | SPA | @0 Imán @5 03 |
|---|
| C03 | 04 | X | FRE | @0 Surface équivalente radar @5 04 |
|---|
| C03 | 04 | X | ENG | @0 Radar cross section @5 04 |
|---|
| C03 | 04 | X | SPA | @0 Superficie equivalente radar @5 04 |
|---|
| C03 | 05 | X | FRE | @0 Cyclage @5 05 |
|---|
| C03 | 05 | X | ENG | @0 Cycling @5 05 |
|---|
| C03 | 05 | X | SPA | @0 Ciclaje @5 05 |
|---|
| C03 | 06 | X | FRE | @0 Synchrotron @5 06 |
|---|
| C03 | 06 | X | ENG | @0 Synchrotrons @5 06 |
|---|
| C03 | 06 | X | SPA | @0 Sincrotrón @5 06 |
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| C03 | 07 | X | FRE | @0 Japon @2 NG @5 07 |
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| C03 | 07 | X | ENG | @0 Japan @2 NG @5 07 |
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| C03 | 07 | X | SPA | @0 Japón @2 NG @5 07 |
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| C03 | 08 | X | FRE | @0 Accélérateur proton @5 08 |
|---|
| C03 | 08 | X | ENG | @0 Proton accelerator @5 08 |
|---|
| C03 | 08 | X | SPA | @0 Acelerador protón @5 08 |
|---|
| C03 | 09 | X | FRE | @0 Oscillation forcée @5 09 |
|---|
| C03 | 09 | X | ENG | @0 Forced oscillation @5 09 |
|---|
| C03 | 09 | X | SPA | @0 Oscilación forzada @5 09 |
|---|
| C03 | 10 | X | FRE | @0 Impédance charge @5 10 |
|---|
| C03 | 10 | X | ENG | @0 Load impedance @5 10 |
|---|
| C03 | 10 | X | SPA | @0 Impedancia carga @5 10 |
|---|
| C03 | 11 | X | FRE | @0 Chambre à vide @5 11 |
|---|
| C03 | 11 | X | ENG | @0 Vacuum chamber @5 11 |
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| C03 | 11 | X | SPA | @0 Cámara de vacío @5 11 |
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| C03 | 12 | 3 | FRE | @0 Simulation circuit @5 12 |
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| C03 | 12 | 3 | ENG | @0 Circuit simulation @5 12 |
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| C03 | 13 | X | FRE | @0 Codage @5 13 |
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| C03 | 13 | X | ENG | @0 Coding @5 13 |
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| C03 | 13 | X | SPA | @0 Codificación @5 13 |
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| C03 | 14 | X | FRE | @0 Structure résonnante @5 14 |
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| C03 | 14 | X | ENG | @0 Resonant structure @5 14 |
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| C03 | 14 | X | SPA | @0 Estructura resonante @5 14 |
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| C03 | 15 | X | FRE | @0 Schéma équivalent @5 15 |
|---|
| C03 | 15 | X | ENG | @0 Equivalent circuit @5 15 |
|---|
| C03 | 15 | X | SPA | @0 Esquema equivalente @5 15 |
|---|
| C03 | 16 | X | FRE | @0 Céramique @5 22 |
|---|
| C03 | 16 | X | ENG | @0 Ceramic materials @5 22 |
|---|
| C03 | 16 | X | SPA | @0 Cerámica @5 22 |
|---|
| C03 | 17 | X | FRE | @0 Electronique puissance @5 46 |
|---|
| C03 | 17 | X | ENG | @0 Power electronics @5 46 |
|---|
| C03 | 17 | X | SPA | @0 Electrónica potencia @5 46 |
|---|
| C03 | 18 | X | FRE | @0 2920L @4 INC @5 56 |
|---|
| C07 | 01 | X | FRE | @0 Asie @2 NG |
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| C07 | 01 | X | ENG | @0 Asia @2 NG |
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| C07 | 01 | X | SPA | @0 Asia @2 NG |
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| N21 | | | | @1 007 |
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| N44 | 01 | | | @1 OTO |
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| N82 | | | | @1 OTO |
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|
|---|
| pR |
| A30 | 01 | 1 | ENG | @1 International Conference on Magnet Technology @2 22 @3 Marseille FRA @4 2011-09-12 |
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|
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Links toward previous steps (curation, corpus...)
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Pascal:13-0011400
Le document en format XML
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<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
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</affiliation><author><name sortKey="Irie, Y" sort="Irie, Y" uniqKey="Irie Y" first="Y." last="Irie">Y. Irie</name>
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</affiliation><series><title level="j" type="main">IEEE transactions on applied superconductivity</title>
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</seriesStmt><profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Ceramic materials</term>
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<term>Coding</term>
<term>Cycling</term>
<term>Equivalent circuit</term>
<term>Forced oscillation</term>
<term>Japan</term>
<term>Load impedance</term>
<term>Magnet</term>
<term>Power electronics</term>
<term>Power supply</term>
<term>Proton accelerator</term>
<term>Radar cross section</term>
<term>Resonant structure</term>
<term>Synchrotrons</term>
<term>System simulation</term>
<term>Vacuum chamber</term>
</keywords><keywords scheme="Pascal" xml:lang="fr"><term>Simulation système</term>
<term>Alimentation électrique</term>
<term>Aimant</term>
<term>Surface équivalente radar</term>
<term>Cyclage</term>
<term>Synchrotron</term>
<term>Japon</term>
<term>Accélérateur proton</term>
<term>Oscillation forcée</term>
<term>Impédance charge</term>
<term>Chambre à vide</term>
<term>Simulation circuit</term>
<term>Codage</term>
<term>Structure résonnante</term>
<term>Schéma équivalent</term>
<term>Céramique</term>
<term>Electronique puissance</term>
<term>2920L</term>
</keywords><keywords scheme="Wicri" type="geographic" xml:lang="fr"><term>Japon</term>
</keywords><keywords scheme="Wicri" type="topic" xml:lang="fr"><term>Codage</term>
<term>Céramique</term>
</keywords><front><div type="abstract" xml:lang="en">The simulation model for a new power supply of the injection bump system magnets [1]-[4] of the 3-GeV RCS (Rapid Cycling Synchrotron) in J-PARC (Japan Proton Accelerator Complex) [5], [6] has been constructed. The new power supply requires the reduction of the ripple noise current which will resonate with load and excites a forced beam oscillation at ∼96 kHz in the injection stage. In order to incorporate the load impedance in the simulation model, the impedances of a feeder line and the bump magnet with a ceramic vacuum chamber [7] inside were measured. The RF shield is formed on the ceramic surface along the beam direction. The results were successfully analysed using the OPERA-3D [8] and the circuit simulation code, Micro-Cap [9], and showed a good agreement. It was found the RF shield of a ceramic chamber has a resonant structure corresponding to ∼96 kHz.</div>
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</fA08><fA09 i1="01" i2="1" l="ENG"><s1>The Twenty-First International Conference on Magnet Technology</s1>
</fA09><fA11 i1="01" i2="1"><s1>TAKAYANAGI (T.)</s1>
</fA11><fA11 i1="02" i2="1"><s1>HAYASHI (N.)</s1>
</fA11><fA11 i1="03" i2="1"><s1>UENO (T.)</s1>
</fA11><fA11 i1="04" i2="1"><s1>TOGASHI (T.)</s1>
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</fA11><fA14 i1="01"><s1>JAEA/J-PARC</s1>
<s2>Ibaraki-ken 319-1195</s2>
<s3>JPN</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
</fA14><fA14 i1="02"><s1>KEK</s1>
<s2>Ibaraki-Ken 305-0801</s2>
<s3>JPN</s3>
<sZ>5 aut.</sZ>
</fA14><fA18 i1="01" i2="1"><s1>IEEE (Institute of Electrical and Electronics Engineers</s1>
<s3>USA</s3>
<s9>org-cong.</s9>
</fA18><fA20><s2>5400704.1-5400704.4</s2>
</fA20><fA21><s1>2012</s1>
</fA21><fA23 i1="01"><s0>ENG</s0>
</fA23><fA43 i1="01"><s1>INIST</s1>
<s2>22424</s2>
<s5>354000506810803660</s5>
</fA43><fA44><s0>0000</s0>
<s1>© 2013 INIST-CNRS. All rights reserved.</s1>
</fA44><fA45><s0>13 ref.</s0>
</fA45><fA47 i1="01" i2="1"><s0>13-0011400</s0>
</fA47><fA60><s1>P</s1>
<s2>C</s2>
</fA60><fA64 i1="01" i2="1"><s0>IEEE transactions on applied superconductivity</s0>
</fA64><fA66 i1="01"><s0>USA</s0>
</fA66><fC01 i1="01" l="ENG"><s0>The simulation model for a new power supply of the injection bump system magnets [1]-[4] of the 3-GeV RCS (Rapid Cycling Synchrotron) in J-PARC (Japan Proton Accelerator Complex) [5], [6] has been constructed. The new power supply requires the reduction of the ripple noise current which will resonate with load and excites a forced beam oscillation at ∼96 kHz in the injection stage. In order to incorporate the load impedance in the simulation model, the impedances of a feeder line and the bump magnet with a ceramic vacuum chamber [7] inside were measured. The RF shield is formed on the ceramic surface along the beam direction. The results were successfully analysed using the OPERA-3D [8] and the circuit simulation code, Micro-Cap [9], and showed a good agreement. It was found the RF shield of a ceramic chamber has a resonant structure corresponding to ∼96 kHz.</s0>
</fC01><fC02 i1="01" i2="X"><s0>001D03D</s0>
</fC02><fC02 i1="02" i2="X"><s0>001D05H</s0>
</fC02><fC02 i1="03" i2="X"><s0>001D05G01</s0>
</fC02><fC02 i1="04" i2="X"><s0>001D03G01</s0>
</fC02><fC03 i1="01" i2="X" l="FRE"><s0>Simulation système</s0>
<s5>01</s5>
</fC03><fC03 i1="01" i2="X" l="ENG"><s0>System simulation</s0>
<s5>01</s5>
</fC03><fC03 i1="01" i2="X" l="SPA"><s0>Simulación sistema</s0>
<s5>01</s5>
</fC03><fC03 i1="02" i2="X" l="FRE"><s0>Alimentation électrique</s0>
<s5>02</s5>
</fC03><fC03 i1="02" i2="X" l="ENG"><s0>Power supply</s0>
<s5>02</s5>
</fC03><fC03 i1="02" i2="X" l="SPA"><s0>Alimentación eléctrica</s0>
<s5>02</s5>
</fC03><fC03 i1="03" i2="X" l="FRE"><s0>Aimant</s0>
<s5>03</s5>
</fC03><fC03 i1="03" i2="X" l="ENG"><s0>Magnet</s0>
<s5>03</s5>
</fC03><fC03 i1="03" i2="X" l="SPA"><s0>Imán</s0>
<s5>03</s5>
</fC03><fC03 i1="04" i2="X" l="FRE"><s0>Surface équivalente radar</s0>
<s5>04</s5>
</fC03><fC03 i1="04" i2="X" l="ENG"><s0>Radar cross section</s0>
<s5>04</s5>
</fC03><fC03 i1="04" i2="X" l="SPA"><s0>Superficie equivalente radar</s0>
<s5>04</s5>
</fC03><fC03 i1="05" i2="X" l="FRE"><s0>Cyclage</s0>
<s5>05</s5>
</fC03><fC03 i1="05" i2="X" l="ENG"><s0>Cycling</s0>
<s5>05</s5>
</fC03><fC03 i1="05" i2="X" l="SPA"><s0>Ciclaje</s0>
<s5>05</s5>
</fC03><fC03 i1="06" i2="X" l="FRE"><s0>Synchrotron</s0>
<s5>06</s5>
</fC03><fC03 i1="06" i2="X" l="ENG"><s0>Synchrotrons</s0>
<s5>06</s5>
</fC03><fC03 i1="06" i2="X" l="SPA"><s0>Sincrotrón</s0>
<s5>06</s5>
</fC03><fC03 i1="07" i2="X" l="FRE"><s0>Japon</s0>
<s2>NG</s2>
<s5>07</s5>
</fC03><fC03 i1="07" i2="X" l="ENG"><s0>Japan</s0>
<s2>NG</s2>
<s5>07</s5>
</fC03><fC03 i1="07" i2="X" l="SPA"><s0>Japón</s0>
<s2>NG</s2>
<s5>07</s5>
</fC03><fC03 i1="08" i2="X" l="FRE"><s0>Accélérateur proton</s0>
<s5>08</s5>
</fC03><fC03 i1="08" i2="X" l="ENG"><s0>Proton accelerator</s0>
<s5>08</s5>
</fC03><fC03 i1="08" i2="X" l="SPA"><s0>Acelerador protón</s0>
<s5>08</s5>
</fC03><fC03 i1="09" i2="X" l="FRE"><s0>Oscillation forcée</s0>
<s5>09</s5>
</fC03><fC03 i1="09" i2="X" l="ENG"><s0>Forced oscillation</s0>
<s5>09</s5>
</fC03><fC03 i1="09" i2="X" l="SPA"><s0>Oscilación forzada</s0>
<s5>09</s5>
</fC03><fC03 i1="10" i2="X" l="FRE"><s0>Impédance charge</s0>
<s5>10</s5>
</fC03><fC03 i1="10" i2="X" l="ENG"><s0>Load impedance</s0>
<s5>10</s5>
</fC03><fC03 i1="10" i2="X" l="SPA"><s0>Impedancia carga</s0>
<s5>10</s5>
</fC03><fC03 i1="11" i2="X" l="FRE"><s0>Chambre à vide</s0>
<s5>11</s5>
</fC03><fC03 i1="11" i2="X" l="ENG"><s0>Vacuum chamber</s0>
<s5>11</s5>
</fC03><fC03 i1="11" i2="X" l="SPA"><s0>Cámara de vacío</s0>
<s5>11</s5>
</fC03><fC03 i1="12" i2="3" l="FRE"><s0>Simulation circuit</s0>
<s5>12</s5>
</fC03><fC03 i1="12" i2="3" l="ENG"><s0>Circuit simulation</s0>
<s5>12</s5>
</fC03><fC03 i1="13" i2="X" l="FRE"><s0>Codage</s0>
<s5>13</s5>
</fC03><fC03 i1="13" i2="X" l="ENG"><s0>Coding</s0>
<s5>13</s5>
</fC03><fC03 i1="13" i2="X" l="SPA"><s0>Codificación</s0>
<s5>13</s5>
</fC03><fC03 i1="14" i2="X" l="FRE"><s0>Structure résonnante</s0>
<s5>14</s5>
</fC03><fC03 i1="14" i2="X" l="ENG"><s0>Resonant structure</s0>
<s5>14</s5>
</fC03><fC03 i1="14" i2="X" l="SPA"><s0>Estructura resonante</s0>
<s5>14</s5>
</fC03><fC03 i1="15" i2="X" l="FRE"><s0>Schéma équivalent</s0>
<s5>15</s5>
</fC03><fC03 i1="15" i2="X" l="ENG"><s0>Equivalent circuit</s0>
<s5>15</s5>
</fC03><fC03 i1="15" i2="X" l="SPA"><s0>Esquema equivalente</s0>
<s5>15</s5>
</fC03><fC03 i1="16" i2="X" l="FRE"><s0>Céramique</s0>
<s5>22</s5>
</fC03><fC03 i1="16" i2="X" l="ENG"><s0>Ceramic materials</s0>
<s5>22</s5>
</fC03><fC03 i1="16" i2="X" l="SPA"><s0>Cerámica</s0>
<s5>22</s5>
</fC03><fC03 i1="17" i2="X" l="FRE"><s0>Electronique puissance</s0>
<s5>46</s5>
</fC03><fC03 i1="17" i2="X" l="ENG"><s0>Power electronics</s0>
<s5>46</s5>
</fC03><fC03 i1="17" i2="X" l="SPA"><s0>Electrónica potencia</s0>
<s5>46</s5>
</fC03><fC03 i1="18" i2="X" l="FRE"><s0>2920L</s0>
<s4>INC</s4>
<s5>56</s5>
</fC03><fC07 i1="01" i2="X" l="FRE"><s0>Asie</s0>
<s2>NG</s2>
</fC07><fC07 i1="01" i2="X" l="ENG"><s0>Asia</s0>
<s2>NG</s2>
</fC07><fC07 i1="01" i2="X" l="SPA"><s0>Asia</s0>
<s2>NG</s2>
</fC07><fN21><s1>007</s1>
</fN21><fN44 i1="01"><s1>OTO</s1>
</fN44><fN82><s1>OTO</s1>
</fN82><pR><fA30 i1="01" i2="1" l="ENG"><s1>International Conference on Magnet Technology</s1>
<s2>22</s2>
<s3>Marseille FRA</s3>
<s4>2011-09-12</s4>
</fA30>
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