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A simple model for electromagnetic field in RFQ channel. / Drivotin, O. I.; Dulatov, I. T.

25th Russian Particle Accelerator Conference, RuPAC 2016. JACoW, 2016. стр. 244-246 (25th Russian Particle Accelerator Conference, RuPAC 2016).

Результаты исследований: Публикации в книгах, отчётах, сборниках, трудах конференций › статья в сборнике материалов конференции › научная › Рецензирование

Harvard

Drivotin, OI & Dulatov, IT 2016, A simple model for electromagnetic field in RFQ channel. в 25th Russian Particle Accelerator Conference, RuPAC 2016. 25th Russian Particle Accelerator Conference, RuPAC 2016, JACoW, стр. 244-246, XXV Всероссийская конференция по ускорителям заряженных частиц , St. Petersburg, Российская Федерация, 21/11/16.

APA

Drivotin, O. I., & Dulatov, I. T. (2016). A simple model for electromagnetic field in RFQ channel. в 25th Russian Particle Accelerator Conference, RuPAC 2016 (стр. 244-246). (25th Russian Particle Accelerator Conference, RuPAC 2016). JACoW.

Vancouver

Drivotin OI, Dulatov IT. A simple model for electromagnetic field in RFQ channel. в 25th Russian Particle Accelerator Conference, RuPAC 2016. JACoW. 2016. стр. 244-246. (25th Russian Particle Accelerator Conference, RuPAC 2016).

Author

Drivotin, O. I. ; Dulatov, I. T. / A simple model for electromagnetic field in RFQ channel. 25th Russian Particle Accelerator Conference, RuPAC 2016. JACoW, 2016. стр. 244-246 (25th Russian Particle Accelerator Conference, RuPAC 2016).

BibTeX

@inproceedings{8c46f5d7c7fa467484d3ccfc8a11c36c,
title = "A simple model for electromagnetic field in RFQ channel",
abstract = "Numerical solution of the RFQ structure optimization problem requires a great amount of computation. Each consecutive step of the numerical optimization includes modification of geometry of the channel and computation of electromagnetic field for modified geometry. Therefore, a simple model describing the field in the channel is needed for the optimization. Such model is proposed in this report. It differs from the commonly used traditional model of the field, which can be applied when profiles of the vanes are described by the harmonic functions of the longitudinal coordinate. Our model is more general and can be applied for arbitrary profiles of the vanes.",
author = "Drivotin, {O. I.} and Dulatov, {I. T.}",
year = "2016",
month = jan,
day = "1",
language = "English",
series = "25th Russian Particle Accelerator Conference, RuPAC 2016",
publisher = "JACoW",
pages = "244--246",
booktitle = "25th Russian Particle Accelerator Conference, RuPAC 2016",
address = "Switzerland",
note = "25th Russian Particle Accelerator Conference, RuPAC 2016, RuPAC 2016 ; Conference date: 21-11-2016 Through 25-11-2016",

}

RIS

TY - GEN

T1 - A simple model for electromagnetic field in RFQ channel

AU - Drivotin, O. I.

AU - Dulatov, I. T.

N1 - Conference code: XXV

PY - 2016/1/1

Y1 - 2016/1/1

N2 - Numerical solution of the RFQ structure optimization problem requires a great amount of computation. Each consecutive step of the numerical optimization includes modification of geometry of the channel and computation of electromagnetic field for modified geometry. Therefore, a simple model describing the field in the channel is needed for the optimization. Such model is proposed in this report. It differs from the commonly used traditional model of the field, which can be applied when profiles of the vanes are described by the harmonic functions of the longitudinal coordinate. Our model is more general and can be applied for arbitrary profiles of the vanes.

AB - Numerical solution of the RFQ structure optimization problem requires a great amount of computation. Each consecutive step of the numerical optimization includes modification of geometry of the channel and computation of electromagnetic field for modified geometry. Therefore, a simple model describing the field in the channel is needed for the optimization. Such model is proposed in this report. It differs from the commonly used traditional model of the field, which can be applied when profiles of the vanes are described by the harmonic functions of the longitudinal coordinate. Our model is more general and can be applied for arbitrary profiles of the vanes.

UR - http://www.scopus.com/inward/record.url?scp=85058694980&partnerID=8YFLogxK

M3 - Conference contribution

AN - SCOPUS:85058694980

T3 - 25th Russian Particle Accelerator Conference, RuPAC 2016

SP - 244

EP - 246

BT - 25th Russian Particle Accelerator Conference, RuPAC 2016

PB - JACoW

T2 - 25th Russian Particle Accelerator Conference, RuPAC 2016

Y2 - 21 November 2016 through 25 November 2016

ER -

ID: 41030298