Second Harmonic TE21 Gyrotron Backward Wave Oscillator
碩士 === 南台科技大學 === 電機工程系 === 92 === The gyrotron backward wave oscillator (gyro-BWO) is a promising source of coherent millimeter wave radiation based on the electron maser instability on a backward waveguide mode. However, a high magnetic field requirement limit on its applicability as a millimeter-...
Main Authors: | , |
---|---|
Other Authors: | |
Format: | Others |
Language: | zh-TW |
Published: |
2004
|
Online Access: | http://ndltd.ncl.edu.tw/handle/42474045171733932471 |
id |
ndltd-TW-092STUT0442017 |
---|---|
record_format |
oai_dc |
spelling |
ndltd-TW-092STUT04420172016-11-22T04:12:28Z http://ndltd.ncl.edu.tw/handle/42474045171733932471 Second Harmonic TE21 Gyrotron Backward Wave Oscillator 二次諧波TE21磁旋返波振盪器 Ting-Shu Wu 吳庭旭 碩士 南台科技大學 電機工程系 92 The gyrotron backward wave oscillator (gyro-BWO) is a promising source of coherent millimeter wave radiation based on the electron maser instability on a backward waveguide mode. However, a high magnetic field requirement limit on its applicability as a millimeter-wave source. The required magnetic field is reduced by the harmonic operation in this project. The harmonic gyrotron backward-wave oscillator not only has the feature of the frequency tuning using by the applied magnetic field and beam voltage, but also has the low applied magnetic field and high beam current. A comparative analysis between the fundamental and second cyclotron harmonics of gyrotron backward-wave oscillators (gyro-BWOs) is analyzed presented. The simulation results reveal that the nonlinear field contraction is a common feature for both harmonics interactions. Besides, the electron transit angle, used to characterize the axial modes of the fundamental harmonic TE11 mode at the start-oscillation conditions, is found to be applicable even for the second harmonic TE21 mode. Each axial mode of either the fundamental harmonic TE11 or the second harmonic TE21 modes is maintained at a constant value of the electron transit angle while changing the operating parameters, such as magnetic field and beam voltage. Extensive numerical calculations have been conducted for the starting currents and tuning properties. A single-mode operating regime is suggested where the second harmonic TE21 gyro-BWO is stable with a decent output power, comparing with the fundamental harmonic TE11 gyro-BWO. Yi Sheng Yeh 葉義生 2004 學位論文 ; thesis 64 zh-TW |
collection |
NDLTD |
language |
zh-TW |
format |
Others
|
sources |
NDLTD |
description |
碩士 === 南台科技大學 === 電機工程系 === 92 === The gyrotron backward wave oscillator (gyro-BWO) is a promising source of coherent millimeter wave radiation based on the electron maser instability on a backward waveguide mode. However, a high magnetic field requirement limit on its applicability as a millimeter-wave source. The required magnetic field is reduced by the harmonic operation in this project. The harmonic gyrotron backward-wave oscillator not only has the feature of the frequency tuning using by the applied magnetic field and beam voltage, but also has the low applied magnetic field and high beam current.
A comparative analysis between the fundamental and second cyclotron harmonics of gyrotron backward-wave oscillators (gyro-BWOs) is analyzed presented. The simulation results reveal that the nonlinear field contraction is a common feature for both harmonics interactions. Besides, the electron transit angle, used to characterize the axial modes of the fundamental harmonic TE11 mode at the start-oscillation conditions, is found to be applicable even for the second harmonic TE21 mode. Each axial mode of either the fundamental harmonic TE11 or the second harmonic TE21 modes is maintained at a constant value of the electron transit angle while changing the operating parameters, such as magnetic field and beam voltage. Extensive numerical calculations have been conducted for the starting currents and tuning properties. A single-mode operating regime is suggested where the second harmonic TE21 gyro-BWO is stable with a decent output power, comparing with the fundamental harmonic TE11 gyro-BWO.
|
author2 |
Yi Sheng Yeh |
author_facet |
Yi Sheng Yeh Ting-Shu Wu 吳庭旭 |
author |
Ting-Shu Wu 吳庭旭 |
spellingShingle |
Ting-Shu Wu 吳庭旭 Second Harmonic TE21 Gyrotron Backward Wave Oscillator |
author_sort |
Ting-Shu Wu |
title |
Second Harmonic TE21 Gyrotron Backward Wave Oscillator |
title_short |
Second Harmonic TE21 Gyrotron Backward Wave Oscillator |
title_full |
Second Harmonic TE21 Gyrotron Backward Wave Oscillator |
title_fullStr |
Second Harmonic TE21 Gyrotron Backward Wave Oscillator |
title_full_unstemmed |
Second Harmonic TE21 Gyrotron Backward Wave Oscillator |
title_sort |
second harmonic te21 gyrotron backward wave oscillator |
publishDate |
2004 |
url |
http://ndltd.ncl.edu.tw/handle/42474045171733932471 |
work_keys_str_mv |
AT tingshuwu secondharmonicte21gyrotronbackwardwaveoscillator AT wútíngxù secondharmonicte21gyrotronbackwardwaveoscillator AT tingshuwu èrcìxiébōte21cíxuánfǎnbōzhèndàngqì AT wútíngxù èrcìxiébōte21cíxuánfǎnbōzhèndàngqì |
_version_ |
1718396157385768960 |