• Title/Summary/Keyword: Pulse width

Search Result 1,790, Processing Time 0.031 seconds

Output Characteristics of a Flashlamp pumped Nd:YAG Lasers at 1.444 nm (플래시 램프로 펌핑한 Nd:YAG 레이저의 $1.444{\mu}m$ 출력 특성)

  • Lee, Hee-Chul;Kim, Gyu-Ug;Kim, Dong-Hyun;Gong, Sung-Hwan;Kim, Yong-Pyung
    • The Transactions of the Korean Institute of Electrical Engineers C
    • /
    • v.55 no.12
    • /
    • pp.606-610
    • /
    • 2006
  • We investigated the output characteristics of Nd:YAG lasers at wavelength of 1444 nm, which were pumped by 450 Xe-flashlamp, 700 torr Xe-flashlamp and 700 torr Kr-flashlamp. With a Xe-flashlamp of 700 torr of gas pressure, the pulse energy of 0.738 J was obtained with repetition rate of 9.16 Hz and pumping pulse width of 400 ms. In case pumping pulse width of 5 ms and repetition rate of 1 Hz, 700 torr Kr-flashlamp showed the highest pulse energy of 1.44 J.

Design of X-Band High Efficiency 60 W SSPA Module with Pulse Width Variation (펄스 폭 가변을 이용한 X-대역 고효율 60 W 전력 증폭 모듈 설계)

  • Kim, Min-Soo;Koo, Ryung-Seo;Rhee, Young-Chul
    • The Journal of Korean Institute of Electromagnetic Engineering and Science
    • /
    • v.23 no.9
    • /
    • pp.1079-1086
    • /
    • 2012
  • In this paper, X-band 60 W Solid-State Power Amplifier with sequential control circuit and pulse width variation circuit for improve bias of SSPA module was designed. The sequential control circuit operate in regular sequence drain bias switching of GaAs FET. The distortion and efficiency of output signals due to SSPA nonlinear degradation is increased by making operate in regular sequence the drain bias wider than that of RF input signals pulse width if only input signal using pulsed width variation. The GaAs FETs are used for the 60 W SSPA module which is consists of 3-stage modules, pre-amplifier stage, driver-amplifier stage and main-power amplifier stage. The main power amplifier stage is implemented with the power combiner, as a balanced amplifier structure, to obtain the power greater than 60 W. The designed SSPA modules has 50 dB gain, pulse period 1 msec, pulse width 100 us, 10 % duty cycle and 60 watts output power in the frequency range of 9.2~9.6 GHz and it can be applied to solid-state pulse compression radar using pulse SSPA.

Evaluation of reactor pulse experiments

  • I. Svajger;D. Calic;A. Pungercic;A. Trkov;L. Snoj
    • Nuclear Engineering and Technology
    • /
    • v.56 no.4
    • /
    • pp.1165-1203
    • /
    • 2024
  • In the paper we validate theoretical models of the pulse against experimental data from the Jozef Stefan Institute TRIGA Mark II research reactor. Data from all pulse experiments since 1991 have been collected, analysed and are publicly available. This paper summarizes the validation study, which is focused on the comparison between experimental values, theoretical predictions (Fuchs-Hansen and Nordheim-Fuchs models) and calculation using computational program Improved Pulse Model. The results show that the theoretical models predicts higher maximum power but lower total released energy, full width at half maximum and the time when the maximum power is reached is shorter, compared to Improved Pulse Model. We evaluate the uncertainties in pulse physical parameters (maximum power, total released energy and full width at half maximum) due to uncertainties in reactor physical parameters (inserted reactivity, delayed neutron fraction, prompt neutron lifetime and effective temperature reactivity coefficient of fuel). It is found that taking into account overestimated correlation of reactor physical parameters does not significantly affect the estimated uncertainties of pulse physical parameters. The relative uncertainties of pulse physical parameters decrease with increasing inserted reactivity. If all reactor physical parameters feature an uncorrelated uncertainty of 10 % the estimated total uncertainty in peak pulse power at 3 $ inserted reactivity is 59 %, where significant contributions come from uncertainties in prompt neutron lifetime and effective temperature reactivity coefficient of fuel. In addition we analyse contribution of two physical mechanisms (Doppler broadening of resonances and neutron spectrum shift) that contribute to the temperature reactivity coefficient of fuel. The Doppler effect contributes around 30 %-15 % while the rest is due to the thermal spectrum hardening for a temperature range between 300 K and 800 K.

A Study on The PWM Control of Resonant Inverters (공진형 인버터의 PWM 제어에 관한 연구)

  • Shin, Jae-Hwa;Cho, Kyu-Min;Kim, Young-Seok
    • Journal of the Institute of Electronics Engineers of Korea SC
    • /
    • v.38 no.1
    • /
    • pp.53-60
    • /
    • 2001
  • In many applications of power electronics, high frequency resonant inverters are used, and the PAM(Pulse Amplitude Modulation), PFM(Pulse Frequency Modulation) or PWM(Pulse Width Modulation) techniques are used to control the output power of resonant inverters. And the resonant inverters have to control the output frequency for the reliable operation under the variable load conditions. In this paper, a new switching scheme is proposed as a PWM control of resonant inverters. With the proposed method, it can be obtained that optimum resonant frequency and unity output displacement factor under the variable resonant frequency adaptively. The detail algorithm or the proposed PWM switching scheme and its output characteristics are discussed. And the veridity of the proposed method is confirmed with the experimental results.

  • PDF

Optimal Characteristics of a Long-pulse $CO_2$Laser by Controlling SCR Firing Angle in AC Power Line

  • Noh, Ki-Kyung;Kim, Geun-Yong;Chung, Hyun-Ju;Min, Byoung-Dae;Song, Keun-Ju;Kim, Hee-Je
    • KIEE International Transactions on Electrophysics and Applications
    • /
    • v.2C no.6
    • /
    • pp.304-308
    • /
    • 2002
  • We demonstrate a simple pulsed $CO_2$ laser with millisecond long pulse duration in a tube at a low pressure of less than 30 Torr. The novel power supply for our laser system switches the voltage of the AC power line (60Hz) directly. The power supply doesn't need elements such as a rectifier bridge, energy-storage capacitors, or a current-limiting resistor in the discharge circuit. To control the laser output power, the pulse repetition rate is adjusted up to 60Hz and the firing angle of SCR(Silicon Controlled Rectifier) gate is varied from 30。 to 150。. A ZCS (Zero Crossing Switch) circuit and a PIC one-chip microprocessor are used to control precisely the gate signal of the SCR. The maximum laser output of 35 W is obtained at a total pressure of 18 Torr, a pulse repetition rate of 60 Hz, and a SCR gate firing angle of 90。 . In addition, the resulting laser pulse width is approximately 3㎳(FWHM). This is a relatively long pulse width, compared with other repetitively pulsed $CO_2$ lasers.

VOLTAGE CONTROLLED PULSE WIDTH MODULATOR

  • Rahman, Md. Fayzur;Lee, Kwang-Sik;Lee, Dong-In
    • Proceedings of the KIEE Conference
    • /
    • 1997.07f
    • /
    • pp.2200-2203
    • /
    • 1997
  • This paper presents a model for p voltage controlled pulse width modulator (VCPWM), which can be used in any phase controlled converter having either manual or microprocessor based control. The circuit uses only one 555 timer, an OpAmp, some resistors, and capacitors. Although a large varieties of such circuits are available in the literature, this model is very simple with low cost and high performance.

  • PDF

New Driving Method for Fast Addressing of AC-Plasma Display Panel

  • Kim, Gun-Su;Choi, Hoon-Young;Lee, Seok-Hyun;Seo, Jeong-Hyun
    • 한국정보디스플레이학회:학술대회논문집
    • /
    • 2003.07a
    • /
    • pp.726-729
    • /
    • 2003
  • A new driving method is proposed to reduce the address period. The scan time of new driving method overlaps with the next scan time during the discharge lag time. Thus, without reducing the address pulse width and the scan pulse width, the new addressing method can reduce the address period. The results show that the scan time of about 100ns ${\sim}$ 300ns can be overlapped without the misfiring,.

  • PDF

Sliding Mode Control for Attitude Tracking of Thruster-Controlled Spacecraft

  • Cheon, Yee-Jin
    • Transactions on Control, Automation and Systems Engineering
    • /
    • v.3 no.4
    • /
    • pp.257-261
    • /
    • 2001
  • Nonlinear pulse width modulation (PWM) controlled system is considered to achieve control performance of thruster controlled spacecraft. The actual PWM controlled motions occur, very closely, around the average model trajectory. Furthermore nonlinear PWM controller design can be directly applied to thruster controlled spacecraft to determine thruster on-time. Sliding mode control for attitude tracking of three-axis thruster-controlled spacecraft is presented. Simulation results are shown which use modified Rodrigues parameters and sliding mode control law to achieve attitude tracking of a three-axis spacecraft with thrusters.

  • PDF

PWM(Pulse Width Modulation) Circuit Using OTA (OTA를 이용한 PWM(Pulse Width Modulation) 회로)

  • 송재훈;김희준;정원섭
    • Proceedings of the IEEK Conference
    • /
    • 2002.06e
    • /
    • pp.247-250
    • /
    • 2002
  • This paper proposes a PWM circuit using CMOS OTAs. The features of the proposed PWM circuit are IC oriented circuits, simple configuration, and bias current controlled output. In order to verily the validity of the proposed circuit, it is simulated by H-SPICE program. Futhermore, the proposed circuit is integrated on chip using 0.35 $\mu\textrm{m}$ CMOS technology.

  • PDF

A Distortionless Digital PWM Implementation by means of a Non-integer delay FIR filtering (소수형 디지털연산 알고리즘을 이용한 디지털 PWM의 고유한 비선형특성의 보상)

  • 정진훈;정동호
    • Proceedings of the IEEK Conference
    • /
    • 2003.07e
    • /
    • pp.2427-2430
    • /
    • 2003
  • A uniformly sampled digital pulse-width modulation adopting a pre-compensation filter scheme for applications in high-resolution digital-to-analog data conversion is described. It is shown that linearization of the intrinsic distortion resulting in uniformly sampled pulse-width modulation can be achieved by using a non-integer delay digital filter embedded within a noise shaping re-quantizer.

  • PDF