峰值輸出功率 的英文怎麼說

中文拼音 [fēngzhíshūchūgōng]
峰值輸出功率 英文
maximum output
  • : Ⅰ名詞1. (山的突出的尖頂) peak; summit 2. (形狀像山峰的事物) peak-like thing Ⅱ量詞(用於駱駝)
  • : Ⅰ動詞1 (運輸; 運送) transport; convey 2 [書面語] (捐獻) contribute money; donate 3 (失敗) l...
  • : 名詞1 (功勞) exploit; merit; meritorious service [deed]: 戰功 military exploits; 立功 render me...
  • : 率名詞(比值) rate; ratio; proportion
  • 輸出 : 1 (從內部送到外部) export 2 [電學] output; outcome; outlet; out fan; fanout; 輸出變壓器 output ...
  1. We apply the agrawal ' s theory model of soa, and study the temporal characteristics of the output pulse for input picosecond optical pulses with different sharpness edges passing through a semiconductor optical amplifier, and find that the peak power and the pulse width of the output pulse depend on the input pulse peak power, the sharpness degree of the input pulse edge and the bias current of soa

    本文應用agrawal的關于soa理論模型,詳細研究了具有不同陡峭邊沿的皮秒超高斯光脈沖經soa后的時域特性的變化,發現脈沖的、脈沖寬度與入脈沖的入脈沖邊沿的陡峭程度以及soa的偏置電流密切相關。
  2. Two, the worth music of output the power pmpo

    音樂pmpo
  3. Advanced peak detector automatic cutoff with mosfet and linear current charges battery to 100 % without overcharging

    高級檢測器自動以切斷和線性電流保證電池能被100 %充滿而不會導致過沖。
  4. Some researches about frequency doubling are made, and two methods to improve intensity of second frequency generation are given. we realized q - switched 532 nm laser, by using nd : gdvo4 as laser crystal, using cr4 + : yag as saturable absorber, using ktp as intra - cavity frequency doubling crystal. average power of 109mw, repetition of 40khz, pulse width of 30ns, pulse energy of 2. 6uj, peak power of 91w are obtained

    4 .對倍頻理論進行研究和分析:討論兩種提高二次諧波密度的方一法;實驗匕在國內首次實現ld端面泵浦nd : gdvo4 / ktp ,用cr4 + : yag作為可飽和吸收片的綠光激光器,腔內倍頻得到了平均為109mw 、重復頻為40khz 、脈寬為3ons 、單脈沖能量為2 . 6閃、為glw的調q綠光
  5. The nonuseful loss of cavity were got by measuring the threshold of laser under the different output mirrors. the loss was caused by prague angle unmatching. 3. the pulse train with minor pulse width 22ns and frequency 23khz, peak power 3. 5kw were obtained in cr4 " : yag passively q - switch experience. the stability of pulse is 6 %

    ( 3 )實現了在大泵浦、無水冷的情況下cr ~ ( 4 + ) : yag飽和吸收體被動調q ,得到了最小脈寬為22ns 、重復頻為23khz 、為3 . 5kw的激光脈沖,脈沖的穩定性為6 。
  6. Using the variational method, analytical conditions for stationary pulse propagation in dense period fibers with strong dispersion management are deduced. the expression of initial soliton peak power is given. by employing the obtained formulas, the soliton evolution semi - analytically in various dispersion maps can be investigated. effects of the third order dispersion are also studied in this paper. the results show that imperfect dispersion slope compensation can cause pulse central position shift and even serious degradation of soliton shape

    利用變分方法,推導了在強色散管理的密集周期光纖中脈沖穩態傳的解析條件,並給了初始脈沖的表達式.運用這些公式,對各種色散管理系統中孤子的演化進行了半解析的考察.三階色散也被考慮在內.結果表明:不完善的色散斜補償將導致脈沖中心位置的偏移甚至嚴重的孤子形狀劣化
  7. The motor has a normal maximum power of 180kw and a peak output of 230kw. external feeds are arranged to the inverter from ( i ) the accelerator pedal, ( ii ) the forwardreverse selector, and ( iii ) the brake pedal, in order to determine power demand, direction of travel ( forwards or backwards ) and brake regeneration

    馬達一般最大為一百八十仟瓦及二百三十仟瓦。外來訊號經由i )油門踏板ii )前後波掣及iii )剎車踏板,傳至轉換器以決定所需、行車方向(前或后)及剎車效能之再生等等。
  8. The third, some groping researches are made on broadband coaxial line filter output circuit of klystron. a broadband output circuit - mode four coupling slots double - gap output cavity loaded with coaxial filter, which has a workable relative bandwidth bigger than 14 % and fits in with l - band multi - beam klystron, is designed. meanwhile some analysis of its stability and peak power capacity is made

    第三,對速調管同軸線濾波器寬帶迴路進行研究和探索,設計了一個適合用於l波段多注速調管、相對帶寬超過14的四耦合槽模強耦合雙間隙腔加載同軸線濾波器迴路,並對其穩定性和容限做了一些分析。
  9. From the theoretical calculation and the experimental results, we makehe conclusion that the last cavity setup is most suitable for the wavelength tuning. we calculated the stable regions and the peak power on the sesam, at the same time, ave the beam size on the sesam and on the crystal. we achieved the q - switchedutput with a three - mirror folded - cavity after optimizing it

    計算了v型腔和五鏡腔的穩區、晶體和sesam上光斑半徑、 sesam上的密度,對腔的參數進行了優化,並做了sesam被動調q和鎖模的激光實驗,實現了v型腔調q 、五鏡腔調q的激光
  10. Based on this arithmetic, the high frequency characteristics of five - cavity with open boundary is calculated by the code written in fortran language. then the transit effect of five modes of five - cavity with open boundary is also calculated using code mathcad and matlab. the results show that the working mode of five - cavity transit tube oscillator is 3 / 6 mode, and the analysis of the theory are in good agreement with the simulation results

    根據從基於四腔渡越時間效應的自調制發,經過一段飄移,然後再採用雙間隙提取腔邊耦合微波的思路,採用粒子模擬方法優化設計一種為1 . 5gw ,頻為9 . 3ghz的六腔渡越輻射振蕩器,並研究了它的一系列工作特性。
  11. The simulation results show the existence of both limits and optima for the studied parameters, related to the stable operation and the maximum efficiency, respectively. underlying the conditions that the longitudinal guiding magnetic field is 1. 8t, diode voltage is 250 kv, the impedance is 150, we got a peak power as high as 100 mw for the tm01 mode at 38ghz

    經優化設計,本文給了一個相對論亞納秒毫米波返波振蕩器的物理模型,在引導磁場為1 . 8t 、二極體電壓為250kv 、阻抗為150的情況下得到了超輻射狀態下微波為100mw 、中心頻為38ghz 、模式為tm _ ( 01 )模的微波輻射。
  12. Presently, the laser pulse from the high power ultrashort laser system is several femtoseconds in duration, tw ( or pw ) level in peak power, 1020 w / cm2 ( or 1021 w / cm2 ) in focusing power density, according electric field is much stronger than coulomb field in atoms

    目前,高超短脈沖激光放大系統的激光,脈寬達到幾個飛秒,達到太瓦甚至拍瓦量級,聚焦密度達10 ~ 20w cm ~ 2 ,甚至1021w cm2 ,相應的電場比原子內庫侖場強得多。
  13. Different distribution of power loss can be worked out by mathcad software based on the formula reasoning. the result of calculation is consistent with that of the experiment, which proves that this method is right. it is pointed out through the analysis of calculating data that the key to improve efficiency at the same output power is to decrease the peak current and rms current of power switches or the on - resistance of mosfet and windings

    由推導可得損耗計算公式,利用數學計算軟體計算電路從空載到410w阻性負載時損耗分佈變化,該結果與實驗數據基本相吻合,證實了這種方法的正確性;通過對計算數據的分析,指了進一步提高效的關鍵在於相同時降低管的電流和有效,減小繞組和mosfet的導通電阻。
  14. The simulation results of the 2. 5 - d pic code for this new structure are presented. a 2. 5 gw peak output power with the frequency of l. 3ghz is generated with the input of 625kv voltage, dc input power of 18gw

    然後對這種器件進行了數模擬研究,得到的典型結果為:入電壓625kv ,入直流18gw ,微波為2 . sgw ,虛陰極振蕩頻被鎖定,微波飽和時間小於sns ,頻為1 . 3ghz 。
  15. Simulation results show 2. 5 gw output power with a frequency of 1. 25ghz can be generated with an input of 620kv voltage, dc input power of 10. 5gw electron beam. ( 3 ) the radial reflex klystron with an open foldaway - concentric cylindrical resonant cavity integrates the resonant cavity and reflex cavity within one foldaway coaxial cavity, so it is a very compact high power microwave device

    然後對這種器件進行了數模擬研究,得到的典型結果為:入電壓620kv ,入直流io . sgw ,微波為2 . sgw ,虛陰極振蕩頻被鎖定,頻為1 . 25ghz ,微波飽和時間小於sns 。
  16. Analytical formulas for the peak power, pulse energy, pulse width, energy extraction efficiency, repetition rate and average output power are derived

    計算了自調q脈沖的,單脈沖能量,脈沖寬度,能量利用,重復頻,平均等。
  17. Pmpo peak music power output

    音樂
  18. It has been presented in this dissertation that using model of q modulated er - glass laser, through replacing typical number of er - doped fiber and single mode fiber into the model, then the theoretical model of self - q - switching by sbs was established. by emulating experiment, the peak value of output power, repeating frequency, width of pulse have been calculated. the data was calculated repeatedly when the length of er - doped fiber changing

    將摻鉺光纖和單模光纖的典型數據代入該模型中,進行模擬實驗研究得sbs自調q光纖激光器、脈寬、重頻等數據,並在改變摻鉺光纖長度的情況下,再次進行模擬實驗,對上述結果進行了分析。
  19. In this paper, after adopting the plane wave approximation, taking into account the fact that the output from a fabry - perot is formed on the basis of the interference of the multi - reflected beams of the input pulse that enters the filter, an analytical expression of the output pulse intensity has been derived

    本文推導了高斯型光脈沖經過濾波器后脈沖的時域表達式。在此基礎上,對射脈沖的、脈沖寬度以及濾波器對入射脈沖的時延等進行了深入的研究。
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