【機械類畢業(yè)論文中英文對照文獻翻譯】CO2激光熔透焊接時工件上及焊縫內(nèi)光致等離子體體的特性【PDF英文5頁word中文翻譯1149字3頁】【有出處】
【機械類畢業(yè)論文中英文對照文獻翻譯】CO2激光熔透焊接時工件上及焊縫內(nèi)光致等離子體體的特性【PDF英文5頁word中文翻譯1149字3頁】【有出處】,機械類畢業(yè)論文中英文對照文獻翻譯,PDF英文5頁,word中文翻譯1149字3頁,有出處,機械類,畢業(yè)論文,中英文,對照,對比,比照,文獻,翻譯,co2,激光,焊接,工件,焊縫,內(nèi)光致,等離子體,特性
外文資料翻譯2激光熔透焊接時工件上及焊縫內(nèi)光致等離子體體的特性段愛琴,陳俐,鞏水利摘要:在此論文中,用一個高速攝像機和一個光學(xué)放射監(jiān)視器來探究激光熔透焊接不銹鋼時光致等離子體的特性。透過光致等離子體光學(xué)發(fā)散的結(jié)果顯示其存在兩個特有頻段,它們分別是100-500HZ和1500-3500HZ。與此同時,光致等離子體和熔池的不斷變化的圖像也顯示了其存在兩個不穩(wěn)定的頻率段。其中一個不穩(wěn)定的頻段顯示出焊縫內(nèi)光致等離子體的特性,它處于167-500HZ之間,另一個不穩(wěn)定的頻段則位于1500-3500HZ之間,這顯然是由保護氣體引起的。某些因素可能會導(dǎo)致焊縫等離子和保護氣體等離子之間頻率的差異,其中的一個原因就是焊縫內(nèi)光致等離子體的壓力會慢慢地增長。關(guān)鍵詞:激光焊接,光致等離子體,焊縫,頻段0 序言如今,激光焊接 已經(jīng)廣泛應(yīng)用于許多領(lǐng)域,例如航空航天零部件的激光焊接 。然而,由于特殊的應(yīng)用環(huán)境它需要更高的焊接質(zhì)量。尤其是,保證長焊縫或復(fù)雜的部件的焊接質(zhì)量被證明是很難的,因為金屬的激光焊接本身就是一個不穩(wěn)定的過程。全世界已經(jīng)有許多關(guān)于焊接穩(wěn)定性的研究?;仡櫱懊娴难芯砍晒?,就能看出大部分焊接質(zhì)量的不穩(wěn)定是由于不穩(wěn)定的焊接過程引起的,尤其在激光焊接中,主要的原因就是光致等離子導(dǎo)致焊接穩(wěn)定性很難控制。在激光深熔焊接中,光致等離子是一種重要的物理現(xiàn)象。因為焊縫和熔池難以直接觀察,所以大部分關(guān)于激光焊接過程的研究都集中于能夠間接地顯示焊縫和熔池運動的光致等離子身上。例如,許多關(guān)于光致等離子的研究都通過它的光傳播和聲音傳播來監(jiān)測焊縫的缺陷。然而,光致等離子的物理性能還沒有引起足夠的重視。例如,焊縫中光致等離子的不穩(wěn)定頻段是否和被加工工件的相同,焊縫中的光致等離子有怎樣的組成和運動等等。實際上,所有這些基本問題不是很清楚。本文介紹了用高速攝像機和光學(xué)放射監(jiān)視器對激光焊接中光致等離子的研究。1材料及焊接工藝在這個研究中,實驗材料是304不銹鋼,厚度為2毫米。激光焊接是利用4kW快速軸流Q型激光實現(xiàn)的光致等離子體和熔池的圖像是通過帶有精密光學(xué)濾波器的幻影V4.1高速相機拍攝到的。激光是通過一個特別的激光監(jiān)控系統(tǒng)計算獲得的。在整個激光焊接加工過程中氬被用來作為同軸保護氣體。2結(jié)果和討論在304不銹鋼激光焊接過程中,典型的頻譜由光致等離子體顯示在圖1中。圖1波長/nm這表明,光譜成分的范圍大多是400-700納米氬。而較高強度的譜線波長都在400-600納米范圍內(nèi)。這些結(jié)果顯示波動范圍從400納米到600納米的光學(xué)發(fā)射信號的波動特性可用來描述波動光致等離子體。實驗數(shù)據(jù)顯示在這個變動范圍的波長的相對強度的發(fā)射光的波動具有周期性,并且,已有的研究結(jié)果也表明他在一個不穩(wěn)定的周期中波動??焖俑道锶~變換(FFr)技術(shù)是一種有用的分析信號頻率的方法,因此在本文中被用來識別焊接工藝的特征頻率。FFTCO2激光焊接304不銹鋼的光學(xué)發(fā)射頻譜是圖2。圖2頻率/HZBehavior of vaporplasma within the keyhole and above the workpiece during CO2 laser penetration welding 7 Behavior of vaporplasma within the keyhole and above the workpiece during CO2 laser penetration welding Duan Aiqin,Chen Li and Gong Shuili 段愛琴,陳俐,鞏水利 Abstract In this paper,a highspeed camera and an optical emission monitor were used to study the behavior of vapor plasma during CO2 laser welding of SUS304 stainless stee1Results of optical emission from vaporplasma show that two characteristicfrequency bands exist,100500 Hz and 1 5003 500 HzAt the same time,the changing images ofvapor plasma and bottom pool also confirm that there are two different fluctuation frequency bandsOne of the frequency bands represents the characteristic of vaporplasma within the keyhole,and it is within 167500 HzAnother frequency band is within 1 5003 500 Hz,and it obviously derives from the shielding gasSome factors may cause these frequency differences between the keyhole plasma and the shielding gas plasmaOne of them is that the vaporplasma pressure within the keyhole will ncrease slowly Key words CO2 laser welding,vaporplasma,keyhole,frequency 0 Intr0ductiOn Nowadays,laser welding has been widely used in many fields,such as laser welding of aerospace compo nentsHowever,it needs much higher weld quality be cause of their applied conditionsEspecially,maintaining stability of weld quality for long welds or complex compo nents proves to be difficult,for laser welding of metal is an inherent unstable processThere have been many studies about welding process stability all over the worldRevie wing published study results,it can be found that most of weld quality instabilities can be caused by unstable weld ing processes,especially in CO2 laser weldingThe main reason is that vaporplasma makes stability control diffi culty 一 Vaporplasma is a sort of important physical phenom enon during laser penetration weldingBecause the key hole and molten pool are difficult to be directly observed, most of studies about laser welding processes concentrated on vaporplasma,which can indirectly show the movement of the pool and the keyhole3-41 In addition,many stud ies about vaporplasma have been relative to monitoring weld imperfection by optical emission and acoustic emis sion from vaporplasmaHowever,physical features of va porplasma have not been paid a sufficient attentionFor instance,whether the fluctuation frequency of vaporplas ma within the keyhole is as same as that above the work- piece,how vaporplasma within the keyhole forms and e jects,and so onIn fact,all these fundamental questions are not quite clear This paper presents the study of vaporplasma during CO2 laser welding by highspeed camera and optical emis sion monitor 1 Materials and welding procedure In this study,the experimental material was SUS304 stainless steel with thickness of 2 mmThe laser welding performed using a 4 kW fast axial flow Qmode CO2 laser The images of vaporplasma and molten pool were cap tured by a Phantom V41 high-speed camera with narrow optical filtersThe optical emission was acquired and cal culated by a special plasma monitoring systemAr was used as coaxial gas shielding during laser welding process一 Duan Aiqin,Chen Li and Gong Shuili,National Key Laboratory for High Density Beam Processing Technology,Beijing Aeronautical Manufacturing Research Institute,Beijing,100024 Email:duanaiqintomcorn(Duan Aiqin) CHINA WELDING Vo117 No4 December 2008 2 Results and discussion During CO2 laser welding of SUS304 stainless steel, the typical spectrum from vaporplasma is shown in Fig1This shows that the spectral components in the range of 400700 nm are mostly lines of Ar 11And spec tral lines with higher intensity are within wavelength 400 600 nmThese resuIts show that the fluctl】atinn haracter 50 000 40 000 皇 30 000 嘗20 000 10 000 O istic of optical emission signals of range from 400 nm to 600 nm can describe fluctuation of vaporplasmaExperi mental data had shown that relative intensities of optical e mission in such range of wavelength fluctuate periodically, and published study results also confirmed that it chan ges at an unstable periodicity Ar50 5-204 Ar 5017164, 509 05 Ar | 514178 _ IJ 1 11 I 1 J4 1 l L一一I一卜I J 400 450 500 550 600 650 700 Wavelengthnm Fig1 Spectrum of CO2 laser welding of stainless steel(Laser power 1 650 W and welding speed 1 mmin) Fast Fourier transform(FFr)technique is an useful method that analyzes frequencies of signals,so it was used for identifying characteristic frequency of welding proces ses in this paperF盯spectrum of optical emission during CO2 laser welding of SUS304 stainless steel is given in Fig2It is found that the frequency components of vapor plasma are quite complex and have not a dominant fre quency componentHowever,two characteristic frequency bands exist,one is 100500 Hz(range A)and the other is 1 5003 500 Hz(range B)Infrared(IR:1564 nm)e inission from the welding process can indirectly reveal the radiation of heatThis radiation mostly comes from vapor plasma and molten poo1Fig3 is the raw timedependent 謄g SE+3 茸+3 3K3 2K43 111+3 I卜2 curve of IR optical emission measured during the same process as Fig2This diagram obviously reflects that the IR emission can be separated into fluctuation component and invariable componentIt has been known that the heat radiation from molten pool only changes with the size and temperature of molten poo1And it also has been well demonstrated that,for a stable process,the size and tern- perature of molten pool are almost constant。 So FFT spectrum of IR emission by a 1006 000 Hz band-pass filter is mainly correlated to heat radiation from vapor plasma,as shown in Fig4Both Fig2 and Fig4 have almost the same distributions of frequenciesHowever, their intensities are quite differentFor the IR emission, FrequencyHz Fig2 FFT spectrum of 400600 am optical emission from vaporplasma(Laser power 1 650 W and welding speed 1 mmin) 一 一 審_f0 Behavior of vaporplasma within the keyhole and ab。ve the workpiece during CO 2 laser penetration welding 9 ; 蚤I 。 , | l 一一一一 一一 f Sample position Fig3 Time dependence of IR emission from vaporplasma(Laser power 1 650 W and welding speed 1 mmin) FrequencyHz Fig4 FFT spectrum of IR emission from vaporplasma(Laser power l 650 W and welding speed 1 mmin1 intensity within the range A(100500 rlz)is two times as strong as that within the range B(1 5003 500 Hz)But for 400600 nm optical emission ,intensity within the range A is nearly the same as that within the range BIt can be concluded that there are two different processes and their fluctuation frequencies are within the range A and B respectivelyThe process correlated with the range A has obvious heat effect,but the process correlated with the range B shows obviously irradiance phenomenon Two kinds of vaporplasmas were observed above the workpieee through the highspeed camera with a narrow (a)Two kinds of vaporplasmas filterTheir fluctuation frequencies are obviouslv differ entFig5 shows several typical images of two kinds of va porplasmasFig5a presents simultaneously two vapor plasmas,C area is Ar plasma image and D area is vapor plasma image from the keyhole But in Fig5bthere is only the Ar plasma to be discovered Howeverin Fig5c,the Ar plasma completely disappears and only the vaporplasma from the keyhole is observed Therefore it could be thought that vaporplasmas consist of two differ ent parts deriving from the keyhole and shielding gas re spectivelyCompared with the results of optical emission , (b)Ar plasma (C)Keyhole vapodplasma Fig5 Different states of the vaporplasmas(Laser power 1 650 W and welding speed 1 mmin 1 皇 0葛一0 0 占一 葛一 A1 一0 CHINA WELDING Vo11 7 No4 December 2008 the two different frequency range A and B are obviously caused by these two different vaporplasmasThe follow ing question is which characteristic frequency band repre sents the vaporplasma within the keyhole Changing images of vaporplasma are shown in Fig6One of typical fluctuating period is from 1 Ills to 5 ms,and another process is from 5 IIIS to 8 msIn each fluctuating period,the vaporplasma within the keyhole e jects and then disappears graduallyFrequency of the va D【】rplasma from the keyhole iS within 1 67500 HzThis can also be revealed by images of bottom pool in penetra tion welding processshown in Fig7It can be found that the vaporplasma starts to eject from the bottom pool f t=l ms),and then gradually decrease until disappearance(t 3 ms)The next image(t=4 ins)clearly shows that the Vaporplasma occurs againAnd this process repeats again and again during whole welding processThe statistical data show that fluctuation frequency of the vaporplasma from the keyhole is within 167500 Hz,just as same as the results of optical emission =1 ms t=2InS t=3ms t=4ms t=5InS t=6mS t=7ms f=8ms =9IllS 拄10ms Fig6 Changing images of vaporplasma above the weld(Laser power 1 650 W and welding speed 1 mmin) 扛l ms t=2IllS f=3 Ills t=4ms =6ms t=7ms t=8ms t=9Ills t=3ms Fig7 Changing images of bottom pool(Laser power 1 650 W and welding speed 1 mrain) l0 HIS Behavior of vaporplasma within the keyhole and above the workpiece during CO2 laser penetration welding ll The physical process associated with frequency of the range B has been discussed in the other article 。which showed the features of vaporplasma arising from the shiel ding gas above the workpiece The fluctuation frequency of the vaporplasma within the keyhole is different from the shielding gas plasma a bove the workpieeeThe reason is mainly that formation of these two kinds of vaporplasmas are quite differentThe shielding gas plasma is caused by the process,which gas is heated to high temperature and then ionizes rapidly When its pressure reaches to a certain value,the plasma will explode and then disappear rapidlyHowever,the formation of the vaporplasma within the keyhole is quite differentWhile laser beam acts on workpiece,vaporiza tion will generate within the keyhole;then the vapor is heated to temperature higher than the boiling point;finally heated vapor explodes and ejects from both top and bottom 0f the weld under the condition of fullpenetration weld ingAccording to forming principle of two kinds of vapor plasmas during fullpenetration welding,three factors may cause theseFirstly,because of existence of bottom key hole,the pressure of the vaporplasma within the keyhole will increase slowlyMost vaporplasma within the key hole comes from vaporization of base metal,but most shielding gas plasma derives from shielding gas heated and ionized directlyFinally,higher vaporization pressure can be remained in the keyhole,but shielding gas plasma is in free and explodes at lower pressure 3 Conclusions For CO,laser welding of SUS304 stainless steel, some conclusions about vaporplasma are as follows: (1)The spectrum shows that the spectral components in the range of400700 nm are mostly lines ofArand most intense spectral lines are within 400600 nm (2)The study of optical emission from vaporplas ma,both for 400600 nm and IR emission,shows that the frequency components of the vaporplasma are quite complex and have not a dominant frequency component However,two characteristic frequency bands exist,one is 100500 Hz and the other is 1 5003 500 HzThe process correlated with 100500 Hz frequency component has obvious heat effect (3)Changing images of vaporplasma and bottom pool captured by high speed camera confirm that there are two kinds of vaporplasmasAnd their fluctuation frequen- ties are obviously differentThese vaporplasmas derive from the keyhole and shielding gas respectivelyThe sta tistical data show that fluctuation frequency of the vapor plasma in the keyhole is within 1 67500 Hz,just as same as the resuhs of optical emission References 1 Zhang X DMechanism and prevention of process instability in CO2 laser weldingBeijing:Tsinghua University,1997(in Chinese) 2Duley W WLaser weldingNew York:John Wiley&Sons Inc,1998 3Aalderink B J,Aarts R G K M,Jonker J B,et a1Study of the optical emission during Nd:YAG laser welding of AA5182Congress Proceedings ICALEO,San Francisco, California,USA,October 47,2004:1122 4 Naito YPenetration characteristics in YAG laser and TIG arc hybrid welding,and arc and plasmaplume behavior during weldingProceeding of Welding Association,2006,24(1): 3238 5Duan A Q,Chen LDynamic behavior of plasma in CO2 laser welding of stainless stee1Transactions of the China Welding Institution,2005,26(11):1720(in Chinese) 6Duan A Q,Chen LMolten pool and temperature field in CO2 laser weldingChina Welding,2006,15(1):3033
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機械類畢業(yè)論文中英文對照文獻翻譯
PDF英文5頁,word中文翻譯1149字3頁
有出處
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比照
文獻
翻譯
co2
激光
焊接
工件
焊縫
內(nèi)光致
等離子體
特性
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【機械類畢業(yè)論文中英文對照文獻翻譯】CO2激光熔透焊接時工件上及焊縫內(nèi)光致等離子體體的特性【PDF英文5頁word中文翻譯1149字3頁】【有出處】,機械類畢業(yè)論文中英文對照文獻翻譯,PDF英文5頁,word中文翻譯1149字3頁,有出處,機械類,畢業(yè)論文,中英文,對照,對比,比照,文獻,翻譯,co2,激光,焊接,工件,焊縫,內(nèi)光致,等離子體,特性
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