【正文】 感謝！其次,此次設計的開始我對理論還部熟悉的情況下，還得到了學長、學姐們的幫助和指導,這一路以來也在他們不斷的鼓勵和支持下一直完成工作,在此向他們送上我最誠摯的謝意。最后,在此論文完成之際,向我們一起工作、討論的小組成員,道一聲感謝。，也預示著我將離開西安工業(yè)大學，我將時刻銘記我曾是一名西安工業(yè)大學的學子，在以后的學習、工作中再接再厲，盡我最大的努力做到最好來回報母校給我的教導之恩。畢業(yè)設計（論文）知識產權聲明本人完全了解西安工業(yè)大學光電工程學院有關保護知識產權的規(guī)定，即：本科學生在校攻讀學士學位期間畢業(yè)設計（論文）工作的知識產權屬于西安工業(yè)大學光電工程學院。本人保證畢業(yè)離校后，使用畢業(yè)設計（論文）工作成果或用畢業(yè)設計（論文）工作成果發(fā)表論文時署名單位仍然為西安工業(yè)大學光電工程學院。學校有權保留送交的畢業(yè)設計（論文）的原文或復印件，允許畢業(yè)設計（論文）被查閱和借閱；學?？梢怨籍厴I(yè)設計（論文）的全部或部分內容，可以采用影印、縮印或其他復制手段保存畢業(yè)設計（論文）。（保密的畢業(yè)設計（論文）在解密后應遵守此規(guī)定）畢業(yè)設計（論文）作者簽名：指導教師簽名：日期：畢業(yè)設計（論文）獨創(chuàng)性聲明秉承學校嚴謹的學風與優(yōu)良的科學道德，本人聲明所呈交的畢業(yè)設計（論文）是我個人在導師指導下進行的研究工作及取得的研究成果。盡我所知，除了文中特別加以標注和致謝的地方外，畢業(yè)設計（論文）中不包含其他人已經發(fā)表或撰寫過的成果，不包含他人已申請學位或其他用途使用過的成果。與我一同工作的同志對本研究所做的任何貢獻均已在論文中作了明確的說明并表示了致謝。畢業(yè)設計（論文）與資料若有不實之處，本人承擔一切相關責任。畢業(yè)設計（論文）作者簽名：指導教師簽名：日期：附 錄附錄A單片機連接圖附錄B 單片機主程序設計單片機主程序設計如下：includeincludeinclude //包含有左右循環(huán)移位子函數的庫 includeincludedefine uchar unsigned chardefine ulint unsigned long intint date =0。 //接收AD的采樣值 ulint shuzhi=0。 //將要顯示的數值賦給它ulint bijiao[3]={100,10,1}。uchar disdate[3]={0,0,0}。uchar AA[]={0123456789}。void main(){ int ii=0。 P1 = 0x00。 delay(1000)。 Initlcd()。 //液晶初始化 while(1) {date=AD(0)。 shuzhi=date。 //AD值賦給變量數值shuzhi= (shuzhi*5/)*。 for(ii=0。ii3。ii++) { disdate[ii]=AA[shuzhi / bijiao[ii]]。 shuzhi=shuzhi % bijiao[ii]。 } }} 附錄C外文翻譯Study of electrodeless discharge lamp properties and plasma/wall interaction, G. Revalde1, , ,1 Institute of Atomic Physics and Spectroscopy, Univerisity of Latvia, Skunu 4, Riga, LV1050, Latvia2 Institute of Theoretical and Applied Mechanics, Novosibirsk, RussiaOur work is concerned with the preparation and investigation of highfrequency light sources,containing different elements, excited by means of outer electrodes, so called, electrodeless light sources. In this work we consider our experience in the technology of the electrodeless light sources, on the example of mercury and rare gases. The interaction process with the discharge vessel is investigated using spectroscopic emission measurements of the filling elements and the wall surface diagnostics by means of the atomic force microscope. The necessary quantity of the mercury filling is estimated to reach a considerably long working life.1. GeneralThe history and development of lamps has always been closely connected to materials properties used for them. The properties of materials have always determined new steps towards more efficient light sources. The trend in modern light source development clearly points towards a miniaturization with the effect of higher radiation intensity from the lamp, also bined with demands of higher lifetime. New aggressive fillings are introduced and the thermal loading can reach the temperature limits of the wall material. The large diversity of lamp applications requires specific properties of the used envelope material and in practice it has caused some problems: wall corrosion and blackening, layer formation, solarisation and UV radiation resistance, increasing ignition voltage, luminescence, outdiffusion of filling ponents, microcracks under VUV –radiation [1]. In this work we deal with the study of filling problems as well as spectroscopic properties of electrodeless discharge lamps for broad range of applications.Electrodeless lamps, driven with the high,radio or microwave frequencies, have nowadays many nonlighting applications, but they start to penetrate also general lighting markets. Light sources, based on highfrequency or radiofrequency electrodeless discharge are widely used for atomic absorption analysis,magnetometry, etc. Our research is concerned with the preparation and diagnostics of new performance high frequency electrodeless light sources (HFEDLs), filled with different elements for their use in scientific devices [2].The history of development of highfrequency (HF) electrodeless light sources (EDL) in science and technique goes back to the twenties. Jackson began to use the HF discharge, which was excited in a tube, filled with rubidium, by means of electrodes placed outside the tube. The rubidium pressure was mbar, and the source was heated to increase the line intensities [3]. A similar design was used by different research groups until the beginning of fifties to excite the spectra of various elements [4, 5]. One of the first HF light sources as often used today was created by Bell and Bloom in 1961 [6].The HF EDS vessels are mostly made of glass or quartz and filled with a working element and buffer gas (usually rare gas). Lamp contains lamp balloon and a short side branch (cold spot) containing working element. The lamp vessel is placed in highfrequency generator coil to induce an inductivecoupled electrodeless discharge. Typically, the HFelectromagnetic is applied. The side branch could be thermostated to control the metal vapour pressure in the lamp. The light source vessel is placed into some thermo isolation. In general, the lamps could be designed in different forms.Such light sources have many advantages than many others due to the absence of the electrodes and hence they are easier to manufacture and to create plasma describing models. Many problems which are caused by electrodes, in these lamps are eliminated. In these lamps the optimal amount of filling has to be found experimentally for each element [7, 8]. However, during the lamp operation time, interaction of the filling element with the walls of the vessel occurs. This process depends strongly on the light source operating conditions and on the filling type.2. ExperimentaIn order to find out the optimum and to study the plasma interaction with a wall, we have prepared HF EDL samples from quartz with a spherical form of 20 mm diameter with mercury in a metal phase of different amount. The inductive coupled discharge was induced in the light