html head titleGaussian beamtitle meta http-equiv=Content-Type content=texthtml;charset=utf-8 style .mainbody{margin 0 auto;width90%;background-color#ffffff;text-alignleft;} .webtitle {height80px;background-imageurl('httpdemo177.qxdwl.comimageslogo.png');background-repeatno-repeat;background-positionleft;} .calcname {top 100px; width100%; height50px; padding-top10px;padding-bottom10px;margin-bottom15px;background-color#ffffff;text-aligncenter;font-weightbold;font-size14pt;font-family黑体,SimHei;line-height20px;border-stylesolid;border-width0px;border-top-width1px;border-color#f9f9f9;} .calctitle {border-styledotted;border-width 1px;width70px;color#000000;font-weightnone;font-size12pt;font-family黑体,SimHei;displayinline;padding10px;margin-top0px;} .container {top10px; width97.8%;height480px;margin-top9px;margin-bottom12px;padding-top20px;padding-left20px;line-height30px;border-stylesolid;border-width0px;border-top-width1px;border-color#eeeeee;background-color#f6f6f6;font-size11pt;font-family黑体,SimHei;color#444444;} .calcblock {font-size11pt;font-family黑体,SimHei;color#444444;text-alignleft;line-height25px;} .adblock {height50px;width890px;bordersolid 1px #eeeeee;margin-bottom12px;margin-left0px;background-color#a9a9a9;text-alignleft;padding-top25px;} body {background-color#f1f1f1;text-aligncenter;} .equblock {font-size11pt;font-weightbold;font-family黑体,SimHei;color#444444;text-alignleft;line-height20px;margin-top15px;margin-left20px;} .dispblock1 {font-size11pt;font-family黑体,SimHei;font-weightnone;text-alignleft;} a {font-size10pt;color#000000;text-decorationnone;font-weightbold;} avisited {font-size10pt;color#333333;text-decorationnone;font-weightbold;} ahover {font-size10pt;color#0000ff;text-decorationunderline;font-weightbold;} .SHGcanvas {background-colorwhite;} table {text-aligncenter;vertical-aligncenter;font-size11pt;font-weightbold;font-family黑体,SimHei;border-collapsecollapse;border-spacing0;color#444444;} tr {height30px;} td {width60px;border1px solid #444444;color#444444;} style script type=textx-mathjax-config MathJax.Hub.Config({tex2jax {inlineMath [['$','$'], ['(',')']]},displayAlign center}); script script type=textjavascript src=httpcdn.mathjax.orgmathjaxlatestMathJax.jsconfig=TeX-AMS-MML_HTMLorMML script script function setblock(a) { titleblock='ftitle'; contentblock='container1'; b='fblock'+a.charAt(a.length-1); var x1=document.getElementById(titleblock).childNodes; for(i=0;ix1.length;i++) { if((x1[i].className=='calctitle') && (x1[i].id!=a)) { document.getElementById(x1[i].id).style.backgroundColor=#ffffff; document.getElementById(x1[i].id).style.color=#000000; document.getElementById(x1[i].id).style.borderStyle=solid; document.getElementById(x1[i].id).style.borderColor=#ffffff; document.getElementById(x1[i].id).style.borderBottomColor=#f6f6f6; } } document.getElementById(a).style.backgroundColor=#f3f3f3; document.getElementById(a).style.color=#000000; document.getElementById(a).style.borderColor=#ccddff; document.getElementById(a).style.borderBottomColor=#f6f6f6; document.getElementById(a).style.borderStyle=solid; var x2=document.getElementById(contentblock).childNodes; for(i=0;ix2.length;i++) { if((x2[i].className=='calcblock') && (x2[i].id!=b)) document.getElementById(x2[i].id).style.display=none; } document.getElementById(b).style.display=block; } window.onload=function() { setblock('f_title1'); } script script function num2e(num) { var p = Math.floor(Math.log(num)Math.LN10); var n = num Math.pow(10, -p); return n.toFixed(4) + '10sup' + p +'sup'; } function do1() { var n1=document.getElementById(wavelength); var n2=document.getElementById(r0); var n3=document.getElementById(Z1); var pi=Math.PI; var q1=pin2.valuen2.valuen1.valueMath.pow(10,6); var q2=2n2.valueq11000; var q3=n2.valueMath.sqrt(1+n3.valueq1n3.valueq1); var q4=n3.value(1+q1q1n3.valuen3.value); var q5=n2.value1010; var q6=n3.value1010; var disp1=document.getElementById(dispblock1); disp1.innerHTML=计算结果br远场发散角+q2.toFixed(2)+ mradbr瑞利长度+num2e(q1)+ mmbrz处的光斑半径+q3.toFixed(2)+ mmbrz处的波前曲率半径+num2e(q4)+ mm; } script head body div class=mainbody div id=weblogo class=webtitle div div id=calcname class=calcname b高斯光束的空间分布bbr bfont color=#888888 size=2Calculator of Gaussian beamfontb div div id=ftitle div id=f_title1 class=calctitle onClick=setblock('f_title1');参数计算div div id=f_title2 class=calctitle onClick=setblock('f_title2');程序说明div div id=f_title3 class=calctitle onClick=setblock('f_title3');主要公式div div id=f_title4 class=calctitle onClick=setblock('f_title4');参考div div div id=container1 class=container style=height450px; div id=fblock1 class=calcblockcenter table cellspacing=0 cellpadding=0 style=text-alignleft;border1px solid #444444;margin-left0px;margin-top20px;font-weightbold;trtd valign=top style=border-right1px solid #000000;line-height25px;font-size11pt;font-family黑体,SimHei;color#444444;width300px;padding-left40px;padding-bottom20px; br 1.激光波长λ input type=text id=wavelength value=800 size=4 style=margin-left9px; nm br 2.束腰半径ωsub0sub input type=text id=r0 value=0.5 size=4 style=margin-left2px; mm br 3.距束腰距离z input type=text id=Z1 value=100 size=4 style=margin-left0px; mm brbr centerinput type=button id=calcbutt1 style=width100px;height40px;font-weightbold;margin-left-20px; value=计 算 size=15 onClick=do1();center tdtd valign=top style=line-height25px;font-size11pt;font-family黑体,SimHei;color#444444;width300px;padding-left40px;padding-bottom20px;padding-right40px;br div id=dispblock1  div tdtrtrtd colspan=2 style=text-aligncenter;a href=F06Plus.html图示版a    tdtrtablecenter div div id=fblock2 class=calcblock style=text-indent2em;padding-top10px;line-height30px;padding-left0px;font-weightbold; font color=#dd3333本程序font用于计算高斯光束的空间分布。br 功能计算高斯光束的远场发散角、瑞利长度、距离腰斑距离处的光斑半径和波前曲率半径。br div div id=fblock3 class=calcblock title=右键单击公式选择'Show Math as'-'TeX commands'可获得公式的tex源码,方便引用。 style=padding-left20px;font-weightbold; 1.远场发散角br div style=margin-left20px;color#000000 $${theta} =frac{2lambda}{pi w_0}$$ div 2.瑞利长度br div style=margin-left20px;color#000000 $${Z_R} =frac{pi w^2_0}{lambda}$$ div 3.距离腰斑距离z出的光斑半径br div style=margin-left20px;color#000000 $${w_z} ={w_0}sqrt{1+{(frac{z}{Z_R})}^2}$$ div 4.距离腰斑距离z出的波面曲率半径br div style=margin-left20px;color#000000 $${R_z} ={z}[{1+{(frac{Z_R}{z})}^2}]$$ div 其中ωsub0sub为激光腰斑半径,θ为远场发散角,λ为光波长,ZsubRsub为瑞利长度,ωsubzsub为距腰斑z处的光斑半径,Rsubzsub为波面曲率半径。 div div id=fblock4 class=calcblock style=padding-left20px;padding-top10px;line-height30px;font-size11pt;font-weightbold; div div div body html