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href=3D"view.php?bn=3Dfusor_ionguns&key=3D1261428592" title=3D= "View thread collapsed" onmouseover=3D"window.status=3D'View thread coll= apsed';return true" onMouseout=3D"window.status=3D'';return true" class=3D= "wa_link">standard view</a></div><div align=3Dleft><ul><li><font size=3D= -1>2009-21-12 14:49</font> <a href=3D'#N1261428592'><em>Inverter Microwa= ve for Ion Source RF</em></a> (lutzhoffman) <ul> <li><font size=3D-1>2009-21-12 16:01</font> <a href=3D'#N1261432886'><em= >Re: Inverter Microwave for Ion Source RF</em></a> <img src=3D"images/fi= le_types/multiple.gif" border=3D"0" width=3D"15" height=3D"15" align=3D"= absmiddle"> (Doug Coulter) <ul> <li><font size=3D-1>2009-21-12 19:11</font> <a href=3D'#N1261444275'><em= >Re: Inverter Microwave for Ion Source RF</em></a> (lutzhoffman) <ul> <li><font size=3D-1>2009-21-12 21:35</font> <a href=3D'#N1261452945'><em= >Re: Inverter Microwave for Ion Source RF</em></a> (Doug Coulter) </ul> </ul> <li><font size=3D-1>2009-22-12 11:08</font> <a href=3D'#N1261501712'><em= >Re: Inverter Microwave for Ion Source RF</em></a> <img src=3D"images/fi= le_types/image.gif" border=3D"0" width=3D"16" height=3D"16" align=3D"abs= middle" alt=3D"JPG picture"> (Doug Coulter) <ul> <li><font size=3D-1>2009-22-12 16:15</font> <a href=3D'#N1261520147'><em= >Re: Inverter Microwave for Ion Source RF</em></a> (lutzhoffman) <ul> <li><font size=3D-1>2009-22-12 16:44</font> <a href=3D'#N1261521842'><em= >Re: Inverter Microwave for Ion Source RF</em></a> (Doug Coulter) <ul> <li><font size=3D-1>2009-23-12 15:36</font> <a href=3D'#N1261604190'><em= >Re: Inverter Microwave for Ion Source RF</em></a> (lutzhoffman) </ul> </ul> </ul> <li><font size=3D-1>2009-22-12 16:24</font> <a href=3D'#N1261520681'><em= >Re: Inverter Microwave for Ion Source RF</em></a> <img src=3D"images/fi= le_types/image.gif" border=3D"0" width=3D"16" height=3D"16" align=3D"abs= middle" alt=3D"GIF picture"> (Doug Coulter) <li><font size=3D-1>2009-22-12 18:09</font> <a href=3D'#N1261526953'><em= >Re: Inverter Microwave for Ion Source RF</em></a> <img src=3D"images/fi= le_types/multiple.gif" border=3D"0" width=3D"15" height=3D"15" align=3D"= absmiddle"> (Doug Coulter) <ul> <li><font size=3D-1>2010-05-01 12:15</font> <a href=3D'#N1262715354'><em= >Re: Inverter Microwave for Ion Source RF</em></a> (Kevin Dooley) <ul> <li><font size=3D-1>2010-05-01 13:22</font> <a href=3D'#N1262719367'><em= >Re: Inverter Microwave for Ion Source RF</em></a> (Doug Coulter) <ul> <li><font size=3D-1>2010-05-01 13:31</font> <a href=3D'#N1262719876'><em= >Re: Inverter Microwave for Ion Source RF</em></a> (Kevin Dooley) </ul> </ul> </ul> </ul> </ul></div><a name=3D'N1261428592'><br><TABLE BORDER=3D"0" CELLPADDING=3D= "0" CELLSPACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Inverter Microwave for I= on Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:lutz.hoffman@kp.org?su= bject=3D[fusor_ionguns] Inverter Microwave for Ion Source RF'>lutzhoffma= n</a> on <b>2009-21-12 14:49</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Hello:<br /><br />In the interest of building a microwave ion source, = I have been looking for an old microwave to gut for RF parts. Doug Coult= er is currently building exactly such an ion source, and his work in thi= s area is brilliant to say the least. He is much more knowledgeable on t= he subject than I am, and he is kind enough to share his work. Between C= arl, and Doug's work, quality ion sources will soon be a simple buil= d for the amateur. In my opinion this is a fairly profound event, which = may lead to many great discoveries in the future. As far as nuclear phys= ics on an amateur level goes, ion sources ARE a very big deal, and perha= ps the most difficult single component home build.<br /><br />Originally= I planned on using Carl's design, but I soon discovered that it is = very difficult to obtain the required set of RF components, which are sm= all enough to fit inside of the HV terminal of my project, even with the= aid of a small amplifier, like the ones from Communications Concepts. <= br /><br />This is where Doug's idea of using microwaves comes in. W= ith a microwave based ion source the nearly complete set of RF component= s, can be had at the local Walmart for under $50! Better yet they fit in= side of a small space, with simple control circuits. If my ion source we= re at ground potential then I think I would go with Carl's design si= mply because it is the proven, and traditional way to go, with few unkno= wns, or potential issues. So in a nutshell I like both approaches very m= uch, but I want to try Doug's design on this project.<br /><br />I r= ecently scored a working Panasonic Inverter Microwave oven, rated at135= 0W, at the local dump. To my delight it is in perfect working order, the= interior has some burn marks, and a broken glass plate, so the owners m= ust have "assumed" it was toast, or that it was to expensive t= o fix.<br /><br />I very carefully removed all of the innards, being car= eful not to mess anything up. This went very well, I was even able to re= move the control panel leaving it attached. After a short time I was abl= e to get the magnetron to work outside of the oven (While observing RF s= afety measures) just fine. By leaving the factory control circuit attach= ed, I have full control over the output, both in terms of power, and tim= e. My feeling here is that instead of trying to engineer a new control c= ircuit, it would be very easy to just wire an extension from the control= board to the magnetron. I will just have to make a translation table li= ke: 1 Pound Auto Defrost =3D 100uA Beam x 10min, this could be handy : )= <br /><br />What I cannot figure out is the properties of the microwave= output from this Panasonic assembly. Traditional tranny based microwave= s produce a pulsed output, via the HV diode / capacitor circuit. Looking= at the Panasonic inverter based design, I notice that the input 120V 60= Hz, goes into a FW rectifier and is first converted into DC. The DC then= goes into a circuit with what looks like a fairly solid MOSFET, or IGBT= , then to an inductor / small capacitors, and to the HF ferrite transfor= mer, then finally the magnetron. It could be a resonant system. The circ= uit however lacks anything like a substantial HV capacitor which has me = wondering about the nature of the RF output?<br /><br />Some promotional= literature on the net seems to imply that the output is CW? By referenc= ing to a traditional microwaves "pulsed output" being inferior= . My question is: Is the output of this inverter microwave pulsed, or is= it CW? Or if it is pulsed, is it pulsed at very fast rates like in the= KHz range? I do not own a scope so I cannot just figure it out this way= <br /><br />I could not find a clear answer about this question when I r= esearched on the net, which led me to writing this post. For an ion sour= ce CW is normally preferred, but when I think about it the efficiency of= ion sources normally goes up with increased RF power. Thus a fast enoug= h pulsed RF output could be an ideal situation. The higher peak RF energ= y increasing efficiency, while the HF pulsing rate is fast enough to ena= ble easy power measurement, and monitoring. Personally I do not want to = have a 60-120Hz ion source output, but 10 or 20 KHz would be just fine, = and maybe even preferred to CW : )<br /><br />Can anyone shed some light= on this, by explaining the nature of the RF output from an inverter mic= rowave? <br /><br />Thank You.....Lutz </TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1261432886'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:clab@swva.net?subject=3D= [fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>Doug Coulter</= a> on <b>2009-21-12 16:01</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Well, you speak of the devil, and here I am.<br /><br />I own two of tho= se ovens myself, they are fantastic for cooking.<br /><br />No, they are= n't CW, they pulse at 30khz or so. But to reduce power, they reduce= the pulse height/width at that frequency. This looks enough like CW to= the food to make no difference, compared to the old on for a few second= s, off for a few seconds older machines used to control power.<br /><br = />Getting a maggie to go really CW is kind of a trick, and one I guess I= should start writing up for others.<br />My basic idea is far from new,= I copied the basic RF design from a rev-sci-ins article from way back t= here, where they used a medical diathermy source (so they didn't hav= e to figure that part out at all) and were mainly interested in cavity d= esign. I just copied theirs more or less with some slight improvements = of my own, and added the ECR magnets they forgot to put in there for bet= ter performance, and indeed this is better than they claimed by a large = factor. If I can believe my mass spectrometer it makes mostly atomic io= ns, not D2+. I even see that with the mass spec fairly far away from it= in the tank -- I see some D2+ too, but that would be about the amount f= rom some hitting the walls and recombining on the way to the spectromete= r.<br /><br />I am debating whether to make a real long thread entry her= e on "how to make a magnetron that was never meant to run CW do it = anyway" but I'm having second thoughts as it would be pretty lo= ng.<br />You're not going to get there with either the panasonic mag= gie (far too big) or that power supply (completely unsuited for this wor= k on several levels). I am not sure either of the power supplies I'= ve done this with would easily float up to HV, mine are operating near g= round. They wouldn't go into a HV terminal easily at HV unless ther= e's one heck of a fine isolation transformer, or a shaft drive/gener= ator kind of thing around, these things take some real power input, abou= t 80 or 90 watts to run.<br /><br />Lutz, if you wanna email me, I can s= end the sloppy version, I want the one I put up here to be pretty good f= or beginners to follow.<br /><br />But the key is this:<br /><br />Find = a magnetron tube about the *lowest* power you can find -- the panasonic = one is a monster. We just picked a small one from dumpster microwave ov= ens, but they're not expensive at the microwave repair stores either= .<br />You may need to try more than one anyway, as they mode-hop at low= /medium powers, in and out of the resonance of the high Q cavity sometim= es - a small one does this less as there's a lot of stored energy in= the cavity to help keep it from doing that. You must run them very low= power CW, as these have no facility to handle electron buildups and eve= ntually you burn out the ends when the electrons spiral up and down to t= hem, or in some, just build up in the tube cavity and eat RF power and s= top all oscillations. A little tilt on the mag field stops that one, ea= sy, and usually is there by "made sloppy and cheap" for free.<= br /><br />You then need a "constant current" well filtered DC= supply, at pretty low current, 10-20ma max. I've made two, one wit= h standard parts from an oven (but I used a transformer at higher volts = than required for this tube so I could afford to lose some in the filter= ing) and one that uses my H bridge switcher. They both work fine. You = will need a fan on the maggie, the filament power alone will get them ab= ove max spec temperature without one. That's around 33 watts there.= Then you put in maybe another 20-50 watts DC. Above that, things fail= quick, and it's more than you need anyway. <br /><br />It's a = balancing act running this thing right at were it will oscillate at all,= not mode hop, and not burn up, but once you find that point, it works e= very time you flip the switch, very nice -- I've run it for many hou= rs (maybe 100 or more, and many off on cycles), no problems. I am using= a variac in mine with the standard xfrmr, set at about 89 volts....high= er and it mode hops and becomes useless (and burns up) and lower it just= won't oscillate.<br /><br />To make a supply with a standard MOT yo= u need to use a small series cap, on the order of 1/10 the one they norm= ally supply (I am using a .1uf and it's still too big, about half th= at would be better), a series R and another diode/cap (2 uf used here) o= n the output to get decent DC. I am using about 2k series R there and h= ave a neon bulb with it's own ballast across that as a simple curren= t monitor to see if the thing is drawing some current and a rough indica= tion how much. On peaks the drop across 2k/10w R is plenty to light it.= <br /><br />Kind of surprised the board let me put up this 807kb file, b= ut I copied and improved their cavity number 5 -- just a few helpful cha= nges and builder tweaks to keep the arcing down and make it out of easy = to get parts, mainly. Like I said, not many watts input are needed. I = made a yoke and with magnets from amazing magnets to do the ECR part on = this. I adjusted the field with a hall effect meter for the rignt numbe= r in the middle, it goes up on both sides of that, but seems fine and wo= rks fantastic -- I get the thing lit off, and it stays lit to e-6 mbar l= evels -- very nice if you want to run low pressures and not need differe= ntial pumping to keep the rest of your apparatus down there for long mea= n free path.<br /><br />Quartz tubing is a must for this. It works, bar= ely, with pyrex, but needs higher powers, and basically it's the pyr= ex getting very hot and needing a fan. The cavity (1" ID Cu pipe f= rom the hardware store) gets warm, but only warm. I use thin wall 1/2&q= uot; OD quartz for this. I let the gas in via a capillarly tubing in th= e fitting on the outside the tank end.<br /><br />First picture is the t= hing in action, you can see it lighting up the gas. The picture isn'= ;t good enough to show that it's kind of pinched and expands away fr= om the cavity. See fan on maggie tube, that's absolutely required. = This is the business end of the tank, and I put that plexiglass shield = on there to keep arcs from the main feedthrough down.<br /><br />The nex= t pic is the power supply I'm using. It's a standard MOT, with = a wall wart glued on top for fan power. I have kept the original series= cap on there in case I someday want a lot of power, but for now, it'= ;s not hooked up. You can see the end of the white series cap I am usin= g, near the to-220 diodes I series-ed up to get high enough voltage for = this (they are 1.5kv 6a diodes, takes 5 for this use). The big cap on t= he back is the main filter cap, on which the charge is lethal, which is = why it's buried in my rack -- safety, and no I'm not pulling it = out of a working system for pictures!<br /><br /><br />Hope this helps. = Don't tell everyone about the copyright violation that paper repres= ents, just get it quick before we have to take it down.<br /><br />Oh, f= urther issues. I made the endcap on my lathe, and charge that with a po= sitive voltage, and a aluminum tube was turned to fit into the quartz on= the tank end, and extend some beyond this so any sputtering there doesn= 't make the quartz conductive. These are fed from a CCFL inverter w= ith two half wave volt doublers for + and - polarity output, which is co= ntrolled by an adjustable LM 317 on the input of the CCFL inverter. Wor= ks like a champ, and lets you control the amount of ions injected very n= icely and very fast.<br /><br />In my recent record runs, I had to turn = this off. The lm317 puts out enough with the adj terminal grounded to p= ut in too many ions (about +/- 300 volts), and enough just drifted in to= make that mode work. For other modes I use about +/- 3 kv or so, with = about a 33k resistor on both leads for arc protection issues. Those bur= n up before the rest does, kind of a fuse. <div class=3D"att_link"><a hr= ef=3D"getfile.php?bn=3Dfusor_ionguns&att_id=3D6726" title=3D"Download Mi= crowave Discharge Cavities Operating at 2450MHz.pdf (application/pdf - 8= 07.56 Kb)" target=3D"_blank" onMouseover=3D"window.status=3D'Download Mi= crowave Discharge Cavities Operating at 2450MHz.pdf (application/pdf - 8= 07.56 Kb)';return true" onMouseout=3D"window.status=3D'';return true"><i= mg src=3D"images/file_types/pdf.gif" border=3D"0" width=3D"16" height=3D= "16" align=3D"absmiddle" alt=3D"Adobe Acrobat document"><div class=3D"at= t_name">Microwave Discharge Cavities Operating at 2450MHz.pdf</div></a><= div class=3D"att_size">807.56 Kb</div></div> <div class=3D"att_img"= ><img src=3D"getfile.php?bn=3Dfusor_ionguns&att_id=3D6727" alt=3D"uWaveI= onSrc.jpg" border=3D"0" style=3D'Cursor:HAND;' onclick=3D"javascript:win= dow.open('showimg.php?url=3Dgetfile.php%3Fbn%3Dfusor_ionguns%26att_id%3D= 6727&w=3D1024&h=3D683&title=3DuWaveIonSrc.jpg', '', 'scrollbars=3D0,tool= bar=3D0,resizable=3D1,menubar=3D0,directories=3D0,status=3D0,width=3D102= 4,height=3D683')" width=3D600 height=3D401></div> <div class=3D"att= _img"><img src=3D"getfile.php?bn=3Dfusor_ionguns&att_id=3D6728" alt=3D"U= Wavepower.jpg" border=3D"0" style=3D'Cursor:HAND;' onclick=3D"javascript= :window.open('showimg.php?url=3Dgetfile.php%3Fbn%3Dfusor_ionguns%26att_i= d%3D6728&w=3D1024&h=3D683&title=3DUWavepower.jpg', '', 'scrollbars=3D0,t= oolbar=3D0,resizable=3D1,menubar=3D0,directories=3D0,status=3D0,width=3D= 1024,height=3D683')" width=3D600 height=3D401></div> </TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1261444275'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:lutz.hoffman@kp.org?su= bject=3D[fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>lutzho= ffman</a> on <b>2009-21-12 19:11</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Great Reply, Thanks Doug <br /><br />Ok, There is one thing that I jus= t am not getting, sorry, I am not trying to be difficult:<br /><br />If= you feed the microwave ion source with 30Khz pulsed microwaves from an = inverter microwave unit, instead of the normal CW microwave RF, would it= not still function? Instead simply producing an ion beam which pulses a= t 30KHz? <br /><br />I am asking because Sulfur lamps for example are f= ed with pulsed microwaves, and the discharge is not extinguished in betw= een pulses or anything. This has me thinking that if a Sulfur lamp; Whic= h is nothing but a hollow quartz ball filled with low pressure Argon wit= h some elemental Sulfur, works just fine on pulsed microwaves. An ion so= urce is basically the same thing, just with an added magnetic field, and= an extraction electrode. Maybe a RF driven sulfur lamp could even be c= onverted into an ion source, by drilling a gas/extraction hole, and add= ing some magnets? The trouble is the sulfur lamps are hard to find in th= e first place : ) This brings me to another idea, just for fun fill som= e quartz balls with various elements, and energize with RF : ) A Rubid= ium fill focusing on a Nd:YAG rod would be interesting. Anyway back to t= he topic....<br /><br />My thinking here is why not power the ion source= with pulsed microwave RF, if it is fast enough to sustain the discharge= ? If an ion beam pulses at say 10-30KHz, then the beam current could be= averaged out via a capacitor in the faraday cup circuit for an accurate= reading. In other words it would not matter to me if my particle beam p= ulses at 30KHz, as long as I get an high enough average beam current. <b= r /><br />Maybe the ion source could be used both ways: With CW RF for p= recision work, and with pulsed microwave RF for brute force high beam cu= rrent work?<br /><br />Thank you for your thoughts, and for explaining t= he concepts involved.<br /> <br />Aloha.....Lutz : ) </TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1261452945'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:clab@swva.net?subject=3D= [fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>Doug Coulter</= a> on <b>2009-21-12 21:35</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Yes, you'll get a pulsed beam with a 30khz component to it. It won&= #39;t quite match the drive, as some ions get going fast enough to make = more by collisions, the electrons will continue their cyclotron motion f= or awhile, so there's a tail, the length of which depends on a lot o= f things -- how much gas, volume, and so forth. If you use enough extra= ction field, that may do some keep-alive as well.<br /><br />In my case,= I couldn't tolerate the resulting noises as I am studying time-dyna= mics in the fusor just now, and didn't need an additional signal to = have to deal with, or have affect the thing I'm looking at.<br />All= my phenomena don't mind the 2.45 ghz, that's too fast for ions = to do much. And this thing btw makes so little uwave leakage a microwav= e leakage detector that does register the oven I have, just sits on zero= anywhere around it. Nice.<br /><br />Sulfur lamps are designed to be e= asy to light off (most lamps are ;~). This means that they can light of= f on every cycle easy -- and they are dumping real significant power int= o those anyway. They'd be using in the few torr region of gas to pr= omote this, just like merc vapor bulbs do and for the same reason. Low = pressure is a relative term, they are not low in terms of what you need = for accelerator runs, but *many* orders of magnitude higher than that.<b= r /><br />For just making ions, you don't need and can't use hig= h power -- things melt and so on.<br />Note the fan they put on the one = in the paper, for a 75 watt RF source. Mine doesn't need that and m= akes plenty of ions, orders of magnitude more than you'll have the p= ower to accelerate. Or I do, and I have kilowatts for that at much lowe= r volts than your accelerator will need to be interesting.<br />My sourc= e puts out at least 10 ma as configured. That's more than plenty fo= r an accelerator that would typically run in the small uA region at most= .<br /><br />If you try this at the half power minimum the panasonic get= s in near CW, before it reverts to the same old on-off for a couple seco= nds each, your stuff is going to go up in smoke in a rather spectacular = fashion. Even the quartz will melt. That's ~5 times the max power = used in the paper, btw.<br /><br />The beauty of CW operation is that on= ce lit, it will stay lit down to ridiculous low pressures, where over-si= mple armchair theory says "no way, mean free path far too long"= ;. If you let the thing drop, it's hard to start again. Mine seems= to take about 3-4 e-5 mbar or more to start, but will run way below tha= t, but only CW or very fast at any rate -- I tried 70khz and that wasn&#= 39;t fast enough to keep the ions hot until the next pulse. It had to b= e in a gas condition allowing restart every time, more pressure than I t= hink you can tolerate. For a fusor, it's probably fine to pulse if = it's fast -- it will start every cycle at those pressures, I am just= looking at something special and don't want the distraction just no= w.<br /><br />You are going to find that to get high average beam curren= t you'll need something more like DC, not a high peak to average rat= io of pulses.<br />The focus will change with instantaneous current due = to space charge effects, and there will be a maximum you can keep focuse= d to your specification, whatever that is. You don't want high ener= gy particles to almost make it to the target, but hit the tube walls, fo= r example. Ideal focus potential depends on current in ANY beam device,= from CRT's on up. I've acquired a heck of a lot of literature = on all this, and tested a lot of it -- they are not telling lies. Too b= ad I can't upload the nearly 10 gb we've gotten hold of in fusor= /fusion/beam technology papers and related stuff, it's quite the nic= e library.<br /><br />Remember, during off times, gas is still flowing i= nto your accelerator, just not ionized. You're going to have enough= troubles keeping that pressure down low enough to get a mean free path = you need without letting in gas when it's not even getting ionized, = and that's going to be kinda hard to pulse too at those rates. The = big boys all use another vacuum system (called differential pumping whic= h has nothing to do with diffusion pumps) pumping out a space between or= ifices between the source and the accelerator -- the ions go right throu= gh the holes when in focus, the other gas bounces around and gets remove= d, mostly. If you're worried about what you'll need to put in t= he HV terminal....well, a complete additional vac system sounds kind of = troublesome to me. And no, a long quartz tube from ground won't do = it as the gas in there will be highly easy to ionize at that pressure...= .which is why it was AT that pressure to begin with.<br /><br />In fact,= I did all this due to my Scottish repugnance to the idea of another vac= system being needed, and found a way to avoid that need, even for prett= y low tank pressures. At that, it's quite cheap by comparison.<br /= ><br />To be honest, it looks like the source Seltzmann is using might b= e the better one for most fusors, it's certainly simpler to make. I= doubt it lasts as long without maintenance as this one, just because th= is one is pretty phenomenal in that regard -- it's just never failed= in many many runtime hours, and no hint it's degrading in any way a= t all. THAT is cool indeed. </TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1261501712'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:clab@swva.net?subject=3D= [fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>Doug Coulter</= a> on <b>2009-22-12 11:08</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= In answer to a question Roman asked about the transfer of power from the= tube to the cavity:<br /><br />It's not a wave guide, it's a sh= ort (about 1/4 wave) piece of homebrew hardline coax. I don't want = to tear this down just now for pictures, but I can describe it fairly we= ll. A wave guide would have been quite large for this frequency (a coup= le inches across) and had too low an E field in it, with a quarter wave = cavity we can concentrate the E field far higher right where we want it.= So this is all kind of a standard low frequency RF design, just real s= mall. The cavity itself amounts to a 1/4 wave line with one end shorted= and is on the large side for this frequency. Trying to go larger diame= ter would allow other monkey modes to occur in it, rather than the longi= tudinal one we want.<br /><br />The top of the magnetron is the usual an= tenna post, surrounded by the RF ground gasket weaving.<br />I found a C= u pipe adapter that fit that gasket, and was big enough to hold the ante= nna post without clearances being too close. This adapter is brazed int= o a piece of sheet metal so the big end protrudes about 1/8" inch, = and bolting the sheet metal down presses it into the grounded gasket.<br= /><br />Into the top is inserted a piece of 1/2" Cu tubing. Here = in the US we call it pipe if we're talking about specifying the insi= de diameter and tubing if outside. Go figure, it's not a system I i= nvented, just have to live with it.. This is all stuff you can get at L= owes or the local equivalent. I get most things like this at McMaster. = Sad that I had to buy a 25 foot roll of 1/2" tubing to get 2 inche= s, but them's the breaks.<br />A stock of various tubing sizes is su= re handy around the lab anyway.<br /><br />The inner conductor is a piec= e of 1/8" tubing with about a 1/16" ID. One end has a washer = brazed on it, which is then soldered to the end of the "antenna&quo= t; on the tube, using a special flux for SS and nickel from McMaster aga= in. The other end is drilled and tapped for a 4-40 screw, which is the = adjustable length (for coupling to the cavity) part. This wound up more= or less flush with the cavity wall, and the end was "rounded"= or "melted" to eliminate sharp corners that caused arcing. T= rying to tune this while in operation was a joke -- anything you put in = the cavity burns up and mis tunes it, so we had to tune with power off, = try, retune, etc. This coupling adjustment doesn't seem very critica= l at all, since we're running *way* below the tube rated power, some= reflected power is fine as long as nothing arcs and there's enough = forward power coupled. This enters the cavity sort of tangentially like= in the paper (the picture there is all I had to go by myself). Temptin= g to try on the next one to place it closer to the "ground" en= d of the cavity for lower impedance there, but works as it is, near the = hot end just above the quartz tubing hole so it's coupling almost to= the tip of the tuning 1/4 wave stub.<br /><br />This tuning process was= helped a lot by having a DC discharge in the ioniser quartz tubing -- w= hich eventually became the pushme-pullyou ion extractor stuff. You then= always have some light and can tune for "most smoke" more eas= ily. Once it's all tuned, it stays that way really well, I've n= ever re adjusted that parameter for any set of conditions -- it works fi= ne, it ain't broke, and I ain't fixin it no more.<br /><br />The= cavity is about 2" long inside. It's a piece of 1" pipe = (eg one inch ID). I made the top piece which is threaded for a 1/4-20 b= rass tuning stub screw, and that's pretty thick in and outside the c= avity so as to have plenty of thread length, it's about 1/2" or= a little thicker, turned out of 1.25" Cu billet stock. I had to g= rind off the threads and round the end of the screw near the quartz tube= to cut down arcing there. I also put a spring under the screw head, as= this tuning is very twitchy indeed -- the entire range might be 20 degr= ees of turn on that screw.<br /><br />Again, resonance was found by tuni= ng this while there was already a discharge going on in the quartz tubin= g -- it's easy to tell when you get it right that way. Every now an= d then, a tiny jiggle on this screw helps the thing get going in high va= cuum, other than that I never touch it anymore. That's good as in u= se it's very near the HV and I'd rather not "go there"= when in operation.<br /><br />The cavity bottom is a pipe cap for that = size, that I shortened before grooving it and the cavity tubing for the = quartz to pass through -- you can take this off without breaking vacuum.= I drilled and tapped both that cap for 4-40 and the cavity tubing at t= he top for the same screw size so I can take all this apart. I should p= robably just solder the top on now, as that joint is a high current node= in this design and more conductivity is better, it's probably the m= ain loss I now have.<br /><br />Allow me to stress again that you NEED q= uartz tubing. Yes, it will kind of work with pyrex, at about double the= input RF power -- dicey due to arcs, and all that additional power goes= into heating the pyrex, not good. As is, the cavity doesn't need a= fan at all, barely gets hot, never hot enough to burn you. Yes, it'= ;s very clean inside, I did the usual anal prep there, and may silver pl= ate it for fun. It works fine as is, however -- I'll plate it if it= starts corroding in there.<br /><br />A key is finding the "right&= quot; magnetron. this is a smaller one from a junkyard oven. Some mag= netrons do a thing we RF guys call mode hopping (I guess laser guys use = the same term, and it's the same thing). There are usually 8 caviti= es in a magnetron, and never are they all just the same, so sometimes on= e or another will "take control" and it will then go at that f= requency. If that's not the frequency this very high Q cavity happe= ns to be tuned for, it stops working. Some of this is controlled by the= amount of power input, so finding one that doesn't mode hop much at= the desired power level is key. Having it be a smaller tube helps here= too as the amount of stored energy in the cavity can help keep it from = mode hopping better -- we're adding a ninth resonator, a better one = than those in the tube, even under load.<br /><br />It seems to be a luc= k factor, but luckily magnetrons are cheap even bought new. The key, ag= ain is getting a *small* one. We don't need the big power here at a= ll, too much of a good thing is bad for this. Do remember if the power = supply is remoted, even a couple feet, that these are 3.3v at 10 amp fil= aments, you'll need some really fat wire for that. The tube I happe= ned to pull off the shelf is a samsung OM52 series for what it's wor= th -- a very used one. Since it worked fine, I've not run through a= bunch of other types to test them for this, but since there's deman= d, I'll probably wind up making a few more for other people.<br /><b= r />The quartz tubing enters the chamber through a viton o ring coupler = I bought from Lesker, welded into a 1.33" CF flange (which was a tr= ick indeed, but that's what I had on that end flange).<br />That end= has a 1.5" long piece of Al pipe in it, most of that turned down t= o fit into the quartz, with about 1/4" extending from the end, so a= ny sputtering that happens doesn't land on the tubing and make it co= nductive. Al is good for not sputtering BTW as things go.<br /><br />At= the other end of the quartz is a fitting I made of brass that holds an = O ring for sealing, and is bored for a soldered in piece of SS capillary= tubing that is 1.5" long and .007" ID, to control gas flow. = This one's a little short and fat for that, but one I made on anothe= r source was 2" of .005" tubing and it was a little too restri= ctive, to give an idea of the range that works. You have to low temp so= lder this stuff as getting it hot enough to braze will cause some flakey= oxide to form inside the tubing and jam it up, and it's a darn hard= place to clean. The reason to have the gas flow orifice here is so tha= t all the rest of the plumbing can run at or near atmospheric pressure, = so all leaks are "out" rather than dirty shop air leaking &quo= t;in". I have not noticed any sputtering off the end of the SS cap= illary tubing, but hey, it's at the positive polarity side of things= , so shouldn't sputter anyway. Theory does work now and then.<br />= <br />Picture is a closeup of the homebrew hard line. As you can see, I= had to make an adapter to make the 1/2" tubing fit into the pipe a= dapter, and slotted the latter and put a clamp on it to hold things toge= ther. I've never adjusted that length, it's fine just as it was= put together.<br />Drilling that hole in the side of the main cavity wa= s actually the hardest part of all this, not that turning the endcap of = OFHC copper was a breeze, at least that part was thick and sturdy. Pipe= is another issue altogether, and needed a good jig to hold it and caref= ul milling machine work with very light cuts with a 1/2" end mill t= o get that off center oval hole made. I turned a piece of wood down to = keep the vise from crushing the pipe while doing that. The end of the h= ard line that has to be curved to match the cavity curve was done in sim= ilar fashion on the mill, but really you could do that with a round file= good enough without too much fuss.<br /><br />Oh, there's nothing b= ut air in there -- no dielectric at all other than 1.000000x air. <div c= lass=3D"att_img"><img src=3D"getfile.php?bn=3Dfusor_ionguns&att_id=3D673= 0" alt=3D"HardlineDetail.jpg" border=3D"0" style=3D'Cursor:HAND;' onclic= k=3D"javascript:window.open('showimg.php?url=3Dgetfile.php%3Fbn%3Dfusor_= ionguns%26att_id%3D6730&w=3D768&h=3D1152&title=3DHardlineDetail.jpg', ''= , 'scrollbars=3D0,toolbar=3D0,resizable=3D1,menubar=3D0,directories=3D0,= status=3D0,width=3D768,height=3D1152')" width=3D600 height=3D900></div>&= nbsp;</TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1261520147'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:lutz.hoffman@kp.org?su= bject=3D[fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>lutzho= ffman</a> on <b>2009-22-12 16:15</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Thank you so much for taking the time to explain everything, now I am be= gining to understand, at least enough to be willing to take a "wack= at it". <br /><br />Initialy I plan to run my accelerator at about= 150-200KV, this is without any SF-6 insulating gas, with the tube in de= humidified air. The tube should handle this voltage in air at STP. At h= is low energy level I would like to be able to crank up the beam current= big time, up to a maximum of 5-10ma for short times. For most experimen= ts 100-500uA should be fine.<br /><br />The next step will be to ramp up= the KV to the 400-500KV range, this could be done with an SF-6 gas mixt= ure at atmospheric - 2 bar pressure, now the max. beam current would be = about 2-5ma pulsed even for experiments requiring high power. For only 2= -bar, the pressure the vessel can even be PVC irrigation pipe, with an e= quipotential metal rings on the inside surface as well.<br /><br />So in= a nutshell the microwave ion source should work for me "as is"= ; just like Doug designed it. I was thinking about a "hybrid" = design which I call the CAD Ion Source (Carl and Doug). I am wondering i= f Carl's bottom end, and extractor, could be mated to Doug's mic= rowave ion source. At this point I am not familiar with the bottom end o= f Doug's ion source so it is to early to really consider anything li= ke this.<br /><br />One thing I did wonder about is Vicor high silica gl= ass? I know quartz is probably the best as Doug pointed out, but if Vico= r comes close enough, and if it is much superior to Pyrex, then it may b= e worth consideration for some applications, since Vicor can be worked j= ust like normal glass with oxy-propane. But then again it would probabl= y be just as easy to buy a quartz test tube to begin with. Thanks......L= utz </TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1261521842'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:clab@swva.net?subject=3D= [fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>Doug Coulter</= a> on <b>2009-22-12 16:44</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Lutz, <br />you may have focus troubles unless your volt gradient is WAY= steep trying to run that current. You need about 60x the gradient as f= or electrons for D ions for the same amount of beam blooming vs current.= Depending, as always, what you call "focus". TV CRT tubes r= un a few ma at 30kv or so.....you can work it out from there. This is b= ecause the D ions are going slower, so for a given current and volts, th= ere's more in flight next to one another than for electrons at the s= ame volts and amps, and they have more time to repel one another on the = way to the target.<br /><br />Glass "alloys" are just about as= diverse as for steel, it's astonishing how many there are, all char= acterized in the Kohl book on "materials and techniques for vacuum = devices". Or maybe even not all, but it's a heck of a loooonng= chapter.<br /><br />Vycor is one of "those", there are "= flavors". The top grade is quartz, plain and simple -- no differen= ce.<br />Some is kind of porous, and I'd not use that for this, but = you have to ask the source supplier.<br /><br />The reason for this is q= uartz is far lower loss than pyrex glass (DC and AC both), and more resi= stant to being taken apart chemically by hot hydrogen ions. Alumina isn= 't even in the running for this, too lossy by far.<br /><br />Here i= s where we get ours, a small outfit, and nice to deal with too -- they l= ike big orders, though, so people may want to get together and do a grou= p purchase (I will do one for this area if people want me to -- I am usi= ng the stuff up and want more myself).<br /><br /><A Href=3D"http://www= .quartz.com/" target=3D"_blank">http://www.quartz.com/</A><br /><br />I = also use their stuff to make my own HV feedthroughs, having gotten disgu= sted with the commercial versions.<br /><br />I work this with either a = small oxy propane torch I made using a wire welder tip as a gas tip (wor= ks great!) or an oxy-acetylene welder for bigger stuff. You need danger= -sensing sunglasses as it has to be white hot indeed and is blinding to = work on. The regular "didyium" glass blower's glasses are= n't the thing here, they only block the Na lines and you're stil= l blinded. Welding goggles are about right.<br /><br />This design need= s *none* of that, I guess I wasn't clear enough on that yet -- more = pix to come. It's just a cut piece of tubing, easy to cut another s= hould replacement be needed, on the lathe with a tool post grinder and d= iamond wheel. Quartz you can't just score and break like glass. It= comes apart at random if you try, and you might get cut while that expe= nsive stuff gets ruined. I don't even flame polish the ends for thi= s. </TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1261604190'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:lutz.hoffman@kp.org?su= bject=3D[fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>lutzho= ffman</a> on <b>2009-23-12 15:36</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Hello:<br /><br />Thank you so much for all your info on the ion source,= I think I have enough to get going on it when the time comes. I checked= with NEC reference the ion current which the tube can handle, and they = put the max at around 25-50ma with the main limitation being the ion sou= rce flooding the vacuum. Thank you so much for your help : ) I am curiou= s about one remaining thing which is the extraction end of the microwave= ion source? Is it the same as Carl's, or do you just have a small h= ole at the other end of the quartz tube, with an intermediate extraction= electrode close by at - potential? If I understand correctly this is w= here the CFL inverter comes in?<br /><br />An interesting feature of the= tube is built in intermediate focusing electrodes which are located bet= ween each accelerating section. Basicaly they are the same as the first = elecrostatic focusing lens which accepts the ion beam entering the tube.= This gives some control of the ion beam between sections. The entire as= sembly contains 28 electrodes including the entrance, and the other 2 fo= cusing electrodes. My plan is to drive the tube with a 14 stage FWCW mul= tiplier, with 13 equipotential rings, the terminal being connected to th= e 14th stage . I am considering two options on how to connect the tube t= o the VM, the first is: <br /><br />Every other electrode would be conne= cted to the 14 stage VM directly , via a HV resistor. Then the electrode= s in between these would be connected to the driven electrode below it, = also via a different value HV resistor. The question here was do I conne= ct the 14 intermediate electrodes to the VM connected electrode; Above, = or Below it?<br /><br />The second method being considered is to simply = build a 28 stage resistive divider, connected at 28 points to the tube, = and at 14 points to the VM stack?<br /><br />The first method would seem= to be more efficient, but the second would seem like it would have a be= tter potential distibution. My plan is to build the first 6 stages, and = then run the stack at a reduced voltage, and do a bunch of testing : )<b= r /><br />The actual VM stack is fairly well protected with series resis= tors (About 5-10K ohm combined value) between each stage capacitor, in e= ach stack. This is in addition to all of the normal protective measures = like spark gaps, input resistor ect. I am also using 3-4 times the nomal= number of HV diodes, in the first, and in last stages of the VM (In pa= rallel for higher surge current rating) since these diodes will see the = full surge current if a discharge were to occur, which would only be lim= ited by the series resistance of all of the 5-10K ohm protective resisto= rs. <br /><br />Thanks.....Lutz </TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1261520681'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:clab@swva.net?subject=3D= [fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>Doug Coulter</= a> on <b>2009-22-12 16:24</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Here's the simpler of the two power supplies I've built to run t= his. I did use a nominal 4.3 kv transformer to run a nominal 4.1kv tube= , but this may not matter too much. This could be done a little cheaper= than I did; this was all parts I had on hand anyway.<br /><br />I didn&= #39;t modify the transformer, knock out the saturation inducing cores, o= r anything, just used it.<br />In the actual build, I added a wall wart = and 3 terminal regulator for fan power uses. The Variac is adjusted to = about 89 to 91 volts rms output, or about the place where the transforme= r itself begins to saturate with no load. You may be able to substitute= a large incandescent lamp in series instead, but since I haven't tr= ied that yet, I don't know what the wattage would be, probably on th= e order of 250 w.<br /><br />You might be able to make the 2k resistor s= maller (as in 1k), I made it big so I could light that big neon bulb cur= rent draw "analog meter" I used to monitor operation. In that= huge neon bulb (got it at the last HEAS) you can see how much current b= y how much of the big electrode lights up, it's quick to glance at a= nd verify that things are on the bogey.<br /><br />In use, this results = in somewhat lowered filament power and terminal voltage. That's nee= ded to not burn up the tube which was never designed to run CW -- normal= ly the pulse mode lets extra electrons get out of the gap area naturally= and not bombardment-heat the filament too much, in CW they can build up= and make troubles -- a reason no one uses magnetrons for CW work, or ne= arly no one. I have a 12 volt computer case fan strapped to the tube fo= r cooling, and run another one across the general area to keep my HV fee= dthrough cool as it's designed to couple heat from the grid out of t= he tank (this will be another thread later). You *may* be able to run f= ull line volts, but the transformer will then get hot, if you use a smal= ler than .1uf series cap here to limit tube current. But these MOTs run= in saturation (as a voltage regulation feature in a normal oven) and ge= t quite hot if run for long times without a fan, or really even with one= . Here, we just don't need all that. In this design, nothing gets = hot.<br /><br />I also made PS on a ferrite core, using my H bridge desi= gn, but though it works, it's too complex for this, you just don'= ;t need it -- over engineering is as bad as not enough. And by the way,= since those ferrites run at ~8v a turn, you have to then make a stepdow= n transformer and actually rectify the filament voltage, as otherwise th= e crummy lossy chokes inside the magnetron will burn up! Too much for s= omething that is so simple, so I dropped that project. There's just= no need for the complexity.<br /><br />I will try to get cavity details= posted soon, so post any questions you want answered, as that will be t= he last post I make on this -- I will include the ECR magnet design in t= hat one. My next version will have the cavity inside the tank on a 2.75= " CF flange/pipe so the ions can get in there a lot easier, as only= RF and tuning need to go through the wall, both of which should be fair= ly easy (that is, if the type N weld in RF vacuum connectors I got from = Lesker don't give arc troubles). In that design, there won't be= the quartz tube, and the cavity bottom will be Cu or SS screen wire for= the ions to come out, and the RF stay in. I am still pondering how I c= an do adjustable ion extraction field on that one with least fuss.<br />= <br />In my particular version of this, running up the input power makes= it mode hop and go in and out of operation. This isn't a problem, = as it has plenty of RF output well below that point. And of course ther= e's that nice visual indication it's working. You have to see t= his with neon, it's blindingly bright.<br /><br />I seriously doubt = that you can modify an inverter type oven supply to do this -- they only= go to half power on inverter PWM, then revert to on-off operation for l= ower powers -- I think the issue there is that the filament is run off t= he same ferrite transformer and it gets flaky at low filament voltages. = That's 5-10 times the needed RF for this, and too much is BAD for t= his. You'd have to come up with some filament power some way, and f= ool all the fancy feedback loops in that inverter -- I've torn one d= own to see, then put it back together and sold the oven, it's just n= ot worth it. They *are* great for cooking though. <div class=3D"att_img= "><img src=3D"getfile.php?bn=3Dfusor_ionguns&att_id=3D6731" alt=3D"uWave= IonPS.gif" border=3D"0" style=3D'Cursor:HAND;' onclick=3D"javascript:win= dow.open('showimg.php?url=3Dgetfile.php%3Fbn%3Dfusor_ionguns%26att_id%3D= 6731&w=3D1227&h=3D543&title=3DuWaveIonPS.gif', '', 'scrollbars=3D0,toolb= ar=3D0,resizable=3D1,menubar=3D0,directories=3D0,status=3D0,width=3D1227= ,height=3D543')" width=3D600 height=3D266></div> </TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1261526953'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:clab@swva.net?subject=3D= [fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>Doug Coulter</= a> on <b>2009-22-12 18:09</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= OK, here are the rest of the details needed to replicate this, on a virt= ual silver platter.<br /><br />The cavity is a piece of 1" ID coppe= r pipe. It is 2" long, but the effective length is reduced a littl= e by the tuning cap depth of .2365" sticking inside. The tuning st= ub is a brass screw, 1/4-20 threaded into this to stick in .9860" f= or resonance in my setup -- that should get you within one turn if you&#= 39;re using quartz tubing for the gas.<br />The top cap is held in by ti= ght fit and by 3 4-40 screws threaded into the pipe. There is a spring = under the tuning screw head to get rid of backlash and so on. You will = note the screw has it's threads taken off the end, and the end round= ed to cut down arcing issues.<br /><br />The bottom is a pipe cap, short= ened and held on by tight fit and 3 4-40 screws threaded into it.<br /><= br />The gas inlet is a piece of 1/16 od, .007" id SS cap tubing, i= n a brass fitting I turned down to fit, which seals to the quartz by a v= iton o ring. The other O ring you see in the picture is just a cushion = so I don't stress the quartz (it's rough end, I did not flame po= lish it or even grind it flat) -- this makes it trivially easy to replac= e if needed, but this one has run over 100 hours and is still pristine. = This is charged to a positive voltage for ion extraction, via a CCFL in= verter that has variable DC input to control the extraction voltage. Th= is supply is bi-polar (two half wave volt doublers off the same source, = opposite polarity), eg if it's making 1kv positive, it also makes 1k= v negative for the other electrode. I use about a 20k 2w resistor for p= rotecting this from arcs from the nearby HV tank input.<br /><br />Not s= hown in these pictures is a polycarbonate 1/4" thick shield I also = use to keep arcs away from this.<br /><br />The magnets are NdFeB from A= mazing Magnets, with a half inch center hole. I used 1/2" by 1&quo= t; to stick them to, drilled for a little over half inch to let the tubi= ng pass, and 1/8" by 1" iron for the connecting yoke. You can= see in the picture the shim I taped in there after measuring the field = with a hall effect DC magnetometer to 980 gauss or thereabouts. The fie= ld isn't very uniform, but seems fine, and really makes a *huge* dif= ference in how well this works at very low pressures. Once lit off, I&#= 39;ve seen it still run down to 1.4 e-6 mbar, which happened to be the b= ase pressure of the system at that time, due to air infiltration through= the necessary insulating silicone tubing on the gas input. I may try a= nother flavor for that piece, but it has to be there to run the gas inle= t at high positive voltage to repel ions into the tank proper. With ion= extraction volts at max, about 2.5 kv + and -, and a pressure anywhere = above e-3 millibar, this lights off everytime just by turning it on. No= adjustments needed.<br /><br />Not shown, as the tank is under vacuum j= ust now, is the other end of the tubing. At that end, there is a piece = of 1/2' OD aluminum pipe that is turned down to fit inside, all but = about 1/4" of it, and the end is about flush with the magnet closer= to the tank. The other end projects about 1/4" into the tank past= the end of the quartz tubing, so if it sputters, it won't sputter o= nto the quartz. This is hooked to the negative polarity of the ion extr= action supply through the same value protection ressistor, with a wire r= un inside the tank and insulated with alumina beads -- you can see it in= other pictures I've posted here on fusor operation, glowing red in = X rays.<br /><br />The hole you see in the cavity in the last picture is= for tuning the coupling rod length. It's useless more or less, eve= n a teflon tweaker mis tunes this so bad it's not funny, and burns u= p in the bargain in the field. So that part was tuned with power off an= d try a little this way and that until it seemed fine.<br /><br />So, gr= ab that paper linked above, and this thread, and doing this will get you= a very versatile and reliable ion source of mostly monatomic ions for y= our fusor or accelerator. As I said above, the next step after this is = for the cavity to be in the tank itself so we maybe don't even need = any explicit ion extraction field at all -- the grid field will probably= do fine at that point.<br /><br />So, that's it, any questions? <di= v class=3D"att_img"><img src=3D"getfile.php?bn=3Dfusor_ionguns&att_id=3D= 6732" alt=3D"TuningStub.jpg" border=3D"0" style=3D'Cursor:HAND;' onclick= =3D"javascript:window.open('showimg.php?url=3Dgetfile.php%3Fbn%3Dfusor_i= onguns%26att_id%3D6732&w=3D819&h=3D1140&title=3DTuningStub.jpg', '', 'sc= rollbars=3D0,toolbar=3D0,resizable=3D1,menubar=3D0,directories=3D0,statu= s=3D0,width=3D819,height=3D1140')" width=3D600 height=3D836></div> = <div class=3D"att_img"><img src=3D"getfile.php?bn=3Dfusor_ionguns&att_id= =3D6733" alt=3D"GasDetail.jpg" border=3D"0" style=3D'Cursor:HAND;' oncli= ck=3D"javascript:window.open('showimg.php?url=3Dgetfile.php%3Fbn%3Dfusor= _ionguns%26att_id%3D6733&w=3D1024&h=3D683&title=3DGasDetail.jpg', '', 's= crollbars=3D0,toolbar=3D0,resizable=3D1,menubar=3D0,directories=3D0,stat= us=3D0,width=3D1024,height=3D683')" width=3D600 height=3D401></div> = ;<div class=3D"att_img"><img src=3D"getfile.php?bn=3Dfusor_ionguns&att_i= d=3D6734" alt=3D"Magnets.jpg" border=3D"0" style=3D'Cursor:HAND;' onclic= k=3D"javascript:window.open('showimg.php?url=3Dgetfile.php%3Fbn%3Dfusor_= ionguns%26att_id%3D6734&w=3D1024&h=3D683&title=3DMagnets.jpg', '', 'scro= llbars=3D0,toolbar=3D0,resizable=3D1,menubar=3D0,directories=3D0,status=3D= 0,width=3D1024,height=3D683')" width=3D600 height=3D401></div> </TD= ></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1262715354'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:kdooley608@rogers.com?= subject=3D[fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>Kevi= n Dooley</a> on <b>2010-05-01 12:15</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Doug<br />I have been studying your ion source, and am a bit puzzled by = the apparent direction of the magnetic field and would like some clarifi= cation please.<br />It seems from the photographs and the arrangement of= the yoke, that the flux is running parallel to the direction of ion flo= w, is this interpretation correct?<br /> Thanks in advance and Regards:<= br />-Kevin </TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1262719367'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:clab@swva.net?subject=3D= [fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>Doug Coulter</= a> on <b>2010-05-01 13:22</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Yes, kind of. The gas and ions flow down the tube in general, but may e= xecute some spirals along the way. That's not what's important.= What is important is that the E field of the RF and the H field be 90 = degrees to one another. The E field is across the tube diameter (loosel= y speaking) and the H is along it.<br /><br />The idea is we make a litt= le cyclotron for any electrons that are free (lots, once it's lit of= f) and whirl them around to bash gas molecules to break them up and knoc= k off further electrons to get monatomic ions. A DC E field along the t= ube length then pushes/pulls the ions into the tank proper. This is why= it's called an ECR type source, which stands for Electron Cyclotron= Resonance. Due to the electrons circling around, they have very long p= aths and can be effective even at pressures where the mean free path is = much larger than the tubing size -- because going in a circle, the elect= ron paths can be very long indeed -- basically till they hit something. = So this source works to pressures far lower than an oversimplified inte= rpretation of Paschens's law would at first indicate. </TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1262719876'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:kdooley608@rogers.com?= subject=3D[fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>Kevi= n Dooley</a> on <b>2010-05-01 13:31</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Thanks Doug.<br />I did some calcs and found the cyclotron diameter to b= e about 4.3 mm at 2.45 ghz.Edit: this calc needs to be re-checked!.<br /= >Nice improvement to the ion sources given in the paper you referenced p= reviously.<br />Thanks again.<br />Kevin.<br /><br />Edit: ( still fumbl= ing in the dark!) Clearly this calc only applies if there were no collis= ions with other particles, the radius inside the wave guide will presuma= bly always be less than this because of collisions and a forced rotation= al frequency. </TD></TR> </TABLE> </td></tr></table> </center>  <br><div align=3Dright><a href=3D"download_thread.php?bn=3Dfusor_ionguns= &thread=3D1263367802" title=3D"Previous thread" onmouseover=3D"windo= w.status=3D'Previous thread';return true" onMouseout=3D"window.status=3D= '';return true" class=3D"wa_link"><img src=3D'images/gauche.gif' border=3D= '0' ALT=3D'Previous thread'></a> | <a href=3D"download_thr= ead.php?bn=3Dfusor_ionguns&thread=3D1231212928" title=3D"Next thread= " onmouseover=3D"window.status=3D'Next thread';return true" onMouseout=3D= "window.status=3D'';return true" class=3D"wa_link"><img src=3D'images/dr= oite.gif' border=3D'0' ALT=3D'Next thread'></a></div>  </td></tr></table> <br> <center><font size=3D\"-1\">Current as of Oct 27, 2011 @ 03:08:04 PM CDT= 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<li><font size=3D-1>2009-21-12 16:01</font> <a href=3D'#N1261432886'><em= >Re: Inverter Microwave for Ion Source RF</em></a> <img src=3D"images/fi= le_types/multiple.gif" border=3D"0" width=3D"15" height=3D"15" align=3D"= absmiddle"> (Doug Coulter) <ul> <li><font size=3D-1>2009-21-12 19:11</font> <a href=3D'#N1261444275'><em= >Re: Inverter Microwave for Ion Source RF</em></a> (lutzhoffman) <ul> <li><font size=3D-1>2009-21-12 21:35</font> <a href=3D'#N1261452945'><em= >Re: Inverter Microwave for Ion Source RF</em></a> (Doug Coulter) </ul> </ul> <li><font size=3D-1>2009-22-12 11:08</font> <a href=3D'#N1261501712'><em= >Re: Inverter Microwave for Ion Source RF</em></a> <img src=3D"images/fi= le_types/image.gif" border=3D"0" width=3D"16" height=3D"16" align=3D"abs= middle" alt=3D"JPG picture"> (Doug Coulter) <ul> <li><font size=3D-1>2009-22-12 16:15</font> <a href=3D'#N1261520147'><em= >Re: Inverter Microwave for Ion Source RF</em></a> (lutzhoffman) <ul> <li><font size=3D-1>2009-22-12 16:44</font> <a href=3D'#N1261521842'><em= >Re: Inverter Microwave for Ion Source RF</em></a> (Doug Coulter) <ul> <li><font size=3D-1>2009-23-12 15:36</font> <a href=3D'#N1261604190'><em= >Re: Inverter Microwave for Ion Source RF</em></a> (lutzhoffman) </ul> </ul> </ul> <li><font size=3D-1>2009-22-12 16:24</font> <a href=3D'#N1261520681'><em= >Re: Inverter Microwave for Ion Source RF</em></a> <img src=3D"images/fi= le_types/image.gif" border=3D"0" width=3D"16" height=3D"16" align=3D"abs= middle" alt=3D"GIF picture"> (Doug Coulter) <li><font size=3D-1>2009-22-12 18:09</font> <a href=3D'#N1261526953'><em= >Re: Inverter Microwave for Ion Source RF</em></a> <img src=3D"images/fi= le_types/multiple.gif" border=3D"0" width=3D"15" height=3D"15" align=3D"= absmiddle"> (Doug Coulter) <ul> <li><font size=3D-1>2010-05-01 12:15</font> <a href=3D'#N1262715354'><em= >Re: Inverter Microwave for Ion Source RF</em></a> (Kevin Dooley) <ul> <li><font size=3D-1>2010-05-01 13:22</font> <a href=3D'#N1262719367'><em= >Re: Inverter Microwave for Ion Source RF</em></a> (Doug Coulter) <ul> <li><font size=3D-1>2010-05-01 13:31</font> <a href=3D'#N1262719876'><em= >Re: Inverter Microwave for Ion Source RF</em></a> (Kevin Dooley) </ul> </ul> </ul> </ul> </ul></div><a name=3D'N1261428592'><br><TABLE BORDER=3D"0" CELLPADDING=3D= "0" CELLSPACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Inverter Microwave for I= on Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:lutz.hoffman@kp.org?su= bject=3D[fusor_ionguns] Inverter Microwave for Ion Source RF'>lutzhoffma= n</a> on <b>2009-21-12 14:49</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Hello:<br /><br />In the interest of building a microwave ion source, = I have been looking for an old microwave to gut for RF parts. Doug Coult= er is currently building exactly such an ion source, and his work in thi= s area is brilliant to say the least. He is much more knowledgeable on t= he subject than I am, and he is kind enough to share his work. Between C= arl, and Doug's work, quality ion sources will soon be a simple buil= d for the amateur. In my opinion this is a fairly profound event, which = may lead to many great discoveries in the future. As far as nuclear phys= ics on an amateur level goes, ion sources ARE a very big deal, and perha= ps the most difficult single component home build.<br /><br />Originally= I planned on using Carl's design, but I soon discovered that it is = very difficult to obtain the required set of RF components, which are sm= all enough to fit inside of the HV terminal of my project, even with the= aid of a small amplifier, like the ones from Communications Concepts. <= br /><br />This is where Doug's idea of using microwaves comes in. W= ith a microwave based ion source the nearly complete set of RF component= s, can be had at the local Walmart for under $50! Better yet they fit in= side of a small space, with simple control circuits. If my ion source we= re at ground potential then I think I would go with Carl's design si= mply because it is the proven, and traditional way to go, with few unkno= wns, or potential issues. So in a nutshell I like both approaches very m= uch, but I want to try Doug's design on this project.<br /><br />I r= ecently scored a working Panasonic Inverter Microwave oven, rated at135= 0W, at the local dump. To my delight it is in perfect working order, the= interior has some burn marks, and a broken glass plate, so the owners m= ust have "assumed" it was toast, or that it was to expensive t= o fix.<br /><br />I very carefully removed all of the innards, being car= eful not to mess anything up. This went very well, I was even able to re= move the control panel leaving it attached. After a short time I was abl= e to get the magnetron to work outside of the oven (While observing RF s= afety measures) just fine. By leaving the factory control circuit attach= ed, I have full control over the output, both in terms of power, and tim= e. My feeling here is that instead of trying to engineer a new control c= ircuit, it would be very easy to just wire an extension from the control= board to the magnetron. I will just have to make a translation table li= ke: 1 Pound Auto Defrost =3D 100uA Beam x 10min, this could be handy : )= <br /><br />What I cannot figure out is the properties of the microwave= output from this Panasonic assembly. Traditional tranny based microwave= s produce a pulsed output, via the HV diode / capacitor circuit. Looking= at the Panasonic inverter based design, I notice that the input 120V 60= Hz, goes into a FW rectifier and is first converted into DC. The DC then= goes into a circuit with what looks like a fairly solid MOSFET, or IGBT= , then to an inductor / small capacitors, and to the HF ferrite transfor= mer, then finally the magnetron. It could be a resonant system. The circ= uit however lacks anything like a substantial HV capacitor which has me = wondering about the nature of the RF output?<br /><br />Some promotional= literature on the net seems to imply that the output is CW? By referenc= ing to a traditional microwaves "pulsed output" being inferior= . My question is: Is the output of this inverter microwave pulsed, or is= it CW? Or if it is pulsed, is it pulsed at very fast rates like in the= KHz range? I do not own a scope so I cannot just figure it out this way= <br /><br />I could not find a clear answer about this question when I r= esearched on the net, which led me to writing this post. For an ion sour= ce CW is normally preferred, but when I think about it the efficiency of= ion sources normally goes up with increased RF power. Thus a fast enoug= h pulsed RF output could be an ideal situation. The higher peak RF energ= y increasing efficiency, while the HF pulsing rate is fast enough to ena= ble easy power measurement, and monitoring. Personally I do not want to = have a 60-120Hz ion source output, but 10 or 20 KHz would be just fine, = and maybe even preferred to CW : )<br /><br />Can anyone shed some light= on this, by explaining the nature of the RF output from an inverter mic= rowave? <br /><br />Thank You.....Lutz </TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1261432886'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:clab@swva.net?subject=3D= [fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>Doug Coulter</= a> on <b>2009-21-12 16:01</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Well, you speak of the devil, and here I am.<br /><br />I own two of tho= se ovens myself, they are fantastic for cooking.<br /><br />No, they are= n't CW, they pulse at 30khz or so. But to reduce power, they reduce= the pulse height/width at that frequency. This looks enough like CW to= the food to make no difference, compared to the old on for a few second= s, off for a few seconds older machines used to control power.<br /><br = />Getting a maggie to go really CW is kind of a trick, and one I guess I= should start writing up for others.<br />My basic idea is far from new,= I copied the basic RF design from a rev-sci-ins article from way back t= here, where they used a medical diathermy source (so they didn't hav= e to figure that part out at all) and were mainly interested in cavity d= esign. I just copied theirs more or less with some slight improvements = of my own, and added the ECR magnets they forgot to put in there for bet= ter performance, and indeed this is better than they claimed by a large = factor. If I can believe my mass spectrometer it makes mostly atomic io= ns, not D2+. I even see that with the mass spec fairly far away from it= in the tank -- I see some D2+ too, but that would be about the amount f= rom some hitting the walls and recombining on the way to the spectromete= r.<br /><br />I am debating whether to make a real long thread entry her= e on "how to make a magnetron that was never meant to run CW do it = anyway" but I'm having second thoughts as it would be pretty lo= ng.<br />You're not going to get there with either the panasonic mag= gie (far too big) or that power supply (completely unsuited for this wor= k on several levels). I am not sure either of the power supplies I'= ve done this with would easily float up to HV, mine are operating near g= round. They wouldn't go into a HV terminal easily at HV unless ther= e's one heck of a fine isolation transformer, or a shaft drive/gener= ator kind of thing around, these things take some real power input, abou= t 80 or 90 watts to run.<br /><br />Lutz, if you wanna email me, I can s= end the sloppy version, I want the one I put up here to be pretty good f= or beginners to follow.<br /><br />But the key is this:<br /><br />Find = a magnetron tube about the *lowest* power you can find -- the panasonic = one is a monster. We just picked a small one from dumpster microwave ov= ens, but they're not expensive at the microwave repair stores either= .<br />You may need to try more than one anyway, as they mode-hop at low= /medium powers, in and out of the resonance of the high Q cavity sometim= es - a small one does this less as there's a lot of stored energy in= the cavity to help keep it from doing that. You must run them very low= power CW, as these have no facility to handle electron buildups and eve= ntually you burn out the ends when the electrons spiral up and down to t= hem, or in some, just build up in the tube cavity and eat RF power and s= top all oscillations. A little tilt on the mag field stops that one, ea= sy, and usually is there by "made sloppy and cheap" for free.<= br /><br />You then need a "constant current" well filtered DC= supply, at pretty low current, 10-20ma max. I've made two, one wit= h standard parts from an oven (but I used a transformer at higher volts = than required for this tube so I could afford to lose some in the filter= ing) and one that uses my H bridge switcher. They both work fine. You = will need a fan on the maggie, the filament power alone will get them ab= ove max spec temperature without one. That's around 33 watts there.= Then you put in maybe another 20-50 watts DC. Above that, things fail= quick, and it's more than you need anyway. <br /><br />It's a = balancing act running this thing right at were it will oscillate at all,= not mode hop, and not burn up, but once you find that point, it works e= very time you flip the switch, very nice -- I've run it for many hou= rs (maybe 100 or more, and many off on cycles), no problems. I am using= a variac in mine with the standard xfrmr, set at about 89 volts....high= er and it mode hops and becomes useless (and burns up) and lower it just= won't oscillate.<br /><br />To make a supply with a standard MOT yo= u need to use a small series cap, on the order of 1/10 the one they norm= ally supply (I am using a .1uf and it's still too big, about half th= at would be better), a series R and another diode/cap (2 uf used here) o= n the output to get decent DC. I am using about 2k series R there and h= ave a neon bulb with it's own ballast across that as a simple curren= t monitor to see if the thing is drawing some current and a rough indica= tion how much. On peaks the drop across 2k/10w R is plenty to light it.= <br /><br />Kind of surprised the board let me put up this 807kb file, b= ut I copied and improved their cavity number 5 -- just a few helpful cha= nges and builder tweaks to keep the arcing down and make it out of easy = to get parts, mainly. Like I said, not many watts input are needed. I = made a yoke and with magnets from amazing magnets to do the ECR part on = this. I adjusted the field with a hall effect meter for the rignt numbe= r in the middle, it goes up on both sides of that, but seems fine and wo= rks fantastic -- I get the thing lit off, and it stays lit to e-6 mbar l= evels -- very nice if you want to run low pressures and not need differe= ntial pumping to keep the rest of your apparatus down there for long mea= n free path.<br /><br />Quartz tubing is a must for this. It works, bar= ely, with pyrex, but needs higher powers, and basically it's the pyr= ex getting very hot and needing a fan. The cavity (1" ID Cu pipe f= rom the hardware store) gets warm, but only warm. I use thin wall 1/2&q= uot; OD quartz for this. I let the gas in via a capillarly tubing in th= e fitting on the outside the tank end.<br /><br />First picture is the t= hing in action, you can see it lighting up the gas. The picture isn'= ;t good enough to show that it's kind of pinched and expands away fr= om the cavity. See fan on maggie tube, that's absolutely required. = This is the business end of the tank, and I put that plexiglass shield = on there to keep arcs from the main feedthrough down.<br /><br />The nex= t pic is the power supply I'm using. It's a standard MOT, with = a wall wart glued on top for fan power. I have kept the original series= cap on there in case I someday want a lot of power, but for now, it'= ;s not hooked up. You can see the end of the white series cap I am usin= g, near the to-220 diodes I series-ed up to get high enough voltage for = this (they are 1.5kv 6a diodes, takes 5 for this use). The big cap on t= he back is the main filter cap, on which the charge is lethal, which is = why it's buried in my rack -- safety, and no I'm not pulling it = out of a working system for pictures!<br /><br /><br />Hope this helps. = Don't tell everyone about the copyright violation that paper repres= ents, just get it quick before we have to take it down.<br /><br />Oh, f= urther issues. I made the endcap on my lathe, and charge that with a po= sitive voltage, and a aluminum tube was turned to fit into the quartz on= the tank end, and extend some beyond this so any sputtering there doesn= 't make the quartz conductive. These are fed from a CCFL inverter w= ith two half wave volt doublers for + and - polarity output, which is co= ntrolled by an adjustable LM 317 on the input of the CCFL inverter. Wor= ks like a champ, and lets you control the amount of ions injected very n= icely and very fast.<br /><br />In my recent record runs, I had to turn = this off. The lm317 puts out enough with the adj terminal grounded to p= ut in too many ions (about +/- 300 volts), and enough just drifted in to= make that mode work. For other modes I use about +/- 3 kv or so, with = about a 33k resistor on both leads for arc protection issues. Those bur= n up before the rest does, kind of a fuse. <div class=3D"att_link"><a hr= ef=3D"getfile.php?bn=3Dfusor_ionguns&att_id=3D6726" title=3D"Download Mi= crowave Discharge Cavities Operating at 2450MHz.pdf (application/pdf - 8= 07.56 Kb)" target=3D"_blank" onMouseover=3D"window.status=3D'Download Mi= crowave Discharge Cavities Operating at 2450MHz.pdf (application/pdf - 8= 07.56 Kb)';return true" onMouseout=3D"window.status=3D'';return true"><i= mg src=3D"images/file_types/pdf.gif" border=3D"0" width=3D"16" height=3D= "16" align=3D"absmiddle" alt=3D"Adobe Acrobat document"><div class=3D"at= t_name">Microwave Discharge Cavities Operating at 2450MHz.pdf</div></a><= div class=3D"att_size">807.56 Kb</div></div> <div class=3D"att_img"= ><img src=3D"getfile.php?bn=3Dfusor_ionguns&att_id=3D6727" alt=3D"uWaveI= onSrc.jpg" border=3D"0" style=3D'Cursor:HAND;' onclick=3D"javascript:win= dow.open('showimg.php?url=3Dgetfile.php%3Fbn%3Dfusor_ionguns%26att_id%3D= 6727&w=3D1024&h=3D683&title=3DuWaveIonSrc.jpg', '', 'scrollbars=3D0,tool= bar=3D0,resizable=3D1,menubar=3D0,directories=3D0,status=3D0,width=3D102= 4,height=3D683')" width=3D600 height=3D401></div> <div class=3D"att= _img"><img src=3D"getfile.php?bn=3Dfusor_ionguns&att_id=3D6728" alt=3D"U= Wavepower.jpg" border=3D"0" style=3D'Cursor:HAND;' onclick=3D"javascript= :window.open('showimg.php?url=3Dgetfile.php%3Fbn%3Dfusor_ionguns%26att_i= d%3D6728&w=3D1024&h=3D683&title=3DUWavepower.jpg', '', 'scrollbars=3D0,t= oolbar=3D0,resizable=3D1,menubar=3D0,directories=3D0,status=3D0,width=3D= 1024,height=3D683')" width=3D600 height=3D401></div> </TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1261444275'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:lutz.hoffman@kp.org?su= bject=3D[fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>lutzho= ffman</a> on <b>2009-21-12 19:11</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Great Reply, Thanks Doug <br /><br />Ok, There is one thing that I jus= t am not getting, sorry, I am not trying to be difficult:<br /><br />If= you feed the microwave ion source with 30Khz pulsed microwaves from an = inverter microwave unit, instead of the normal CW microwave RF, would it= not still function? Instead simply producing an ion beam which pulses a= t 30KHz? <br /><br />I am asking because Sulfur lamps for example are f= ed with pulsed microwaves, and the discharge is not extinguished in betw= een pulses or anything. This has me thinking that if a Sulfur lamp; Whic= h is nothing but a hollow quartz ball filled with low pressure Argon wit= h some elemental Sulfur, works just fine on pulsed microwaves. An ion so= urce is basically the same thing, just with an added magnetic field, and= an extraction electrode. Maybe a RF driven sulfur lamp could even be c= onverted into an ion source, by drilling a gas/extraction hole, and add= ing some magnets? The trouble is the sulfur lamps are hard to find in th= e first place : ) This brings me to another idea, just for fun fill som= e quartz balls with various elements, and energize with RF : ) A Rubid= ium fill focusing on a Nd:YAG rod would be interesting. Anyway back to t= he topic....<br /><br />My thinking here is why not power the ion source= with pulsed microwave RF, if it is fast enough to sustain the discharge= ? If an ion beam pulses at say 10-30KHz, then the beam current could be= averaged out via a capacitor in the faraday cup circuit for an accurate= reading. In other words it would not matter to me if my particle beam p= ulses at 30KHz, as long as I get an high enough average beam current. <b= r /><br />Maybe the ion source could be used both ways: With CW RF for p= recision work, and with pulsed microwave RF for brute force high beam cu= rrent work?<br /><br />Thank you for your thoughts, and for explaining t= he concepts involved.<br /> <br />Aloha.....Lutz : ) </TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1261452945'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:clab@swva.net?subject=3D= [fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>Doug Coulter</= a> on <b>2009-21-12 21:35</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Yes, you'll get a pulsed beam with a 30khz component to it. It won&= #39;t quite match the drive, as some ions get going fast enough to make = more by collisions, the electrons will continue their cyclotron motion f= or awhile, so there's a tail, the length of which depends on a lot o= f things -- how much gas, volume, and so forth. If you use enough extra= ction field, that may do some keep-alive as well.<br /><br />In my case,= I couldn't tolerate the resulting noises as I am studying time-dyna= mics in the fusor just now, and didn't need an additional signal to = have to deal with, or have affect the thing I'm looking at.<br />All= my phenomena don't mind the 2.45 ghz, that's too fast for ions = to do much. And this thing btw makes so little uwave leakage a microwav= e leakage detector that does register the oven I have, just sits on zero= anywhere around it. Nice.<br /><br />Sulfur lamps are designed to be e= asy to light off (most lamps are ;~). This means that they can light of= f on every cycle easy -- and they are dumping real significant power int= o those anyway. They'd be using in the few torr region of gas to pr= omote this, just like merc vapor bulbs do and for the same reason. Low = pressure is a relative term, they are not low in terms of what you need = for accelerator runs, but *many* orders of magnitude higher than that.<b= r /><br />For just making ions, you don't need and can't use hig= h power -- things melt and so on.<br />Note the fan they put on the one = in the paper, for a 75 watt RF source. Mine doesn't need that and m= akes plenty of ions, orders of magnitude more than you'll have the p= ower to accelerate. Or I do, and I have kilowatts for that at much lowe= r volts than your accelerator will need to be interesting.<br />My sourc= e puts out at least 10 ma as configured. That's more than plenty fo= r an accelerator that would typically run in the small uA region at most= .<br /><br />If you try this at the half power minimum the panasonic get= s in near CW, before it reverts to the same old on-off for a couple seco= nds each, your stuff is going to go up in smoke in a rather spectacular = fashion. Even the quartz will melt. That's ~5 times the max power = used in the paper, btw.<br /><br />The beauty of CW operation is that on= ce lit, it will stay lit down to ridiculous low pressures, where over-si= mple armchair theory says "no way, mean free path far too long"= ;. If you let the thing drop, it's hard to start again. Mine seems= to take about 3-4 e-5 mbar or more to start, but will run way below tha= t, but only CW or very fast at any rate -- I tried 70khz and that wasn&#= 39;t fast enough to keep the ions hot until the next pulse. It had to b= e in a gas condition allowing restart every time, more pressure than I t= hink you can tolerate. For a fusor, it's probably fine to pulse if = it's fast -- it will start every cycle at those pressures, I am just= looking at something special and don't want the distraction just no= w.<br /><br />You are going to find that to get high average beam curren= t you'll need something more like DC, not a high peak to average rat= io of pulses.<br />The focus will change with instantaneous current due = to space charge effects, and there will be a maximum you can keep focuse= d to your specification, whatever that is. You don't want high ener= gy particles to almost make it to the target, but hit the tube walls, fo= r example. Ideal focus potential depends on current in ANY beam device,= from CRT's on up. I've acquired a heck of a lot of literature = on all this, and tested a lot of it -- they are not telling lies. Too b= ad I can't upload the nearly 10 gb we've gotten hold of in fusor= /fusion/beam technology papers and related stuff, it's quite the nic= e library.<br /><br />Remember, during off times, gas is still flowing i= nto your accelerator, just not ionized. You're going to have enough= troubles keeping that pressure down low enough to get a mean free path = you need without letting in gas when it's not even getting ionized, = and that's going to be kinda hard to pulse too at those rates. The = big boys all use another vacuum system (called differential pumping whic= h has nothing to do with diffusion pumps) pumping out a space between or= ifices between the source and the accelerator -- the ions go right throu= gh the holes when in focus, the other gas bounces around and gets remove= d, mostly. If you're worried about what you'll need to put in t= he HV terminal....well, a complete additional vac system sounds kind of = troublesome to me. And no, a long quartz tube from ground won't do = it as the gas in there will be highly easy to ionize at that pressure...= .which is why it was AT that pressure to begin with.<br /><br />In fact,= I did all this due to my Scottish repugnance to the idea of another vac= system being needed, and found a way to avoid that need, even for prett= y low tank pressures. At that, it's quite cheap by comparison.<br /= ><br />To be honest, it looks like the source Seltzmann is using might b= e the better one for most fusors, it's certainly simpler to make. I= doubt it lasts as long without maintenance as this one, just because th= is one is pretty phenomenal in that regard -- it's just never failed= in many many runtime hours, and no hint it's degrading in any way a= t all. THAT is cool indeed. </TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1261501712'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:clab@swva.net?subject=3D= [fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>Doug Coulter</= a> on <b>2009-22-12 11:08</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= In answer to a question Roman asked about the transfer of power from the= tube to the cavity:<br /><br />It's not a wave guide, it's a sh= ort (about 1/4 wave) piece of homebrew hardline coax. I don't want = to tear this down just now for pictures, but I can describe it fairly we= ll. A wave guide would have been quite large for this frequency (a coup= le inches across) and had too low an E field in it, with a quarter wave = cavity we can concentrate the E field far higher right where we want it.= So this is all kind of a standard low frequency RF design, just real s= mall. The cavity itself amounts to a 1/4 wave line with one end shorted= and is on the large side for this frequency. Trying to go larger diame= ter would allow other monkey modes to occur in it, rather than the longi= tudinal one we want.<br /><br />The top of the magnetron is the usual an= tenna post, surrounded by the RF ground gasket weaving.<br />I found a C= u pipe adapter that fit that gasket, and was big enough to hold the ante= nna post without clearances being too close. This adapter is brazed int= o a piece of sheet metal so the big end protrudes about 1/8" inch, = and bolting the sheet metal down presses it into the grounded gasket.<br= /><br />Into the top is inserted a piece of 1/2" Cu tubing. Here = in the US we call it pipe if we're talking about specifying the insi= de diameter and tubing if outside. Go figure, it's not a system I i= nvented, just have to live with it.. This is all stuff you can get at L= owes or the local equivalent. I get most things like this at McMaster. = Sad that I had to buy a 25 foot roll of 1/2" tubing to get 2 inche= s, but them's the breaks.<br />A stock of various tubing sizes is su= re handy around the lab anyway.<br /><br />The inner conductor is a piec= e of 1/8" tubing with about a 1/16" ID. One end has a washer = brazed on it, which is then soldered to the end of the "antenna&quo= t; on the tube, using a special flux for SS and nickel from McMaster aga= in. The other end is drilled and tapped for a 4-40 screw, which is the = adjustable length (for coupling to the cavity) part. This wound up more= or less flush with the cavity wall, and the end was "rounded"= or "melted" to eliminate sharp corners that caused arcing. T= rying to tune this while in operation was a joke -- anything you put in = the cavity burns up and mis tunes it, so we had to tune with power off, = try, retune, etc. This coupling adjustment doesn't seem very critica= l at all, since we're running *way* below the tube rated power, some= reflected power is fine as long as nothing arcs and there's enough = forward power coupled. This enters the cavity sort of tangentially like= in the paper (the picture there is all I had to go by myself). Temptin= g to try on the next one to place it closer to the "ground" en= d of the cavity for lower impedance there, but works as it is, near the = hot end just above the quartz tubing hole so it's coupling almost to= the tip of the tuning 1/4 wave stub.<br /><br />This tuning process was= helped a lot by having a DC discharge in the ioniser quartz tubing -- w= hich eventually became the pushme-pullyou ion extractor stuff. You then= always have some light and can tune for "most smoke" more eas= ily. Once it's all tuned, it stays that way really well, I've n= ever re adjusted that parameter for any set of conditions -- it works fi= ne, it ain't broke, and I ain't fixin it no more.<br /><br />The= cavity is about 2" long inside. It's a piece of 1" pipe = (eg one inch ID). I made the top piece which is threaded for a 1/4-20 b= rass tuning stub screw, and that's pretty thick in and outside the c= avity so as to have plenty of thread length, it's about 1/2" or= a little thicker, turned out of 1.25" Cu billet stock. I had to g= rind off the threads and round the end of the screw near the quartz tube= to cut down arcing there. I also put a spring under the screw head, as= this tuning is very twitchy indeed -- the entire range might be 20 degr= ees of turn on that screw.<br /><br />Again, resonance was found by tuni= ng this while there was already a discharge going on in the quartz tubin= g -- it's easy to tell when you get it right that way. Every now an= d then, a tiny jiggle on this screw helps the thing get going in high va= cuum, other than that I never touch it anymore. That's good as in u= se it's very near the HV and I'd rather not "go there"= when in operation.<br /><br />The cavity bottom is a pipe cap for that = size, that I shortened before grooving it and the cavity tubing for the = quartz to pass through -- you can take this off without breaking vacuum.= I drilled and tapped both that cap for 4-40 and the cavity tubing at t= he top for the same screw size so I can take all this apart. I should p= robably just solder the top on now, as that joint is a high current node= in this design and more conductivity is better, it's probably the m= ain loss I now have.<br /><br />Allow me to stress again that you NEED q= uartz tubing. Yes, it will kind of work with pyrex, at about double the= input RF power -- dicey due to arcs, and all that additional power goes= into heating the pyrex, not good. As is, the cavity doesn't need a= fan at all, barely gets hot, never hot enough to burn you. Yes, it'= ;s very clean inside, I did the usual anal prep there, and may silver pl= ate it for fun. It works fine as is, however -- I'll plate it if it= starts corroding in there.<br /><br />A key is finding the "right&= quot; magnetron. this is a smaller one from a junkyard oven. Some mag= netrons do a thing we RF guys call mode hopping (I guess laser guys use = the same term, and it's the same thing). There are usually 8 caviti= es in a magnetron, and never are they all just the same, so sometimes on= e or another will "take control" and it will then go at that f= requency. If that's not the frequency this very high Q cavity happe= ns to be tuned for, it stops working. Some of this is controlled by the= amount of power input, so finding one that doesn't mode hop much at= the desired power level is key. Having it be a smaller tube helps here= too as the amount of stored energy in the cavity can help keep it from = mode hopping better -- we're adding a ninth resonator, a better one = than those in the tube, even under load.<br /><br />It seems to be a luc= k factor, but luckily magnetrons are cheap even bought new. The key, ag= ain is getting a *small* one. We don't need the big power here at a= ll, too much of a good thing is bad for this. Do remember if the power = supply is remoted, even a couple feet, that these are 3.3v at 10 amp fil= aments, you'll need some really fat wire for that. The tube I happe= ned to pull off the shelf is a samsung OM52 series for what it's wor= th -- a very used one. Since it worked fine, I've not run through a= bunch of other types to test them for this, but since there's deman= d, I'll probably wind up making a few more for other people.<br /><b= r />The quartz tubing enters the chamber through a viton o ring coupler = I bought from Lesker, welded into a 1.33" CF flange (which was a tr= ick indeed, but that's what I had on that end flange).<br />That end= has a 1.5" long piece of Al pipe in it, most of that turned down t= o fit into the quartz, with about 1/4" extending from the end, so a= ny sputtering that happens doesn't land on the tubing and make it co= nductive. Al is good for not sputtering BTW as things go.<br /><br />At= the other end of the quartz is a fitting I made of brass that holds an = O ring for sealing, and is bored for a soldered in piece of SS capillary= tubing that is 1.5" long and .007" ID, to control gas flow. = This one's a little short and fat for that, but one I made on anothe= r source was 2" of .005" tubing and it was a little too restri= ctive, to give an idea of the range that works. You have to low temp so= lder this stuff as getting it hot enough to braze will cause some flakey= oxide to form inside the tubing and jam it up, and it's a darn hard= place to clean. The reason to have the gas flow orifice here is so tha= t all the rest of the plumbing can run at or near atmospheric pressure, = so all leaks are "out" rather than dirty shop air leaking &quo= t;in". I have not noticed any sputtering off the end of the SS cap= illary tubing, but hey, it's at the positive polarity side of things= , so shouldn't sputter anyway. Theory does work now and then.<br />= <br />Picture is a closeup of the homebrew hard line. As you can see, I= had to make an adapter to make the 1/2" tubing fit into the pipe a= dapter, and slotted the latter and put a clamp on it to hold things toge= ther. I've never adjusted that length, it's fine just as it was= put together.<br />Drilling that hole in the side of the main cavity wa= s actually the hardest part of all this, not that turning the endcap of = OFHC copper was a breeze, at least that part was thick and sturdy. Pipe= is another issue altogether, and needed a good jig to hold it and caref= ul milling machine work with very light cuts with a 1/2" end mill t= o get that off center oval hole made. I turned a piece of wood down to = keep the vise from crushing the pipe while doing that. The end of the h= ard line that has to be curved to match the cavity curve was done in sim= ilar fashion on the mill, but really you could do that with a round file= good enough without too much fuss.<br /><br />Oh, there's nothing b= ut air in there -- no dielectric at all other than 1.000000x air. <div c= lass=3D"att_img"><img src=3D"getfile.php?bn=3Dfusor_ionguns&att_id=3D673= 0" alt=3D"HardlineDetail.jpg" border=3D"0" style=3D'Cursor:HAND;' onclic= k=3D"javascript:window.open('showimg.php?url=3Dgetfile.php%3Fbn%3Dfusor_= ionguns%26att_id%3D6730&w=3D768&h=3D1152&title=3DHardlineDetail.jpg', ''= , 'scrollbars=3D0,toolbar=3D0,resizable=3D1,menubar=3D0,directories=3D0,= status=3D0,width=3D768,height=3D1152')" width=3D600 height=3D900></div>&= nbsp;</TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1261520147'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:lutz.hoffman@kp.org?su= bject=3D[fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>lutzho= ffman</a> on <b>2009-22-12 16:15</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Thank you so much for taking the time to explain everything, now I am be= gining to understand, at least enough to be willing to take a "wack= at it". <br /><br />Initialy I plan to run my accelerator at about= 150-200KV, this is without any SF-6 insulating gas, with the tube in de= humidified air. The tube should handle this voltage in air at STP. At h= is low energy level I would like to be able to crank up the beam current= big time, up to a maximum of 5-10ma for short times. For most experimen= ts 100-500uA should be fine.<br /><br />The next step will be to ramp up= the KV to the 400-500KV range, this could be done with an SF-6 gas mixt= ure at atmospheric - 2 bar pressure, now the max. beam current would be = about 2-5ma pulsed even for experiments requiring high power. For only 2= -bar, the pressure the vessel can even be PVC irrigation pipe, with an e= quipotential metal rings on the inside surface as well.<br /><br />So in= a nutshell the microwave ion source should work for me "as is"= ; just like Doug designed it. I was thinking about a "hybrid" = design which I call the CAD Ion Source (Carl and Doug). I am wondering i= f Carl's bottom end, and extractor, could be mated to Doug's mic= rowave ion source. At this point I am not familiar with the bottom end o= f Doug's ion source so it is to early to really consider anything li= ke this.<br /><br />One thing I did wonder about is Vicor high silica gl= ass? I know quartz is probably the best as Doug pointed out, but if Vico= r comes close enough, and if it is much superior to Pyrex, then it may b= e worth consideration for some applications, since Vicor can be worked j= ust like normal glass with oxy-propane. But then again it would probabl= y be just as easy to buy a quartz test tube to begin with. Thanks......L= utz </TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1261521842'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:clab@swva.net?subject=3D= [fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>Doug Coulter</= a> on <b>2009-22-12 16:44</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Lutz, <br />you may have focus troubles unless your volt gradient is WAY= steep trying to run that current. You need about 60x the gradient as f= or electrons for D ions for the same amount of beam blooming vs current.= Depending, as always, what you call "focus". TV CRT tubes r= un a few ma at 30kv or so.....you can work it out from there. This is b= ecause the D ions are going slower, so for a given current and volts, th= ere's more in flight next to one another than for electrons at the s= ame volts and amps, and they have more time to repel one another on the = way to the target.<br /><br />Glass "alloys" are just about as= diverse as for steel, it's astonishing how many there are, all char= acterized in the Kohl book on "materials and techniques for vacuum = devices". Or maybe even not all, but it's a heck of a loooonng= chapter.<br /><br />Vycor is one of "those", there are "= flavors". The top grade is quartz, plain and simple -- no differen= ce.<br />Some is kind of porous, and I'd not use that for this, but = you have to ask the source supplier.<br /><br />The reason for this is q= uartz is far lower loss than pyrex glass (DC and AC both), and more resi= stant to being taken apart chemically by hot hydrogen ions. Alumina isn= 't even in the running for this, too lossy by far.<br /><br />Here i= s where we get ours, a small outfit, and nice to deal with too -- they l= ike big orders, though, so people may want to get together and do a grou= p purchase (I will do one for this area if people want me to -- I am usi= ng the stuff up and want more myself).<br /><br /><A Href=3D"http://www= .quartz.com/" target=3D"_blank">http://www.quartz.com/</A><br /><br />I = also use their stuff to make my own HV feedthroughs, having gotten disgu= sted with the commercial versions.<br /><br />I work this with either a = small oxy propane torch I made using a wire welder tip as a gas tip (wor= ks great!) or an oxy-acetylene welder for bigger stuff. You need danger= -sensing sunglasses as it has to be white hot indeed and is blinding to = work on. The regular "didyium" glass blower's glasses are= n't the thing here, they only block the Na lines and you're stil= l blinded. Welding goggles are about right.<br /><br />This design need= s *none* of that, I guess I wasn't clear enough on that yet -- more = pix to come. It's just a cut piece of tubing, easy to cut another s= hould replacement be needed, on the lathe with a tool post grinder and d= iamond wheel. Quartz you can't just score and break like glass. It= comes apart at random if you try, and you might get cut while that expe= nsive stuff gets ruined. I don't even flame polish the ends for thi= s. </TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1261604190'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:lutz.hoffman@kp.org?su= bject=3D[fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>lutzho= ffman</a> on <b>2009-23-12 15:36</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Hello:<br /><br />Thank you so much for all your info on the ion source,= I think I have enough to get going on it when the time comes. I checked= with NEC reference the ion current which the tube can handle, and they = put the max at around 25-50ma with the main limitation being the ion sou= rce flooding the vacuum. Thank you so much for your help : ) I am curiou= s about one remaining thing which is the extraction end of the microwave= ion source? Is it the same as Carl's, or do you just have a small h= ole at the other end of the quartz tube, with an intermediate extraction= electrode close by at - potential? If I understand correctly this is w= here the CFL inverter comes in?<br /><br />An interesting feature of the= tube is built in intermediate focusing electrodes which are located bet= ween each accelerating section. Basicaly they are the same as the first = elecrostatic focusing lens which accepts the ion beam entering the tube.= This gives some control of the ion beam between sections. The entire as= sembly contains 28 electrodes including the entrance, and the other 2 fo= cusing electrodes. My plan is to drive the tube with a 14 stage FWCW mul= tiplier, with 13 equipotential rings, the terminal being connected to th= e 14th stage . I am considering two options on how to connect the tube t= o the VM, the first is: <br /><br />Every other electrode would be conne= cted to the 14 stage VM directly , via a HV resistor. Then the electrode= s in between these would be connected to the driven electrode below it, = also via a different value HV resistor. The question here was do I conne= ct the 14 intermediate electrodes to the VM connected electrode; Above, = or Below it?<br /><br />The second method being considered is to simply = build a 28 stage resistive divider, connected at 28 points to the tube, = and at 14 points to the VM stack?<br /><br />The first method would seem= to be more efficient, but the second would seem like it would have a be= tter potential distibution. My plan is to build the first 6 stages, and = then run the stack at a reduced voltage, and do a bunch of testing : )<b= r /><br />The actual VM stack is fairly well protected with series resis= tors (About 5-10K ohm combined value) between each stage capacitor, in e= ach stack. This is in addition to all of the normal protective measures = like spark gaps, input resistor ect. I am also using 3-4 times the nomal= number of HV diodes, in the first, and in last stages of the VM (In pa= rallel for higher surge current rating) since these diodes will see the = full surge current if a discharge were to occur, which would only be lim= ited by the series resistance of all of the 5-10K ohm protective resisto= rs. <br /><br />Thanks.....Lutz </TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1261520681'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:clab@swva.net?subject=3D= [fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>Doug Coulter</= a> on <b>2009-22-12 16:24</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Here's the simpler of the two power supplies I've built to run t= his. I did use a nominal 4.3 kv transformer to run a nominal 4.1kv tube= , but this may not matter too much. This could be done a little cheaper= than I did; this was all parts I had on hand anyway.<br /><br />I didn&= #39;t modify the transformer, knock out the saturation inducing cores, o= r anything, just used it.<br />In the actual build, I added a wall wart = and 3 terminal regulator for fan power uses. The Variac is adjusted to = about 89 to 91 volts rms output, or about the place where the transforme= r itself begins to saturate with no load. You may be able to substitute= a large incandescent lamp in series instead, but since I haven't tr= ied that yet, I don't know what the wattage would be, probably on th= e order of 250 w.<br /><br />You might be able to make the 2k resistor s= maller (as in 1k), I made it big so I could light that big neon bulb cur= rent draw "analog meter" I used to monitor operation. In that= huge neon bulb (got it at the last HEAS) you can see how much current b= y how much of the big electrode lights up, it's quick to glance at a= nd verify that things are on the bogey.<br /><br />In use, this results = in somewhat lowered filament power and terminal voltage. That's nee= ded to not burn up the tube which was never designed to run CW -- normal= ly the pulse mode lets extra electrons get out of the gap area naturally= and not bombardment-heat the filament too much, in CW they can build up= and make troubles -- a reason no one uses magnetrons for CW work, or ne= arly no one. I have a 12 volt computer case fan strapped to the tube fo= r cooling, and run another one across the general area to keep my HV fee= dthrough cool as it's designed to couple heat from the grid out of t= he tank (this will be another thread later). You *may* be able to run f= ull line volts, but the transformer will then get hot, if you use a smal= ler than .1uf series cap here to limit tube current. But these MOTs run= in saturation (as a voltage regulation feature in a normal oven) and ge= t quite hot if run for long times without a fan, or really even with one= . Here, we just don't need all that. In this design, nothing gets = hot.<br /><br />I also made PS on a ferrite core, using my H bridge desi= gn, but though it works, it's too complex for this, you just don'= ;t need it -- over engineering is as bad as not enough. And by the way,= since those ferrites run at ~8v a turn, you have to then make a stepdow= n transformer and actually rectify the filament voltage, as otherwise th= e crummy lossy chokes inside the magnetron will burn up! Too much for s= omething that is so simple, so I dropped that project. There's just= no need for the complexity.<br /><br />I will try to get cavity details= posted soon, so post any questions you want answered, as that will be t= he last post I make on this -- I will include the ECR magnet design in t= hat one. My next version will have the cavity inside the tank on a 2.75= " CF flange/pipe so the ions can get in there a lot easier, as only= RF and tuning need to go through the wall, both of which should be fair= ly easy (that is, if the type N weld in RF vacuum connectors I got from = Lesker don't give arc troubles). In that design, there won't be= the quartz tube, and the cavity bottom will be Cu or SS screen wire for= the ions to come out, and the RF stay in. I am still pondering how I c= an do adjustable ion extraction field on that one with least fuss.<br />= <br />In my particular version of this, running up the input power makes= it mode hop and go in and out of operation. This isn't a problem, = as it has plenty of RF output well below that point. And of course ther= e's that nice visual indication it's working. You have to see t= his with neon, it's blindingly bright.<br /><br />I seriously doubt = that you can modify an inverter type oven supply to do this -- they only= go to half power on inverter PWM, then revert to on-off operation for l= ower powers -- I think the issue there is that the filament is run off t= he same ferrite transformer and it gets flaky at low filament voltages. = That's 5-10 times the needed RF for this, and too much is BAD for t= his. You'd have to come up with some filament power some way, and f= ool all the fancy feedback loops in that inverter -- I've torn one d= own to see, then put it back together and sold the oven, it's just n= ot worth it. They *are* great for cooking though. <div class=3D"att_img= "><img src=3D"getfile.php?bn=3Dfusor_ionguns&att_id=3D6731" alt=3D"uWave= IonPS.gif" border=3D"0" style=3D'Cursor:HAND;' onclick=3D"javascript:win= dow.open('showimg.php?url=3Dgetfile.php%3Fbn%3Dfusor_ionguns%26att_id%3D= 6731&w=3D1227&h=3D543&title=3DuWaveIonPS.gif', '', 'scrollbars=3D0,toolb= ar=3D0,resizable=3D1,menubar=3D0,directories=3D0,status=3D0,width=3D1227= ,height=3D543')" width=3D600 height=3D266></div> </TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1261526953'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:clab@swva.net?subject=3D= [fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>Doug Coulter</= a> on <b>2009-22-12 18:09</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= OK, here are the rest of the details needed to replicate this, on a virt= ual silver platter.<br /><br />The cavity is a piece of 1" ID coppe= r pipe. It is 2" long, but the effective length is reduced a littl= e by the tuning cap depth of .2365" sticking inside. The tuning st= ub is a brass screw, 1/4-20 threaded into this to stick in .9860" f= or resonance in my setup -- that should get you within one turn if you&#= 39;re using quartz tubing for the gas.<br />The top cap is held in by ti= ght fit and by 3 4-40 screws threaded into the pipe. There is a spring = under the tuning screw head to get rid of backlash and so on. You will = note the screw has it's threads taken off the end, and the end round= ed to cut down arcing issues.<br /><br />The bottom is a pipe cap, short= ened and held on by tight fit and 3 4-40 screws threaded into it.<br /><= br />The gas inlet is a piece of 1/16 od, .007" id SS cap tubing, i= n a brass fitting I turned down to fit, which seals to the quartz by a v= iton o ring. The other O ring you see in the picture is just a cushion = so I don't stress the quartz (it's rough end, I did not flame po= lish it or even grind it flat) -- this makes it trivially easy to replac= e if needed, but this one has run over 100 hours and is still pristine. = This is charged to a positive voltage for ion extraction, via a CCFL in= verter that has variable DC input to control the extraction voltage. Th= is supply is bi-polar (two half wave volt doublers off the same source, = opposite polarity), eg if it's making 1kv positive, it also makes 1k= v negative for the other electrode. I use about a 20k 2w resistor for p= rotecting this from arcs from the nearby HV tank input.<br /><br />Not s= hown in these pictures is a polycarbonate 1/4" thick shield I also = use to keep arcs away from this.<br /><br />The magnets are NdFeB from A= mazing Magnets, with a half inch center hole. I used 1/2" by 1&quo= t; to stick them to, drilled for a little over half inch to let the tubi= ng pass, and 1/8" by 1" iron for the connecting yoke. You can= see in the picture the shim I taped in there after measuring the field = with a hall effect DC magnetometer to 980 gauss or thereabouts. The fie= ld isn't very uniform, but seems fine, and really makes a *huge* dif= ference in how well this works at very low pressures. Once lit off, I&#= 39;ve seen it still run down to 1.4 e-6 mbar, which happened to be the b= ase pressure of the system at that time, due to air infiltration through= the necessary insulating silicone tubing on the gas input. I may try a= nother flavor for that piece, but it has to be there to run the gas inle= t at high positive voltage to repel ions into the tank proper. With ion= extraction volts at max, about 2.5 kv + and -, and a pressure anywhere = above e-3 millibar, this lights off everytime just by turning it on. No= adjustments needed.<br /><br />Not shown, as the tank is under vacuum j= ust now, is the other end of the tubing. At that end, there is a piece = of 1/2' OD aluminum pipe that is turned down to fit inside, all but = about 1/4" of it, and the end is about flush with the magnet closer= to the tank. The other end projects about 1/4" into the tank past= the end of the quartz tubing, so if it sputters, it won't sputter o= nto the quartz. This is hooked to the negative polarity of the ion extr= action supply through the same value protection ressistor, with a wire r= un inside the tank and insulated with alumina beads -- you can see it in= other pictures I've posted here on fusor operation, glowing red in = X rays.<br /><br />The hole you see in the cavity in the last picture is= for tuning the coupling rod length. It's useless more or less, eve= n a teflon tweaker mis tunes this so bad it's not funny, and burns u= p in the bargain in the field. So that part was tuned with power off an= d try a little this way and that until it seemed fine.<br /><br />So, gr= ab that paper linked above, and this thread, and doing this will get you= a very versatile and reliable ion source of mostly monatomic ions for y= our fusor or accelerator. As I said above, the next step after this is = for the cavity to be in the tank itself so we maybe don't even need = any explicit ion extraction field at all -- the grid field will probably= do fine at that point.<br /><br />So, that's it, any questions? <di= v class=3D"att_img"><img src=3D"getfile.php?bn=3Dfusor_ionguns&att_id=3D= 6732" alt=3D"TuningStub.jpg" border=3D"0" style=3D'Cursor:HAND;' onclick= =3D"javascript:window.open('showimg.php?url=3Dgetfile.php%3Fbn%3Dfusor_i= onguns%26att_id%3D6732&w=3D819&h=3D1140&title=3DTuningStub.jpg', '', 'sc= rollbars=3D0,toolbar=3D0,resizable=3D1,menubar=3D0,directories=3D0,statu= s=3D0,width=3D819,height=3D1140')" width=3D600 height=3D836></div> = <div class=3D"att_img"><img src=3D"getfile.php?bn=3Dfusor_ionguns&att_id= =3D6733" alt=3D"GasDetail.jpg" border=3D"0" style=3D'Cursor:HAND;' oncli= ck=3D"javascript:window.open('showimg.php?url=3Dgetfile.php%3Fbn%3Dfusor= _ionguns%26att_id%3D6733&w=3D1024&h=3D683&title=3DGasDetail.jpg', '', 's= crollbars=3D0,toolbar=3D0,resizable=3D1,menubar=3D0,directories=3D0,stat= us=3D0,width=3D1024,height=3D683')" width=3D600 height=3D401></div> = ;<div class=3D"att_img"><img src=3D"getfile.php?bn=3Dfusor_ionguns&att_i= d=3D6734" alt=3D"Magnets.jpg" border=3D"0" style=3D'Cursor:HAND;' onclic= k=3D"javascript:window.open('showimg.php?url=3Dgetfile.php%3Fbn%3Dfusor_= ionguns%26att_id%3D6734&w=3D1024&h=3D683&title=3DMagnets.jpg', '', 'scro= llbars=3D0,toolbar=3D0,resizable=3D1,menubar=3D0,directories=3D0,status=3D= 0,width=3D1024,height=3D683')" width=3D600 height=3D401></div> </TD= ></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1262715354'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:kdooley608@rogers.com?= subject=3D[fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>Kevi= n Dooley</a> on <b>2010-05-01 12:15</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Doug<br />I have been studying your ion source, and am a bit puzzled by = the apparent direction of the magnetic field and would like some clarifi= cation please.<br />It seems from the photographs and the arrangement of= the yoke, that the flux is running parallel to the direction of ion flo= w, is this interpretation correct?<br /> Thanks in advance and Regards:<= br />-Kevin </TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1262719367'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:clab@swva.net?subject=3D= [fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>Doug Coulter</= a> on <b>2010-05-01 13:22</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Yes, kind of. The gas and ions flow down the tube in general, but may e= xecute some spirals along the way. That's not what's important.= What is important is that the E field of the RF and the H field be 90 = degrees to one another. The E field is across the tube diameter (loosel= y speaking) and the H is along it.<br /><br />The idea is we make a litt= le cyclotron for any electrons that are free (lots, once it's lit of= f) and whirl them around to bash gas molecules to break them up and knoc= k off further electrons to get monatomic ions. A DC E field along the t= ube length then pushes/pulls the ions into the tank proper. This is why= it's called an ECR type source, which stands for Electron Cyclotron= Resonance. Due to the electrons circling around, they have very long p= aths and can be effective even at pressures where the mean free path is = much larger than the tubing size -- because going in a circle, the elect= ron paths can be very long indeed -- basically till they hit something. = So this source works to pressures far lower than an oversimplified inte= rpretation of Paschens's law would at first indicate. </TD></TR> </TABLE> </td></tr></table> </center> <a name=3D'N1262719876'><br><TABLE BORDER=3D"0" CELLPADDING=3D"0" CELLSP= ACING=3D"0" WIDTH=3D750 align=3D"center"> <TR><TD BGCOLOR=3D"#000000"> <TABLE BORDER=3D"0" CELLPADDING=3D"5" CELLSPACING=3D"1" width=3D"100%">= <tr><td BGCOLOR=3D"#D0D0FF"> <font size=3D"+1">Subject</i> <b>Re: Inverter Microwave f= or Ion Source RF</b></font><br> <font size=3D"-1"> Posted by <a href=3D'mailto:kdooley608@rogers.com?= subject=3D[fusor_ionguns] Re: Inverter Microwave for Ion Source RF'>Kevi= n Dooley</a> on <b>2010-05-01 13:31</b></font> </th></TR> <TR valign=3D'middle'><TD BGCOLOR=3D'#EEEEEE' style=3D'padding: 15px'>= Thanks Doug.<br />I did some calcs and found the cyclotron diameter to b= e about 4.3 mm at 2.45 ghz.Edit: this calc needs to be re-checked!.<br /= >Nice improvement to the ion sources given in the paper you referenced p= reviously.<br />Thanks again.<br />Kevin.<br /><br />Edit: ( still fumbl= ing in the dark!) Clearly this calc only applies if there were no collis= ions with other particles, the radius inside the wave guide will presuma= bly always be less than this because of collisions and a forced rotation= al frequency. </TD></TR> </TABLE> </td></tr></table> </center>  <br><div align=3Dright><a href=3D"download_thread.php?bn=3Dfusor_ionguns= &thread=3D1263367802" title=3D"Previous thread" onmouseover=3D"windo= w.status=3D'Previous thread';return true" onMouseout=3D"window.status=3D= '';return true" class=3D"wa_link"><img src=3D'images/gauche.gif' border=3D= '0' ALT=3D'Previous thread'></a> | <a href=3D"download_thr= ead.php?bn=3Dfusor_ionguns&thread=3D1231212928" title=3D"Next thread= " onmouseover=3D"window.status=3D'Next thread';return true" onMouseout=3D= "window.status=3D'';return true" class=3D"wa_link"><img src=3D'images/dr= oite.gif' border=3D'0' ALT=3D'Next thread'></a></div>  </td></tr></table> <br> <center><font size=3D\"-1\">Current as of Oct 27, 2011 @ 03:08:04 PM CDT= 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