http://home.earthlink.net/~jimlux/hv/hvwire.htm
With bare conductors, air is the insulator, and clearance distances can be calcuated using standard values for the breakdown of air. A common rule of thumb which is very conservative is 1 inch per 10 kV. Since the breakdown field for air is around 71 kV/inch, this provides a 7:1 safety factor.
Popular insulation materials for hookup type wire are polyethylene, PTFE, rubber, and silicone, particularly the latter. Neon signs are a cost sensitive application, so inexpensive wire ($.15/ft) rated at 15 kV with polyethylene insulation is widely available. Rubber is popular for test leads at the 5 kV level, although many rubbers degrade in the presence of ozone, which is often present in HV equipment. High quality high voltage wire has silicone insulation which is quite flexible and high temperature resistant.Typical prices for silicone insulated wire range from $.20/ft for 10kV rated to $2.00/ft for 50 kV rated.
Corona resistant wire is typically constructed with a central copper core surrounded by a semiconducting sheath, which in turn is surrounded by the insulation. The semiconducting sheath effectively increases the diameter of the wire, reducing the tendency for corona discharge. Suppliers of such wire include Belden, Caton, Tally, etc.
Coaxial cable of the RG-8 (RG-213) family is often used as high voltage cabling for several tens of kV. Grounding the outer shield makes the field distribution inside the cable very even, reducing the field concentrations that start corona. RG-8 is rated at 5 kV RMS, however, the polyethylene insulation is (.285-.01??) .120 inches thick which corresponds to 120 kV breakdown. I suspect that the 5kV rating (7 kV pk) allows for a substantial VSWR in transmission line use without breakdown. Certainly, many systems use RG-8 at 25 kV, and I have seen some at 50 kV using RG-8 as a conductor. Also, the field strength at the inner conductor is higher than that at the outer conductor
Equation here.
Having the outer surface of the cable at ground potential also confers some safety advantages. Don't forget though, that in systems with sufficient stored energy, the coax can literally explode in the event of a dielectric failure. If you have several tens of kJoules stored up, the energy has to go somewhere. At least you won't get shocked, just burned.
Coaxial cable using foamed dielectrics (e.g. RG-8X) are not useful, since the nitrogen used to make the foam has a much lower breakdown than the PE. The same goes for RG-59 cable TV remnants, because they are usually foamed insulation (cheaper and lower loss).
http://www.practicalmachinist.com/vb/general/custom-spark-plug-wires-high-voltage-app-139958/
If you are in the 30,000 V range you do not need insulation surrounding the wire other than for your safety.
You just need support insulators with sufficinent over the surface
length. The short time breakdown voltage of most insulators within the
insulating material is in the range of 300 to 1000 V per 0.001"
thickness. As thickness increases breakdown voltage drops
some. So 30 to 50/1000" of Mylar would be a minimum for 30,000 V.
On the outside of the insulator in dry air the breakdown at standard
conditions is about 3,000,000 V/M. Thus, 1/100 M for 30,000 V or
39.37/100" = 0.4". At lower pressure down to a minimum the distance
increases, and as pressure increases the distance is less.
That is why spark plug gaps are so small.
But over the surface of the insulator will be less than the air breakdown value.
Bannana plugs and jacks are fine. If you have sharp corners cover them
with non-conductive epoxy. High frequency radio insulators may be a
useful support. I used one for a 50,000 V scope input voltage divide
that I made many years ago when working on the development
of an automotive ignition system. The dropping resistor was 6" long to
reduce the voltage gradient along the resistor.
Describe more about what you want to accomplish. Also look inside a color CRT and see what is done there.
Also note above about 10,000 V X-rays are generated. That is the reason for lead in the CRT tubes.
Be careful.
http://www.generalcable.com/NR/rdonlyres/F3629AA7-1B9E-40E6-A74B-4D3949CD1B9B/0/AUT_0060_1002.pdf
The demands on ignition wires are increasing
as a result of higher-revving
engines, higher operating temperatures, exposure to potentially damaging fuels and
chemicals, increased utilization of on-board electronics, and increasing number of
miles driven per year. The additional functional requirements of isolating and
delivering the 30,000 – 50,000 volts required to reliably provide the spark needed
for an internal combustion engine,
Good Better Best
Insulating Properties Silicone EVA EPDM
(Dielectric)
http://www.allaboutcircuits.com/vol_1/chpt_12/8.html
Material* Dielectric strength (kV/inch)
===========================================
Vacuum ------------------- 20
Air ---------------------- 20 to 75
Porcelain ---------------- 40 to 200
Paraffin Wax ------------- 200 to 300
Transformer Oil ---------- 400
Bakelite ----------------- 300 to 550
Rubber ------------------- 450 to 700
Shellac ------------------ 900
Paper -------------------- 1250
Teflon ------------------- 1500
Glass -------------------- 2000 to 3000
Mica --------------------- 5000
* = Materials listed are specially prepared for electrical use.
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http://file.yizimg.com/305304/2012060809264490.pdf
TABLE 2 Dielectric Strength
A
Data Summary From Four Laboratories
Material Thickness Dielectric Strength (V/mil) Standard Coefficient of
(in. nom.) mean max min Deviation Variation (%)
Polyethylene
Terephthalate 0.001 4606 5330 4100 332 7.2
Polyethylene
Terephthalate 0.01 1558 1888 1169 196 12.6
Fluorinated
Ethylene
Propylene 0.003 3276 3769 2167 333 10.2
Fluorinated
Ethylene
Propylene 0.005 2530 3040 2140 231 9.1
PETP fiber
reinforced
epoxy resin 0.025 956 1071 783 89 9.3
PETP fiber
reinforced
epoxy resin 0.060 583 643 494 46 7.9
Epoxy-Glass
Laminate 0.065 567 635 489 43 7.6
Crosslinked
Polyethylene 0.044 861 948 729 48 5.6
Average 8.7
Mike Bushroe
Honeywell Glendale
.As for the high voltage source itself, as Jasper pointed out the Cockcroft-Walton voltage multiplier is simple to build, keeps the components from see the full, final voltage so that lower voltage, much cheaper parts can be used. With 5KV capacitors fairly inexpensive, and microwave oven capacitors cheap and easy to get but rather low in peak voltage we should be able to find affordable parts to build up the voltage:Excellent research there Larry. I ran into that equation today while browsing to find typical capacitor values. But I wasn't willing to dig in to it and try to calculate the size caps we needed. I was still hoping to find somewhere that someone else had done the heavy lifting.
One note, if we really need 30mA into the negative grid on the fusor, at 30KV, that comes to 900 watts of power! The neon sign transformers I am seeing put out 30mA, but at only 7 to 15KV, and that is a half to a quarter the power that we need. We can try a 15KV, 30mA transformer and do a full wave rectifier and voltage doubler to get 30KV DC, but by conservation of energy, that will at best be 15mA, and probably circuit losses will bring that down to 10 to 12mA. That may still be enough for a modest sized fusor, but not the final solution that we want to build up to.
The microwave transformers are good for 700 to 1200 watts delivered, so they would be powerful enough. But even 7KV capacitors in the multiple microfarad range are usually rated in pico farads. It is easy to caps from China that are 0.01uF at 10KV+ for $3 a piece or even less. But the first 10KV 0.1uF capacitor I found is $22 a piece! And that is still one to two orders of magnitude short of what we need for 60Hz input.
So it looks like we will have to chop the power to up the frequency so that we can afford the capacitors. And that probably means AC to DC conversion first, filter capacitors, then 10 to 100Khz chopping and feeding into the voltage multiplier. The big question is how high a voltage do we want the intermediate DC to be? If we could run the chopper directly off a microwave transformer, we would have the power we need, a transformer designed for its input frequency, and the ability to chop the output to make the higher frequency at a voltage we wouldn't need too many sytages to build up to 30KV. However, the best switches for high voltage, high frequency are either MOSFETs, IGBTs, or stacked high voltage JFETs with a standard voltage MOSFET at the bottom, probably to provide rapid cut off. MOSFETs rated to only 4.5KV are $15-$50 and IGBTs of only 4KV are about the same. Where as 500V+ MOSFETs that handle 2A+ are $1 a piece. Unfortunately, this means that a second transformer is needed, that works at both high frequency and high voltage. Iron core transformers, usually the choice for power transformers lose efficiency even at 400Hz, let alone 10Khz. Most high frequency transformers are air-core, which does not have eddie current or hysteresis losses, but tend to have poor magnetic coupling, and are often used for low voltage, audio applications. High frequency, high voltage transformers are sometimes used by ham radio operators, but may be heard to find on short notice. Another possible source is medical or dental X-ray machines. The medical ones tend to have higher voltages and currents and should be able to directly supply the voltage a current we are looking for. The dental ones tend to be lower in voltage and power, but should be good for a modest sized fusor.
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you will not get 10uF out of stacked glass plates that will fit in the building nor layden jars. You will need rolled or stacked mica, with precision cut plates to get this kind of performance. There's a reason caps are expensive.Are you sure you can't live with the DC ripple?
What is the current handling capability of the diodes that you ordered?
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Well, first of all no transformer in the world can sustain its open circuit voltage while under short circuit conditions. Second, you can remove the magnetic shunts like I did with the tesla coil NST. Third, you can find old skool NSTs without the GFI fairly easily still. I have three 12kV 60mA models and a 15kV 30mA core.Is there any reason why we don't use flyback transformers instead? they're much smaller, quite powerful, and can work with much smaller multiplier caps.
On Fri, May 30, 2014 at 9:27 PM, Michael Mathers <
Larry, you are good with about 400-500 watts into the grid. 30 mA is too high at fusing conditions but you may need close to that in earlier operating conditions at lower voltage.
35 KV at 15 mA will get you easily detectable fusion. However, early in operation (prior to fusion) you may need > 20 at lower voltage and higher vacuum pressure. But bottom line is 400-500 Watts. You need to hit that in variable current/voltage conditions targeting 30-35 KV @ 10-15 mA.
In my own research I'm coming to the same conclusion with the NSTs. It will be difficult, although not impossible, to achieve this with NSTs. I have a 9 KV, 60 mA NST that I was planning on using. However, upon learning more about how NSTs are configured I'm not sure it's a road I want to continue to go down. NSTs are magnetically shunted. This is the technique used to effectively current limit the transform at the rated current. Fuck me if I really understand what that means but essentially it means the label of 9000 V, 60mA does not mean what we normally read that to mean. NST cannot sustain their 9000V at full load. The study I've seen show approximately 2/3 power at full load. Under the designed load this makes a lot of sense (neon tubes). A high voltage is initially required to ionize the tube but afterwards a much lower voltage and sustaining current is all that is needed. That's the first problem.Problem #2: Most modern(ish) NSTs are Secondary Ground Fault Protected (ie, local GFI). That needs to either be disabled or the entire transformer needs to be capacitatively isolated (large caps that can support the entire secondary output). Problem #3: Barring that....Any NST 6 KV or over has the center tap grounded to the case chassis. This makes it problematic to get the full output out of the transformer. If you use the transformer end to end the chassis will be floating at (in my case) at 6-7 KV. Not nice (although I may do it anyway). Also, unless the GFI is disabled nor can you just take 120 Hz pulse DC at half the voltage (ground the center and rectify each half) w/o tripping the GFI (it sees unequal load on each of the secondary and trips).
Unless you want to get into switched capacitor voltage multiplication it will be difficult to get to 35 KV at 15 mA.I'm all ears if you have any ideas on how to get a hold of Xray transformers but that doesn't seem particularly appealing to me either (was hoping to avoid lots of oil bath).
I know nothing about MOTs so please share if you have any experience with them.
Michael
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Jasper Nance - KE7PHI
Creative and Scientific Imagery
http://www.nebarnix.com/
When you say etch do you mean like taking the copper off a copper clad board to make a pcb?
That's what I get for posting so soon after I get up. That should be threw instead of through. Would the layers go mylar-insulator-mylar-insulator or insulator-mylar-mylar-insulator?
Is this the design we are making? http://makezine.com/projects/make-36-boards/nuclear-fusor/