Effects of gaps in inductors and transformers

Tony Williams wrote:
In article <vt0tt2pg9i917bcl669h5athguln1bul7p@4ax.com>,
MassiveProng wrote:


On Thu, 22 Feb 2007 21:30:49 -0800, John Larkin
jjlarkin@highNOTlandTHIStechnologyPART.com> Gave us:

Please explain to us what a ferroresonant transformer is for,
and how it works.


The term for today is:
MAG AMP.


Nothing to do with a magnetic amplifier, which is
the active controlling of AC or DC power via a DC
control winding.

A ferroresonant CVT is a passive device and is a
clever design of a core, with a non-saturating
primary limb, a magnetic shunt, and a saturating
secondary limb. The winding on that secondary limb
inherently produces a constant output voltage.
The output is square, (mainly third and fifth
harmonics), and the capacitor is there to resonate-
-out those harmonics. There are even more clever
designs that use compensating windings to reduce the
secondary harmonics.

The CVT is adjusted by "shimming the shunt". I've seen
it done on some special CVT's we were buying, and that
is definitely a black art.

http://www.research.ibm.com/journal/rd/316/ibmrd3106H.pdf
Wow, great link, thanks!

I have the following magamp books:

Nonlinear magnetic control devices, Geyger
Magnetic amplifiers, Storm

these two have small sections on CVTs.

Magnetic amplifier engineering, Attura
Magnetic amplifier analysis, LaFuze
Magnetic amplifier circuits, Geyger
Magnetic amplifiers, Platt
Square Loop Ferrite Core Switching, Neetson
Square Loop Ferrite Core circuitry, Quartly
The Magnetic amplifier, Reyner

none of these even mention ferro-resonant CVTs.

OK its not an exhaustive list of magamp books, but its gotta be getting
close.

Cheers
Terry
 
Paul E. Schoen wrote:
bill.sloman@ieee.org> wrote in message
news:1172141833.429696.85370@v33g2000cwv.googlegroups.com...

On Feb 22, 8:28 am, "Paul E. Schoen" <pst...@smart.net> wrote:

In a thread in SEB there was a discussion on transformer failure modes
that
also mentioned gaps in the magnetic path. I never fully understood the
function of gaps in the core, but I observed that they are generally
present in iron core inductors, but not in most transformers.

I found some information
athttp://www.micrometals.com/appnotes/appnotedownloads/id4hf.pdf, where
it is
explained that the gap size can maximize energy storage in an inductor
by
balancing the point of magnetic saturation (and core heating) with
winding
losses. It seems that a wider (or longer) core gap extends the point of
magnetic saturation by allowing more current to flow through the
windings,
so the effect is to lower the inductance. A smaller gap will have higher
inductance, but will saturate the core much more quickly, resulting in
less
energy storage.

This is not quite the right way to describe what is going on.

The maximum magnetic field you can build up in the magnetic path is
independent of the gap - it is limited by the saturation flux for the
core material. The number of ampere-turns of current through the
winding required to generate that flux depends on the magnetic path
length. The magnetic path length through the core itself is divided by
the relative permeability of the core (about 1000 times air for
ferrites, and 10,000 times air for iron) so even a small air-gap can
dramatically increase the magnetic path length.

A ten-fold increase in magnetic path length allows a ten fold increase
in current through the winding before you ht stuaration, and reduces
the inductance of the assembly by a factor of ten, thus allowing a
factor of ten increase in the energy stored in the inductance (LI^2)
before saturation sets in.



OK. That is very helpful in understanding the principles involved. The gaps
I saw in some large C-core inductors I have are about 0.1", and the
laminated steel has a length of about 10". So if the magnetic path length
is increased to 1000, that is a 100 fold decrease in inductance, allowing
100 times the ampere turns, and thus 100 times the energy. This is a 100 mH
inductor rated about 10 amperes.
usually when designing a flyback style transformer, the input & output
voltages and max duty cycle set the turns ratio.

then choose a core, a switching frequency and the peak flux density (<
Bsat at max Tcore).

then select the primary turns to give the desired Bmax,

Np = Vin*Ton/(Bmax*Ae)

then choose the air gap to give the correct inductance. If the air gap
is -ve, you've picked the wrong core. And unless the gap is very small,
just assume all of the energy is stored in the gap, and use

Lmag = mu_0*Np^2*Ae/l_gap so

l_gap = mu_0*Np^2*Ae/Lmag so

As an inductor is used more for energy storage, a gap (whether actually
cut
in the magnetic material or distributed as with powdered iron), allows
more
energy storage by allowing more current flow, and energy is proportional
to
the square of the current. For a transformer, as I understand it, the
energy is transferred from the primary to secondary by mutual
inductance,
so the absense of a gap results in higher inductance and a higher volts
per
turn.

A gap in a transformer core increases the leakage inductance, which is
usually undesirable.

Moreoever, a transformer isn't usually used as an energy storage
device, so increasing the energy storage capacity is rarely a design
priority.



Thank you for that information. I had posted on SEB that some small
transformers may be made with a gap to make them impedance protected in
case of an output overload or short. There are probably other ways to
achieve this effect with looser coupling. As I had posted there, it comes
at the price of low efficiency and poor regulation, but that's what is
desired for self-protection.


More information can be found
athttp://ece-www.colorado.edu/~ecen4517/course_material/Exp6/Inductor.pdf,
which describes filter inductor design.

I would like to get a better understanding of the characteristics of
transformers and inductors to know how best to design high current 50/60
Hz
transformers as well as switch mode boost converters using inductors.

The transformers I have made use toroidal primary cores with 120/240 VAC
windings, and secondaries consisting of several turns of bus bar or
welding
cable to produce up to 10s of thousands of amps. They will usually
produce
15 to 30 times their nominal output currents for short pulses.

The switch mode boost converter I have designed uses a 10 uH inductor at
100 kHz to boost 12 VDC to 25 or 45 VDC at about 800 mA. However, I
recently found that a small pot core inductor rated at 6.7 amps seemed
to
work better than a larger toroidal inductor rated at 10.8 amps. I think
this might be because the smaller inductor starts to saturate sooner,
lowering its inductance but allowing more current to flow, resulting in
higher energy storage. The larger inductor is probably allowing much
less
current and hence less energy, so it cannot produce the power for the
higher voltage load. I can probably drop the frequency to 75 kHz or 60
KHz
and maybe get the output I need.

At 100kHz you probably need to worry more about inter-winding
capacitance. The detailed structure of the windings can get to be very
important at this sort of frequency. The pot core may well have a two
or four section former with the windings built up as two or four
successive sections, while the toriod is more likely to have its
windings built up as successive layers, one on top of another, which
gives a higher winding capacitance and a lower self-resonant
frequency.

At even higher frequencies, you have to restrict yourself to single-
layer windings to keep the interwinding capacitance within bounds, and
eventually you have to go over to transmission line transformers.



The toroid has only about 10 turns of approx #16 wire on a core about 0.75"
x 0.37". I don't know the internal construction of the pot core, but it is
only about 0.5" square and 0.3" high. It most likely has several layers of
windings.

Thanks,

Paul
 
bill.sloman@ieee.org wrote:
On Feb 23, 12:41 am, MassiveProng
MassivePr...@thebarattheendoftheuniverse.org> wrote:

On 22 Feb 2007 02:57:13 -0800, bill.slo...@ieee.org Gave us:


A gap in a transformer core increases the leakage inductance, which is
usually undesirable.

The gaps are very small. For pot cores, it can be anywhere from
half a mil to around 5 or even 10 mils. Without it, problems do
occur.




Moreoever, a transformer isn't usually used as an energy storage
device, so increasing the energy storage capacity is rarely a design
priority.

In a switcher, it keeps the crossover from banging into each other.
A big source of switcher noise, and LOST efficiency.


This sounds like nonsense to me. For simple, centre-tapped windings a
high leakage inductance, corresponding to poor coupling between the
two sides of the centre-tapped winding, leads to a higher turn-off
dissipation, which can be a major source of lost efficiency, not to
mention over-heated switching transistors.

What you seem to be thinking off would seem to be shoot-through
losses, which are best dealt with by a break-before-make switch
driver.

--
Bill Sloman, Nijmegen
nah, peak current mode control cures all manner of ills. And of course
some design skill ;)

Cheers
Terry
 
In article <1172395738.822203@ftpsrv1>,
Terry Given <my_name@ieee.org> wrote:

http://www.research.ibm.com/journal/rd/316/ibmrd3106H.pdf

Wow, great link, thanks!
Isn't it just. Best I could find quickly.

I have the following magamp books:
Nonlinear magnetic control devices, Geyger
Magnetic amplifiers, Storm
My (one and only) mag amp bible is:-

"Self Saturating Magnetic Amplifiers"
by Lynn, Pula, Ringelman, and Timmel.
Published in 1960 by McGraw-Hill.
Lib Congress Card Number = 60-6979.

It is a serious tome, and the authors were apparently
staffers at the Westinghouse Electric Corp, Air Arm
Division, Baltimore. Inventors of "mag amp?".

Looks like I borrowed it from the Decca Radar Research
Laboratories, (in 1967), and forgot to return it. :)

Amazon has one copy, at $80.

none of these even mention ferro-resonant CVTs.
I don't see why a mag amp book should mention the
ferroresonant CVT. OK, the CVT does have a limb
that saturates, but there is no control winding
and it operates as a passive device.

OK its not an exhaustive list of magamp books, but its gotta be
getting close.
--
Tony Williams.
 
"Paul E. Schoen" <pstech@smart.net> wrote in message
news:45dd4643$0$6831$ecde5a14@news.coretel.net...

[snip]

Thanks for any thoughts and discussion.

Paul
You need the following sums

L = uoueN^2Ae/Le

B = uoueNI/Le

H = NI/Le

dI = VinTon/L


You are not allowed to use one sum without thinking about how it might
affect another one. You avoid that sort of sophistry by using all the sums
to find your answer.

The B field don't depend on the core.

Choice 1) Do Sums.
Choice 2) Use sophistry to prove it does.

Subsequently

Choice 1) Problem Solved.
Choice 2) Invoke 'Ad Hominem' Attack strategy.

A gap affects ue. There is something about permeance and reluctance which is
something like conductance and resistance. The gap appears in series with
things so/but you get the answer by adding the reluctances.

Unfortunately designing magnetic components is hard because there are too
many variables to play with.

N = LI/BAe

Works

But then you might need

AwAe = LIpkIrms/BpkJK

To get a first guess at what the size of your core should be. J and K are
the guesses.... and then Bpk ignores the core loss so you might adjust
something else for another guess. J ignores the winding losses so..... you
might have to guess again.

Do you trust the software?

Leakage inductance has nothing to do with uncoupled flux. It's down to
energy stored in the field(s) between the windings, series term.

If you want to control stuff then you might control the coupling of the flux
and that is a parallel thing.

DNA
 
On Sun, 25 Feb 2007 22:21:01 +1300, Terry Given <my_name@ieee.org>
wrote:

John Larkin wrote:
On Fri, 23 Feb 2007 17:55:37 -0800, MassiveProng
MassiveProng@thebarattheendoftheuniverse.org> wrote:


On Fri, 23 Feb 2007 17:21:52 -0800, John Larkin
jjlarkin@highNOTlandTHIStechnologyPART.com> Gave us:


On 23 Feb 2007 19:54:24 GMT, Robert Latest <boblatest@yahoo.com
wrote:


John Larkin wrote:


I can imagine a geometry in which increasing a gap reduces leakage
inductance.

What would that be? Leakage inductance is caused by flux that doesn't go
through all windings. How could any form of air gap keep more flux inside
the windings?


Your question practically answers itself.


Is that then a recursive loop, or an eddy current?

Oh... that's right... it's a TardCurrent wave.


It's obvious you know almost nothing about magnetics, other than
having some hunches based on working around people who do. That's
fine, but why do you pretend to know stuff that you obviously don't?

If you did understand this stuff, you would have answered my simple
question.

John


X increases.

Cheers
Terry
Correct. Missing Prong couldn't even figure that, the easy part, out.

What happens to flux density?

John
 
On Sat, 24 Feb 2007 09:48:40 -0800, MassiveProng
<MassiveProng@thebarattheendoftheuniverse.org> wrote:

On Sat, 24 Feb 2007 08:51:44 -0800, John Larkin
jjlarkin@highNOTlandTHIStechnologyPART.com> Gave us:

On Fri, 23 Feb 2007 17:38:03 -0800, MassiveProng
MassiveProng@thebarattheendoftheuniverse.org> wrote:


An arc welder is ALWAYS a short circuit when there is a plasma arc
struck up, and during its entire duration. There is virtually no
difference between the resistance of the plasma, and a dead short.

Then from where comes the energy to do the welding?


The plasma, and the molten steel are a resistor. The current going
though said resistor gets dissipated as heat at the resistor site,
which is the tip, and the work (weld) location.
So tha plasma is a short, and the plasma is a resistor.

Thanks for explaining that to us.

John
 
On Sun, 25 Feb 2007 05:47:13 +0000 (UTC), don@manx.misty.com (Don
Klipstein) Gave us:

In article <gfu0u2dh20ie72ltbfbv9411ji5nio86vq@4ax.com>, MassiveProng wrote:
On Sat, 24 Feb 2007 08:51:44 -0800, John Larkin
jjlarkin@highNOTlandTHIStechnologyPART.com> Gave us:

On Fri, 23 Feb 2007 17:38:03 -0800, MassiveProng
MassiveProng@thebarattheendoftheuniverse.org> wrote:


An arc welder is ALWAYS a short circuit when there is a plasma arc
struck up, and during its entire duration. There is virtually no
difference between the resistance of the plasma, and a dead short.

Then from where comes the energy to do the welding?


The plasma, and the molten steel are a resistor. The current going
though said resistor gets dissipated as heat at the resistor site,
which is the tip, and the work (weld) location.

It's mostly in the voltage drop of the arc, mainly in the cathode fall
and anode fall regions of the arc.
True, the arc will not limit current, but it has a voltage drop. The
arc somewhat simulates a hypothetical zener diode with a negative
temperature coefficient.
It also has to be in the work contact area itself as well, otherwise
there would be no heat, no puddles of steel to weld with.
 
On Sun, 25 Feb 2007 09:50:30 -0800, John Larkin
<jjlarkin@highNOTlandTHIStechnologyPART.com> Gave us:

On Sun, 25 Feb 2007 22:21:01 +1300, Terry Given <my_name@ieee.org
wrote:

John Larkin wrote:
On Fri, 23 Feb 2007 17:55:37 -0800, MassiveProng
MassiveProng@thebarattheendoftheuniverse.org> wrote:


On Fri, 23 Feb 2007 17:21:52 -0800, John Larkin
jjlarkin@highNOTlandTHIStechnologyPART.com> Gave us:


On 23 Feb 2007 19:54:24 GMT, Robert Latest <boblatest@yahoo.com
wrote:


John Larkin wrote:


I can imagine a geometry in which increasing a gap reduces leakage
inductance.

What would that be? Leakage inductance is caused by flux that doesn't go
through all windings. How could any form of air gap keep more flux inside
the windings?


Your question practically answers itself.


Is that then a recursive loop, or an eddy current?

Oh... that's right... it's a TardCurrent wave.


It's obvious you know almost nothing about magnetics, other than
having some hunches based on working around people who do. That's
fine, but why do you pretend to know stuff that you obviously don't?

If you did understand this stuff, you would have answered my simple
question.

John


X increases.

Cheers
Terry

Correct. Missing Prong couldn't even figure that, the easy part, out.
I stated it, dumbfuck!

I also stated that despite the SMALL loss such a gap makes, the
benefits outweigh it.

You simply ignored the response, you retarded BASTARD.

What happens to flux density?

You probably wouldn't know.
 
On Sun, 25 Feb 2007 09:53:26 -0800, John Larkin
<jjlarkin@highNOTlandTHIStechnologyPART.com> Gave us:

On Sat, 24 Feb 2007 09:48:40 -0800, MassiveProng
MassiveProng@thebarattheendoftheuniverse.org> wrote:

On Sat, 24 Feb 2007 08:51:44 -0800, John Larkin
jjlarkin@highNOTlandTHIStechnologyPART.com> Gave us:

On Fri, 23 Feb 2007 17:38:03 -0800, MassiveProng
MassiveProng@thebarattheendoftheuniverse.org> wrote:


An arc welder is ALWAYS a short circuit when there is a plasma arc
struck up, and during its entire duration. There is virtually no
difference between the resistance of the plasma, and a dead short.

Then from where comes the energy to do the welding?


The plasma, and the molten steel are a resistor. The current going
though said resistor gets dissipated as heat at the resistor site,
which is the tip, and the work (weld) location.

So tha plasma is a short, and the plasma is a resistor.

Thanks for explaining that to us.
Do us a favor, John. Go outside and get struck by lightning, and
then tell me how little difference there is between that plasma
stroke, and a short.

There are a series of resistances involved. The rod, the plasma
arc, the weld spot molten liquid puddle, and you brain, boy!
 
John Larkin wrote:
On Sun, 25 Feb 2007 22:21:01 +1300, Terry Given <my_name@ieee.org
wrote:


John Larkin wrote:

On Fri, 23 Feb 2007 17:55:37 -0800, MassiveProng
MassiveProng@thebarattheendoftheuniverse.org> wrote:



On Fri, 23 Feb 2007 17:21:52 -0800, John Larkin
jjlarkin@highNOTlandTHIStechnologyPART.com> Gave us:



On 23 Feb 2007 19:54:24 GMT, Robert Latest <boblatest@yahoo.com
wrote:



John Larkin wrote:



I can imagine a geometry in which increasing a gap reduces leakage
inductance.

What would that be? Leakage inductance is caused by flux that doesn't go
through all windings. How could any form of air gap keep more flux inside
the windings?


Your question practically answers itself.


Is that then a recursive loop, or an eddy current?

Oh... that's right... it's a TardCurrent wave.


It's obvious you know almost nothing about magnetics, other than
having some hunches based on working around people who do. That's
fine, but why do you pretend to know stuff that you obviously don't?

If you did understand this stuff, you would have answered my simple
question.

John


X increases.

Cheers
Terry


Correct. Missing Prong couldn't even figure that, the easy part, out.

What happens to flux density?

John
Rather than a waffly story, herewith the full technical description:

bugger all.

Cheers
Terry
 
Tony Williams wrote:
In article <1172395738.822203@ftpsrv1>,
Terry Given <my_name@ieee.org> wrote:


http://www.research.ibm.com/journal/rd/316/ibmrd3106H.pdf


Wow, great link, thanks!


Isn't it just. Best I could find quickly.


I have the following magamp books:
Nonlinear magnetic control devices, Geyger
Magnetic amplifiers, Storm


My (one and only) mag amp bible is:-

"Self Saturating Magnetic Amplifiers"
by Lynn, Pula, Ringelman, and Timmel.
Published in 1960 by McGraw-Hill.
Lib Congress Card Number = 60-6979.

It is a serious tome, and the authors were apparently
staffers at the Westinghouse Electric Corp, Air Arm
Division, Baltimore. Inventors of "mag amp?".

Looks like I borrowed it from the Decca Radar Research
Laboratories, (in 1967), and forgot to return it. :)
:)

I sorta did that with a library book I really liked once. Told them i
lost it, and paid for it ($50 or so IIRC). miraculously turned up
shortly thereafter, but I figure its mine now, and I have the receipt to
prove it :)


and once during a pay review, when I said I wanted more and my boss said
"theres no more money" I ended up convincing him to give me a $1k per
annum book budget, I keep the books but make them available at work.
Thats why I have a copy of Snelling (and Bozorth)

Amazon has one copy, at $80.
I'll add it to my list of books to look for.

none of these even mention ferro-resonant CVTs.


I don't see why a mag amp book should mention the
ferroresonant CVT. OK, the CVT does have a limb
that saturates, but there is no control winding
and it operates as a passive device.


OK its not an exhaustive list of magamp books, but its gotta be
getting close.
Cheers
Terry
 
"Terry Given" <my_name@ieee.org> wrote in message
news:1172436914.204310@ftpsrv1...
John Larkin wrote:
Correct. Missing Prong couldn't even figure that, the easy part, out.

What happens to flux density?

John

Rather than a waffly story, herewith the full technical description:

bugger all.

Cheers
Terry
Amen.

DNA
 
On Fri, 23 Feb 2007 17:58:29 -0800, MassiveProng
<MassiveProng@thebarattheendoftheuniverse.org> wrote:

On Fri, 23 Feb 2007 17:41:42 -0800, John Larkin
jjlarkin@highNOTlandTHIStechnologyPART.com> Gave us:

On Fri, 23 Feb 2007 17:21:46 -0800, MassiveProng
MassiveProng@thebarattheendoftheuniverse.org> wrote:

On Fri, 23 Feb 2007 09:25:09 -0800, John Larkin
jjlarkin@highNOTlandTHIStechnologyPART.com> Gave us:

On Thu, 22 Feb 2007 22:02:20 -0800, MassiveProng
MassiveProng@thebarattheendoftheuniverse.org> wrote:

On Thu, 22 Feb 2007 21:29:09 -0800, John Larkin
jjlarkin@highNOTlandTHIStechnologyPART.com> Gave us:

OK, say we have an ungapped iron-core transformer, with some fixed AC
voltage and frequency applied to a primary winding. Primary
ampere-turns are some value X. Now add an air gap. What happens to X?

Whatever x becomes, it certainly becomes ALLOWED to have a higher
ceiling than without the gap. You need to realize that. The gap
allows the drive to be greater, despite the tiny loss incurred.
Without it, the ceiling for saturation is MUCH lower! Pretty simple
shit.

Gaineth thy selfeth a clue.

Answer the question.

John



X drops a LITTLE BIT, you fucking retard (inferred in my post)! Now
observe what I said above about being able to drive it harder to make
up for, and even surpass your petty claim of severe losses.
Sorry, wrong guess. X, ampere-turns, will increase as air gap is
added. Magnetic path gets longer, reluctance goes down, inductance
goes down, amps increase, turns stay constant.

Did I mention severe losses? Or any losses? I don't recall doing that.

John
 
"Terry Given" <my_name@ieee.org> wrote in message
news:1172437170.111149@ftpsrv1...
Tony Williams wrote:
In article <1172395738.822203@ftpsrv1>,
Terry Given <my_name@ieee.org> wrote:


http://www.research.ibm.com/journal/rd/316/ibmrd3106H.pdf


Wow, great link, thanks!


Isn't it just. Best I could find quickly.


I have the following magamp books:
Nonlinear magnetic control devices, Geyger
Magnetic amplifiers, Storm


My (one and only) mag amp bible is:- "Self Saturating Magnetic
Amplifiers"
by Lynn, Pula, Ringelman, and Timmel.
Published in 1960 by McGraw-Hill.
Lib Congress Card Number = 60-6979.
It is a serious tome, and the authors were apparently
staffers at the Westinghouse Electric Corp, Air Arm
Division, Baltimore. Inventors of "mag amp?".

Looks like I borrowed it from the Decca Radar Research
Laboratories, (in 1967), and forgot to return it. :)


:)

I sorta did that with a library book I really liked once. Told them i
lost it, and paid for it ($50 or so IIRC). miraculously turned up shortly
thereafter, but I figure its mine now, and I have the receipt to prove it
:)


and once during a pay review, when I said I wanted more and my boss said
"theres no more money" I ended up convincing him to give me a $1k per
annum book budget, I keep the books but make them available at work.
Thats why I have a copy of Snelling (and Bozorth)

Amazon has one copy, at $80.

I'll add it to my list of books to look for.



none of these even mention ferro-resonant CVTs.


I don't see why a mag amp book should mention the
ferroresonant CVT. OK, the CVT does have a limb
that saturates, but there is no control winding
and it operates as a passive device.


OK its not an exhaustive list of magamp books, but its gotta be
getting close.



Cheers
Terry
I once tried using a saturable core reactor to dynamically regulate the
current through a recloser, which changes its inductance by a factor of as
much as 3 during its operation (a steel plunger is pulled into a current
sensing coil against a hydraulic piston). It proved to be impractical
because the control current had to be changed within a few cycles,
requiring a very high power source, and also because it distorted the
waveform excessively.

The problem was solved partly by using series resistance, which greatly
stabilized the current because it was in quadrature to the changing
reactance. I obtained a patent on the improved recloser test set in 1980.
The most successful solution, however, was using digital sampling and
computing the true-RMS value over the entire decaying waveform. More
discussion of recloser testing is on my website: www.pstech-inc.com.

Here is a link to a site describing a saturable core reactor made from a
microwave oven transformer:

http://www.geocities.com/aaawelder/reactor.html

It seems the output AC current is roughly proportional to the DC current
through the saturable core. The principles are explained simply here:

http://en.wikipedia.org/wiki/Saturable_reactor
http://en.wikipedia.org/wiki/Magnetic_amplifier
http://en.wikipedia.org/wiki/Constant_voltage_transformer#AC_voltage_stabilizers

Paul
 
In article <spo3u25cck1ddr550snvg5dishol9nd0su@4ax.com>, MassiveProng wrote:
On Sun, 25 Feb 2007 05:47:13 +0000 (UTC), don@manx.misty.com (Don
Klipstein) Gave us:

In article <gfu0u2dh20ie72ltbfbv9411ji5nio86vq@4ax.com>, MassiveProng wrote:
On Sat, 24 Feb 2007 08:51:44 -0800, John Larkin
jjlarkin@highNOTlandTHIStechnologyPART.com> Gave us:

Then from where comes the energy to do the welding?

The plasma, and the molten steel are a resistor. The current going
though said resistor gets dissipated as heat at the resistor site,
which is the tip, and the work (weld) location.

It's mostly in the voltage drop of the arc, mainly in the cathode fall
and anode fall regions of the arc.
True, the arc will not limit current, but it has a voltage drop. The
arc somewhat simulates a hypothetical zener diode with a negative
temperature coefficient.

It also has to be in the work contact area itself as well, otherwise
there would be no heat, no puddles of steel to weld with.
The puddles of steel are molten by heat from the cathode fall and anode
fall mechanisms of the arc. The molten steel does not have enough
resistance to generate that kind of heat from that kind of current - see
what happens if you touch the welding rod to the work. Try that with a
voltmeter across the work and the welding rod, and see how much of the
voltage drop is in the arc and how much is not.

- Don Klipstein (don@misty.com)
 
"Genome" <mrspamizgood@yahoo.co.uk> wrote in message
news:rXjEh.26460$OK6.25334@newsfe4-win.ntli.net...
"Paul E. Schoen" <pstech@smart.net> wrote in message
news:45dd4643$0$6831$ecde5a14@news.coretel.net...

[snip]


Thanks for any thoughts and discussion.

Paul


You need the following sums

L = uoueN^2Ae/Le

B = uoueNI/Le

H = NI/Le

dI = VinTon/L


You are not allowed to use one sum without thinking about how it might
affect another one. You avoid that sort of sophistry by using all the
sums to find your answer.

The B field don't depend on the core.

Choice 1) Do Sums.
Choice 2) Use sophistry to prove it does.

Subsequently

Choice 1) Problem Solved.
Choice 2) Invoke 'Ad Hominem' Attack strategy.

A gap affects ue. There is something about permeance and reluctance which
is something like conductance and resistance. The gap appears in series
with things so/but you get the answer by adding the reluctances.

Unfortunately designing magnetic components is hard because there are too
many variables to play with.

N = LI/BAe

Works

But then you might need

AwAe = LIpkIrms/BpkJK

To get a first guess at what the size of your core should be. J and K are
the guesses.... and then Bpk ignores the core loss so you might adjust
something else for another guess. J ignores the winding losses so.....
you might have to guess again.

Do you trust the software?

Leakage inductance has nothing to do with uncoupled flux. It's down to
energy stored in the field(s) between the windings, series term.

If you want to control stuff then you might control the coupling of the
flux and that is a parallel thing.

DNA
I don't think I need to go through all that calculation, especially when I
am using off the shelf components (but I appreciate the information). The
actual circuit performance and waveforms closely match what I see in
LTspice. I was just surprised that the toroidal inductor rated at higher
current did not produce as much output power. It may be that the smaller
inductor (Sumida CDR127/LD100) may have more effective gap and thus allow
higher current than the larger toroid (Miller 2101-H-RC). I have ordered 8
pieces of the board, and will soon be able to test them. They are designed
so I can use either the on-board SMT inductor, or an external toroid, or
both in parallel.

Basically, I can predict the maximum current in the inductor, and hence the
energy stored, vs frequency. Using LTspice with a 61 ohm load, I found that
at 200 kHz and 70% duty cycle the maximum inductor current with 12 VDC at
10 uH is 4.4A (Energy = 97 uW-sec * 0.2 = 19.4 W), and I get 40 volts (26.2
W). At 100 kHz, I can get 48 volts (37.7W) with a maximum inductor current
of 8 A (32 W). The actual inductor current in the first case, which is
running in continuous mode, includes a DC component of 650 mA from the 12
volt source. Adding that gives a power contribution from the battery of 7.8
watts in the first case and 9.4 watts in the second.

The maximum output will be generated when the inductor starts charging
again after its energy has been discharged into the output capacitor, so
there will be no "dead time". With 12 volts, the inductor charges to 8.4 A
in 7 uSec, and it takes 3 uSec to charge the output capacitor, for 70% duty
cycle. The output is about 48 VDC into 61 ohms, or 38 watts. I calculate
the average input power to be about 70% of sqrt(8.4*8.4/2) * 12 V = 35.3
watts, plus the 780mA * 12V = 9.4W from the battery, or 44.7. I'm guessing
at this, but the simulator measured input watts to be 43, so I'm close.
This is 82% efficiency.

I'm running simulations in LTspice, and I think they are pretty much
correct, but I am still a little puzzled. In the continuous mode operation
at 200 kHz, I can see the DC component through the inductor as a 388 mA
minimum current. I get input power of 28.77 W and output of 25.77 W or
89.5% efficiency. In the discontinuous mode at 100 kHz, I get 38.7 watts
out, 43.1 watts in, and 89.8% efficiency. However, I have a hard time
grasping how it can output 38.7 watts when there is almost no inductor
current (It's actually negative) 10% of the time, and peak energy of 320
uW-Sec at 100 kHz or 32 watts. Maybe I'm simplifying the calculation too
much. The true power is probably the integral of the peak energy
(0.5*I^2*L) over the entire waveform, times frequency. OK, when I do that,
I get an average of about 98 uJ, but a peak of 316 uJ = 31.6 W.

BTW, a good reference for transformers, inductors, and other AC devices is:
http://www.ibiblio.org/obp/electricCircuits/AC/AC_9.html

The entire series is very good.

Paul
 
On Mon, 26 Feb 2007 02:16:23 +0000 (UTC), don@manx.misty.com (Don
Klipstein) Gave us:

In article <spo3u25cck1ddr550snvg5dishol9nd0su@4ax.com>, MassiveProng wrote:
On Sun, 25 Feb 2007 05:47:13 +0000 (UTC), don@manx.misty.com (Don
Klipstein) Gave us:

In article <gfu0u2dh20ie72ltbfbv9411ji5nio86vq@4ax.com>, MassiveProng wrote:
On Sat, 24 Feb 2007 08:51:44 -0800, John Larkin
jjlarkin@highNOTlandTHIStechnologyPART.com> Gave us:

Then from where comes the energy to do the welding?

The plasma, and the molten steel are a resistor. The current going
though said resistor gets dissipated as heat at the resistor site,
which is the tip, and the work (weld) location.

It's mostly in the voltage drop of the arc, mainly in the cathode fall
and anode fall regions of the arc.
True, the arc will not limit current, but it has a voltage drop. The
arc somewhat simulates a hypothetical zener diode with a negative
temperature coefficient.

It also has to be in the work contact area itself as well, otherwise
there would be no heat, no puddles of steel to weld with.

The puddles of steel are molten by heat from the cathode fall and anode
fall mechanisms of the arc. The molten steel does not have enough
resistance to generate that kind of heat from that kind of current - see
what happens if you touch the welding rod to the work. Try that with a
voltmeter across the work and the welding rod, and see how much of the
voltage drop is in the arc and how much is not.

The arc is as hot as the sun's surface, and where it hits the steel,
it melts the flux on the end of the rod, and the rod's steel melts,
and the arc entry/exit point at the work site heats. The fact that
the rod tip became molten is hot enough to take a small portion of the
surface, that being the work site over the edge and they meld, all in
a few fractions of a second, then on to the next bulb of hot steel off
the rod tip. Stack em along a seam and you have a weld. In this
case, an arc weld.
 
"MassiveProng" <MassiveProng@thebarattheendoftheuniverse.org> wrote in
message news:ksq3u2dvabp0bruc6v5a016kn6hancvp77@4ax.com...
Do us a favor, John. Go outside and get struck by lightning, and
then tell me how little difference there is between that plasma
stroke, and a short.
Not much of one, considering the cloud started at eight hundred fucking
million volts. ;-)

Tim

--
Deep Fryer: A very philosophical monk.
Website @ http://webpages.charter.net/dawill/tmoranwms
 
On a sunny day (Sun, 25 Feb 2007 18:09:17 -0500) it happened "Paul E. Schoen"
<pstech@smart.net> wrote in <45e21721$0$6816$ecde5a14@news.coretel.net>:

Here is a link to a site describing a saturable core reactor made from a
microwave oven transformer:

http://www.geocities.com/aaawelder/reactor.html

It seems the output AC current is roughly proportional to the DC current
through the saturable core. The principles are explained simply here:

Interesting.
Did you know that some of the old color CRT television sets used a saturable core,
'transductor' to modulate the scan amplitude to avoid pin-cushion distortion?
You could have been watching one.

There are several references about that on the net too:
http://www.bbcmicro.net/old-8bs/othrdnld/manuals/cubmanual/!cub4.htm#4
 

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