If there is unnecessarily large inrush current that is due to core
saturation late in the first half-cycle, then adding a resistive load on
the secondary won't fix that.
> and look at the current waveforms. When you run out of
>> working triacs you could also google it.
>>
>> The key to understanding this is to realise that the magnetic flux is
>> proportional to the time-integral of the applied voltage, and that in
>> continuous operation the flux is normally close to zero when the voltage
>> is close to maximum, and the flux is close to maximum when the voltage
>> is close to zero. Have a look at the first link here:
>
> Are we talking about inductors or transformers with load resistors
> that cause a steady state primary current 2X their design rating?
It doesn't much matter whether we are talking about transformers or
ungapped inductors, in that the transformer with its secondary
unconnected can still draw a lot of inrush current, and adding a load on
the secondary won't fix that.
Yes I don't know why they put the scope plot backwards. It adds
unnecessary confusion, though at least they do mention it in the text. I
can only assume they lacked the ability to flip it easily in their
chosen method of document preparation.
> I don't have any argument with that. You can certainly manage
> the drive so the core saturates.
>
> My attempts were to arrange the drive signal to MITIGATE inrush
> current.
I know, and I was just suggesting that turning on when the mains voltage
goes through zero is not the best way to do that. Turning on at the
zero-crossing of the mains voltage is good if your load is capacitive,
e.g. the input of a SMPS.
>
> The key point is in the wikipedia link:
> "Worst case inrush happens when the primary winding is connected at an
> instant around the zero-crossing of the primary voltage, (which for a
> pure inductance would be the current maximum in the AC cycle) and if the
> polarity of the voltage half cycle has the same polarity as the remnance
> in the iron core has. (The magnetic remanence was left high from a
> preceding half cycle)."
> end quote
>
> If you always turn off the current at the current zero crossing with
> a positive voltage slope, then always turn on the next weld pulse
> at zero voltage on the positive voltage slope, doesn't that leave
> you in a remanence position to avoid saturation at the next turn on?
> If not, why not?
I think the remanence is clouding the issue. It is a relevant effect but
even without it, there are good and bad times to switch on the
transformer primary, and it would be better to consider remanence only
after the basic situation with a soft-magnetic core is thoroughly
understood. You might be able to use the remaining flux in the
switched-off transformer to choose the least worst of the two zero
crossings to switch it on at, but even then, I think you would do better
to switch on at a different time. Why not seriously try it out with a
current transducer and DSO, (and a vastly over-sized triac or even
better a pair of big SCRs, just in case!). It would be nice to see the
plots, and it is one way to end an argument.
>
> The SSR is gonna turn off near zero current. About all I can control
> is the slope of the voltage sinewave when I give the command.
> To turn it on it's far easier to sense the zero crossing of the line
> voltage than the peak.
The mains frequency (or period) is accurate and stable enough, and
microcontrollers or even 555 timers are cheap enough that as Phil
mentioned, you can figure out the time of the voltage peak from the zero
crossing.
> Isn't a major portion of the primary current
> in phase with the primary voltage due to the resistive secondary load?
> Isn't it the leakage inductance that causes the phase shift?
That sounds reasonable, but if the core saturates then that's the least
of your worries. The primary current is not necessarily a good way to
determine the core flux density, as you can make the primary current be
whatever you want by choosing the secondary current.
>
> Under the control conditions described above where we control both
> ends of the waveform to manage remanence and have a very low value
> resistive load, how much would I gain by waiting for the peak line
> voltage at turn on?
Time for an experiment. It depends a lot on the transformer design. I
have read that toroidal transformers produce more problematic saturation
effects than E-I types, and if the core was nominally run at less than
half of its saturation flux density then there will be no problem. Due
to the more uniform geometry I think they can run toroidal transformers
close to saturation in normal operation.
>
> I'd go look, but it's stored behind a bunch of junk in the garage.
>
> As I recall, I didn't make many measurements without load. But
> with the secondary (almost) shorted in the weld mode, I don't
> remember any horrible input current transients.
I wonder whether they even bother to switch the transformer on at the
right time in a microwave oven. The current that your transformer draws
in steady state might be so high (due to the secondary current) that
saturation doesn't make it all that much worse, but given the choice (or
given a bigger transformer than your circuit breaker likes), you might
as well make it optimum if that is just a matter of inserting a small delay.
I have an arc welder that sometimes trips the breaker if I turn it on at
the wrong time (with a mechanical switch), and it would be nice if it
didn't.
> I do know that synchronization with the line made a major improvement
> in the repeatability of the welds.
>
>
> I'm up for some education.
>
> My thinking was that, if not for saturation, the SCR would be less
> stressed if I turned it on at zero voltage when the primary current was
> zero. And from the unpowered state, the voltage and current can't
> be anything but zero.
The risk of saturation occurs well after the zero crossing when the
voltage is turned on. If the load is not capacitive (not a big SMPS)
then the SCR won't mind if you turn it on when there is voltage across
it, and later on in the cycle it will be much happier.
> And that, if I could arrange the resting place on the B-H curve
> from the previous pulse such that the first half-cycle wouldn't
> saturate the core, that's the best I could do easily.
> Measurements didn't show any horrible first cycle inrush.
> Welds got more repeatable.
>
> Let me say the same thing in different words.
> If the load is linear resistive, the transformer current and voltage
> will be approximately in phase. If the SCR shuts off at zero
> current, the voltage will also be near zero volts (plus whatever the
> leakage inductance allows).
And the magnetizing current too.
> Case 1, you start the next pulse in a nanosecond.
This is not the same thing as I was discussing. If the transformer is in
steady-state operation and if you were able to turn off the primary at a
zero-crossing of the mains voltage, that is a time when there is maximum
flux in the core. If you instantly switch it back on again, sure this
will be pretty much a continuation of steady-state operation.
If instead you turn it off for an integer number of mains cycles that
adds up to a few seconds, the core flux will not be the same when you go
to switch it back on again.
> Isn't the initial current still pretty near zero?
Perhaps but that doesn't really matter as regards the risk of saturation.
> Isn't the point on the B-H curve still about the same?
Yes, if you only switch it off for nanoseconds. No, if you wait a few
seconds until you have repositioned your parts for the next weld.
> Case 2, you start the next pulse next week at the zero crossing
> of the input voltage headed in the same direction.
> What's the initial current?
> What's the initial point on the B-H curve?
> How is restarting it synchronously significantly different from
> just leaving it running?
The flux in the core is different.
Put a big inductor (maybe a car ignition coil) across a 12Vrms AC supply
and make sure you are holding the terminals a nanosecond after you
disconnect the supply, at the instant when the AC supply is at zero
voltage (and the inductor is carrying maximum current).
Then give it to me and I will hold the terminals a week later.
I think you will notice the difference. The state of the flux in the
core matters.
Note that in the case of a transformer, it is possible that some value
of secondary current could result in the primary current being zero (or
any other chosen value) at the zero-crossing of the mains voltage. That
is not relevant to my point, which relates to the flux density in the
core, which won't be affected much by the secondary current if a
low-impedance supply is driving the primary winding.
>
> I'm not disputing the articles you posted.
> I'm not saying anything about the general (worst) case.
> I'm suggesting that this is how you engineer a spot welder using a MOT.
>
> Where did my thinking go wrong?
>
It may just mean that you need a larger rating for your fuse or circuit
breaker and more expensive triac or SCRs than you could otherwise get
away with.
When I tried spot welding, I was never able to get enough current from a
MOT-sized transformer with a few turns on the secondary. I could sort of
weld things if I applied very light pressure so that the workpieces made
poor contact with each other and the resistance was high enough for the
(insufficient) current to heat them, but this wasn't really satisfactory
because getting the force and contact resistance just right was not
reliable.
If I made a transformer big enough to weld thick workpieces with proper
contact pressure, it might cause excessive drop in my mains supply,
and/or trip breakers.
I think the best option for me is a series-parallel array of Maxwell
boostcaps. This would eliminate the requirement for a large mains supply
capability. The 3000F ones are rated for 1900 Amps each, so about 5 in
parallel would probably supply about enough current for any normal sheet
metalwork up to a couple of millimetres thick which seems to require
close to 10kA capability. (Aluminium welding requires several times more
current so I won't try that.) Most of the references that I have seen
tend to suggest that the weld itself requires somewhere in the region of
1.5 Volts, but the electrodes etc. will have some resistive drop so I
think at least 2 banks of boostcaps in series will be desirable. Due to
the capacitors holding more energy than the total that you would want
for one weld, it would be necessary to find a way to switch them off,
and it would also be very useful to be able to adjust the current by PWM
during the weld. Therefore a lot of MOSFETs would be required. It seems
that the best current rating per dollar occurs for individual MOSFETs
rated at about 100A, so about 100 of these in parallel would be required
for 10kA. I think a totem-pole style half-bridge topology might work,
using the output cables as an inductor to smooth the output current. A
multi-phase PWM arrangement with multiple output inductors could make
better use of the current rating of the caps. It would be an interesting
project but I don't have time to do it yet. I am somewhat concerned
about what would happen in the event of one failed MOSFET, and I would
like to think of a way to mitigate that. Perhaps the bondwire or package
pin would be an adequate fuse.
Chris