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Wednesday, January 8, 2020

Measuring the voltage and current of a microwave oven magnetron--- make money online

Measuring the voltage and current of a microwave oven magnetron--- make money online
I took apart my microwave oven and measured the voltage and current supplied to the magnetron. The device appears to start conducting current at 4KV, and will allow lots of current to flow once this threshold voltage is reached.


My current probe is pretty cheapo, so I wouldn't trust its measurement too much, but the final determination of 1300 W average seems pretty spot-on.
hey everyone I'm out in the shop and I
wanted to play with magnetrons so I took
my microwave apart and here's the
magnetron here this is the device that
actually creates the microwaves that
cook food and what I want to do is
characterize the voltage and current
requirements of the magnetron so I've
got some projects in mind that will come
up later but right now I'm just
measuring one of these to see what it's
how it works so a magnetron is a vacuum
tube with a filament and an anode and it
works by swirling around electrons
there's two large magnets if you've ever
taken one of these apart you'll see
there's two doughnut shaped magnets in
there and the magnetic field causes the
electrons to swirl around in a spiral
and the speed at which they're swirling
around past the number of cavities in
there determines the frequency of the
microwaves generated so pretty much all
modern ovens operate at 2.45 gigahertz
and the frequency is determined by the
number of cavities that you've got and
the magnetic field strength so here's a
terrible little schematic diagram in the
center there's a coiled filament and the
filaments are quite heavy duty in these
tubes because they're transmitting so
much power so the filament is heated up
by about maybe 4 volts AC it may be 5 to
10 amps and so it's a really powerful
film and maybe it's only 5 amps but it's
a lot for a filament it's dumping out
quite a lot of power and the electrons
are emitted from the hot filament and
they're attracted towards this outer
ring of cavities but as the electrons
make their way from the filament towards
the anode they actually start spiraling
around because this entire cavity is in
a magnetic field so as the electrons are
emitted from the centre and spiral
around they move past these cavities and
the speed at which they move past the
cavities is determined by the magnetic
field strength
so if you if you take a little tap off
one of these cavities you can draw off
some RF energy so basically just it's
sort of like blowing wind past a you
know like a reed or something or blowing
wind past an open pipe you get some
resonance going on in here and you can
take off some of the energy so this I
mean these things are you know a dime it
doesn't even get a microwave oven for
well under a hundred dollars now and
this you can you know it's over a
kilowatt of transmit power so these
these devices are actually very simple
in operation schematically they look
like this here's your two filament leads
coming in and that's the anode and this
is this little it's it's almost a
symbolic representation of this little
take off line so that's actually how you
get the RF energy out of the microwave
the circuit is almost ridiculously
simple pretty much all microwaves that
I've seen are set up just like this so
when the microwave you know decides that
it should be running you've passed all
the interlocks and the the cook timer is
running it puts power onto this
transformer 115 volts line voltage onto
this transformer and one secondary on
the transformer is high-voltage probably
about 2,000 volts maybe 2,500 open
circuit or something like that and it's
set up with this simple voltage divider
so during half the cycle this capacitor
gets charged up and during the other
half of the cycle this capacitor is put
in series with a negative voltage on
this line here so when when this line is
positive and this is negative the
capacitor is charged through the diode
then when the when the phase changes to
negative here then this capacitor is in
series with the negative voltage on this
transformer and it pumps negative
voltage into the magnetron tube while
this is all going on the film has just
kept hot all the time so the filament
has its own little winding on the
transformer
and it's it's three or four volts AC you
know five or ten amps or something like
that so what this means is that the
magnetron is actually not transmitting
half the time so if you have sixty Hertz
power during the negative half of the
cycle this isn't doing anything at all
it's just charging up this capacitor and
during the other half then the magnetron
is actually transmitting so you'll see a
little later in the video where I sort
of surprised myself I didn't even
realize this myself until I did some
more careful measurements so anyway so
I'm really interested in doing is
finding out what this graph looks like
for a magnetron if it's current versus
voltage if you put a little bit of and
let's assume the filament is already hot
and up to temperature you can put a
little bit of voltage on it
a little more a little more eventually
you know no current really flows until
you get up to about four kilovolts and
then suddenly you get tremendous current
gain and as far as I know this line just
continues essentially straight up so you
can never have a voltage drop greater
than maybe four kilovolts for this type
of magnetron you can just keep dumping
more and more current through them so
for my application I want a really high
pulse of power so what I'm going to do
is charge up a capacitor bank and dump
the capacitor bank through the magnetron
and as soon as the the applied voltage
goes over four kV you should get a
transmitted pulse and you can get much
much higher peak powers then you could
just by supplying it with a transformer
like this
okay here's my next setup so I took the
filament wire off the capacitor terminal
and soldered it in line to the high
voltage wire going to the magnetron so
this way I could keep the filament
currents out of my way I can measure
just the magnetron current going in
emission current so I've got the high
voltage probe hooked up to the line and
I've also got the current probe clamped
on to the wine should be sensing just
the emission current so let me point
this at the scope and you can see what
the start-up behavior is like okay I put
this on auto and I'll start the
microwave now
so you can hear it takes a few seconds
for to stabilize and after it comes up
to power it sort of the curve is quite
repeatable so you can sort of trust
what's going on here so I'm just going
to press single and grab a single
acquisition and we've got the same
really unusually square looking square
wave zero volts negative for kilovolts
and on the current side I switched this
to a hundred millivolts per division and
the zero is here so in the positive or
in the zero part of the waveform there's
zero current as we'd expect and in the
negative part of the waveform it kind of
gets down to about an amp and then
trails back off and it spends most of
its time at about negative one amps one
amp which is still way too much that
would mean this this thing is drawing
three kilowatts input which is far more
than it and it is probably three times
less than that so I'm still trying to
figure out how to get a resistor into
the high side the problem is that you
know I even I even put a 1 ohm resistor
there that you can see I really don't
want to float this I mean even if I had
an isolation transformer big enough to
handle the microwave floating this thing
would mean that the entire case would be
four thousand volts different from the
from ground from real earth ground so
I'd have to connect that to my scope
I could also float the scope but then
that means that the scope case would be
three or four thousand volts above
ground which were below ground whatever
it is it's going to be bad so I'd rather
not do that either so now that I look at
it this is actually probably correct
I changed the scale on the current probe
so that now we've got one volt per amp
or one division per amp on the current
trace which is one the voltage trace is
still two and it's two kilovolts per
division and a is the product of the two
so a is power
and I used the scopes measurement
feature to get the mean value for power
across one full cycle so it's gated on
these two bars here and lo and behold
1.33 kilowatts so that's actually about
right microwave ovens are you know 1200
kilowatts in and the magnetron is
probably outputting 7 to 800 watts of
microwave power but yeah 1200 1300 watts
in that's that's pretty reasonable so
what's interesting is that the current
traced lags behind the voltage trace by
quite a bit almost a full division here
and we're at 2 milliseconds per division
so I'm not sure that this actually might
be an artifact of the current
measurement probe there's probably some
low-pass circuitry in the probe that's
just causing some delay there I find it
hard to believe that the voltage jumps
right up to 4 kilovolts and then there's
2 milliseconds later the current starts
rising I don't believe that so there's
probably some inaccuracy in here but I'm
still surprised that the number there is
as close as it is to reality so what I
forgot to mention was that in this part
of the cycle when the magnetron is
actually firing sure maybe it averages
you know 3 3 kilowatts but when you
average across the whole cycle or down
to below one-and-a-half kilowatts which
which makes sense so in the when the
microwave is running half of the cycle
is used just to charge the capacitor and
then the other half of the cycle is when
the thing fires and it's drawing power
plus using the power that was stored in
the capacitor so really you could say
that your microwave oven is a four
kilowatt or three kilowatt device it's
just only running half the time
basically okay I hope that was helpful I
will keep you posted on my high-power

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