Is it not amazing that the hillbillies from backwoods Missouri with a 
3rd grade education can make a rotary phase converter without all the 
math...

Interesting discussion.

John

Kirk Wallace wrote:
> On Mon, 2011-03-14 at 00:04 -0400, Przemek Klosowski wrote:
>    
>> On Wed, Mar 9, 2011 at 12:35 AM, Kirk Wallace
>> <kwall...@wallacecompany.com>wrote:
>>
>>      
>>> Let me try to provide more details on my understanding of the phase
>>> timing of DIY converters. Attached is a schematic of a common rotary
>>> converter. The source is here:
>>> http://www.metalwebnews.com/howto/ph-conv/ph-conv.html
>>> http://www.metalwebnews.com/howto/ph-conv/fig1.html
>>>
>>> I used this to make my converter and is the only design I have some
>>> understanding of. As the schematic shows L1 and L2 go straight to the
>>> output and are unaffected. Since L1 and L2 are single phase, L1 is a
>>> mirror of L2, therefore 180 degrees out of 360 apart.
>>>
>>>
>>>        
>> But, but, you are committing a tautology. If you reference L1 to L2 and vice
>> versa, of course L1 is a mirror of L2. In your scheme there is no 'ground'
>> or reference point, so you only have one phase coming in,
>>      
> I agree if you combine any two sine waves of the same period, the result
> is a single wave of the same period. I think what does change is the the
> amplitude of the resulting wave as one changes the phase between the two
> original waves. But I'll also agree that the ground or neutral is a red
> herring because it isn't connected to any part of the motor circuit
> (other than 120 VAC for a relay).
>
> So what we have at this point is a 240 Volt sine wave across the idler
> motor connection at L1 and L2. If nothing else is connected, voltage and
> current is alternating between L1 and L2. L3 looks like a center tap, so
> V-L1L3 should be 120 Volts and 0 degrees in reference to V-L1L2, and
> V-L2L3 is 120 Volts and 180 degrees in reference to V-L1L2, just as a
> neutral would be. If the rotor had no mass, my guess is that it would
> vibrate between 0 and 120 degrees. When the idler L1 and L2 is first
> connected to the mains, a start capacitor is switched on between L1 and
> L3, which for an instant, will look like a temporary short circuit of L1
> and L3, as it charges, the field will rotate giving the rotor a kick in
> one direction (?). The rotor mass should carry the rotor through
> subsequent cycles and the start capacitor is disconnected. So now we
> have the idler motor with 240 VAC across L1 and L2 with the rotor
> spinning and nothing connected to L3. Now I'm thinking, what's going on
> at L3? What comes to mind is that any motor is just as much a generator
> as a motor, so there must be a very significant three phase signal
> coming off of L1, L2 and L3 and because of the physical layout of the
> stator windings, each generated leg is 120 degrees apart. Now I'm
> beginning to think of the idler as a three phase generator that is being
> back driven on one phase (L1L2), or as a motor that has two dead phases.
> The only difference between a 240 Volt three phase motor and a 240 Volt
> three phase generator is the current direction, so the idler has motor
> like currents for 120 shaft degrees and generator currents for 240. Also
> the rotor is decelerating or converting inertia into electrical energy
> for 240 degrees and storing inertial energy for 120. I suppose the
> capacitors between L1 and L3, and L2 and L3 are another means to store
> energy to help the rotor get through the generator phase. Uugg, my brain
> hurts but I think I'm getting a better understanding. I haven't even
> begun to think about the math that follows. But, getting the correct
> starting point helps the thought process. Thanks
>
>    
>>   and the motor
>> generates the second (and third) phase L3, shifted with respect to L1/L2.
>> One way to see it comes from the trigonometric identity  holding that sum of
>> three sines shifted by 0, 120 and 240 degrees is zero:
>> sin(x)+sin(x+2*%pi/3)+sin(x+4*%pi/3)=0
>>
>> Let's say we take some arbitrary reference point, so that L1(t) is the
>> voltage on the first leg. Assume L2(t)-L1(t) = V sin(2 pi f t). If the
>> converter generates L3(t)=L1(t)-V sin(2 pi f t + 2/3 pi), then L1-L3 is V
>> sin(2 pi f t + 2/3 pi), i.e. shifted by 120 degrees, and L3-L2 is -V sin(2
>> pi f t + 2/3pi) - V sin(2 pi f t)  which reduces to V sin(x+4*%pi/3) i.e.
>> the same AC shifted 240 degrees. Note that it doesn't matter what the
>> reference point is, because its potential L1(t) drops out --- all that
>> matters are voltage differences between the legs of the circuit, not the
>> potentials of the legs themselves.
>>      
>
>
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