Power factor correction

On a sunny day (Mon, 04 Jan 2010 07:53:30 +0200) it happened Paul Keinanen wrote in :

Yes, the ones I have dealt with also had a huge heavy inductor beteen the rectifiers and the filtercaps. L ========= -------------------------^^^^^^^^^---------------- + | | | | --- --- --- | / \ / \ / \ | --- --- --- | | | | |

--- | | | | | | | ===

--- ) ------| | | | | --- C

--- ) ----- ) ----- | | | | | | --- --- --- | / \ / \ / \ | --- --- --- | | | | | -------------------------------------------------- - The inductor smoothes the main current, and reduces capacitor ripple current. For something like 4kVA and up.

Reply to
Jan Panteltje
Loading thread data ...

n

ams"

looks

hey do,

rectifiers and the filtercaps.

=3D=3D=3D=3D=3D

=A0 =A0 =A0 =A0 =A0 |

=A0 =A0 =A0 =A0 =A0|

=A0 =A0 =A0 =A0 =A0|

=A0 =A0 =A0 =A0 =A0|

=A0 =A0 =A0 =A0 =A0 |

=A0 =A0 =A0 =A0 |

=A0 =A0 =A0 =A0 =A0=3D=3D=3D

=A0 =A0 =A0 =A0 =A0--- C

=A0 |

=A0 =A0 =A0 =A0 =A0 |

=A0 =A0 =A0 =A0 =A0|

=A0 =A0 =A0 =A0 =A0|

=A0 =A0 =A0 =A0 =A0|

=A0 =A0 =A0 =A0 =A0 |

ent.

With the coil, the current is near constant. This makes the harmonic content less but still significant. Adding a moderate sized transformer at each phase and doubling the number of diodes will lower the harmonics quite a bit.

Basically it is 3 of these

------------------ To bridge ( A---------- ( ------------------ To bridge

B----------- ) ) ) C-----------

Since the voltage between B and C is at 90 degrees to the voltage from A to ground, the voltage on the secondary only needs to be the tan() of the angle you are shifting the phase by.

tan(15)=3D0.27

Reply to
MooseFET

On a sunny day (Mon, 4 Jan 2010 06:26:08 -0800 (PST)) it happened MooseFET wrote in :

An interesting solution, never seen that before, maybe I am too old:-)

Reply to
Jan Panteltje

And of course, since you have two phases on two wires (let the other be common), you have a linearly independent basis (not orthonormal, but so what) from which you can span the entire vector space of voltage and phase. So you could, for example, produce a 5-phase system with 10 pulses, or 120 if you wanted. You spend a lot on transformers, though.

What does that do for current, anyway? Current through each phase is essentially a parabolic pulse. All those added up, in the ratios from which they are generated, should distribute to a fairly constant current, shouldn't they? Well, the sum of (three phase) currents is always zero, but the sum of magnitudes isn't: that must oscillate at the 6th harmonic. So it should be that, in the same way as a choke input filter causes relatively more current draw on the flanks of the sine wave than overall, this arrangement also causes more current draw on the flanks, resulting in an inversely phased 6th harmonic. The curious part is, this nonlinear conclusion was based on the linear construction of vectors: of course the diodes, being nonlinear elements, are the reason, but the voltages don't seem like they should do that.

Tim

--
Deep Friar: a very philosophical monk.
Website: http://webpages.charter.net/dawill/tmoranwms
Reply to
Tim Williams

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the=3D

=3D=3D

=A0=3D

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urr=3D

... Or maybe too young. Back when rectifiers couldn't handle the power, you needed more diodes and a way to share the current so doing this didn't add parts.

Reply to
MooseFET

e.

0

which

, but

So it

When the number of poles becomes infinite, the harmonics all drop to zero. Beyond the infinite number, there is no further improvement. I hope this helps.

Reply to
MooseFET

How can there ever not be harmonics, either voltage or current, input or output, when transforming three phase to DC? I think a simple energy budget shows this is necessary.

Ignoring the three phase source, if you start with n equal voltage, equally spaced phases, you will get harmonics of 2n and higher, with a current pulse roughly 1/n of the waveform per phase.

Tim

--
Deep Friar: a very philosophical monk.
Website: http://webpages.charter.net/dawill/tmoranwms
Reply to
Tim Williams

Some issues regarding 3 phase rectifier PFC are discussed in

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It also contains a long list of references, which might be useful when doing Google searches.

Reply to
Paul Keinanen

On a sunny day (Mon, 4 Jan 2010 18:19:15 -0800 (PST)) it happened MooseFET wrote in :

mmm I dunno, designed something for the army that a had selenium rectifier in it..

Reply to
Jan Panteltje

On a sunny day (Tue, 05 Jan 2010 11:22:10 +0200) it happened Paul Keinanen wrote in :

I am impressed, felt back at school for a while. A rather complete design guide!

After reading 240 or so pages...

My head is full :-)

Reply to
Jan Panteltje

udget

ly

lse

I think you missed that the source is 3 phase power and we are constructing more phases with the transformers. If so the rest won't be needed as you will already see it.

Imagine that you have a synchronous motor running on 3 phase. The 3 phase power makes a rotating magnetic field that is of constant strength.

Now imagine that the motor is moving an infinitely fine commutator under some brushes such that the contacts are always at the voltage peaks. This is the infinite number of poles case.

Reply to
MooseFET

Digging deeper into my old archives, the ON Semi PFC Handbook

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might also be useful for single phase applications up to 300 W.

Reply to
Paul Keinanen

I love the smell of burning selenium in the morning.

Reply to
krw

On Sun, 03 Jan 2010 11:51:44 -0800, JosephKK wrote:

Interesting to do if you need to implement synchronous regeneration back into the supply from a big variable frequency drive.

Following on from your posted simulations, I did this, it's a simplified

3 phase, 100 amp PSU circuit from a VFD. Regeneration circuitry omitted. Power factor varies from 0.26 at no load to 0.94 at full load.

Plot definition file and log file included.

File 3phrect.asc

Version 4 SHEET 1 1652 864 WIRE 192 -384 64 -384 WIRE 288 -384 192 -384 WIRE 560 -384 288 -384 WIRE 624 -384 560 -384 WIRE 944 -384 624 -384 WIRE 64 -288 64 -384 WIRE 192 -288 192 -384 WIRE 288 -288 288 -384 WIRE -192 -64 -688 -64 WIRE 288 -64 288 -224 WIRE 288 -64 -112 -64 WIRE -688 -48 -688 -64 WIRE 624 -16 624 -384 WIRE 752 -16 624 -16 WIRE -688 32 -816 32 WIRE 624 32 624 -16 WIRE 752 32 752 -16 WIRE 944 32 944 -384 WIRE -176 112 -688 112 WIRE 192 112 192 -224 WIRE 192 112 -96 112 WIRE -688 144 -688 112 WIRE 624 160 624 96 WIRE 752 160 752 112 WIRE 752 160 624 160 WIRE -816 256 -816 32 WIRE -688 256 -688 224 WIRE -688 256 -816 256 WIRE -192 288 -688 288 WIRE 64 288 64 -224 WIRE 64 288 -112 288 WIRE -688 368 -688 288 WIRE 64 368 64 288 WIRE 192 368 192 112 WIRE 288 368 288 -64 WIRE -816 496 -816 256 WIRE -752 496 -816 496 WIRE -688 496 -688 448 WIRE -688 496 -752 496 WIRE 64 512 64 432 WIRE 192 512 192 432 WIRE 192 512 64 512 WIRE 288 512 288 432 WIRE 288 512 192 512 WIRE 544 512 288 512 WIRE 624 512 624 160 WIRE 624 512 544 512 WIRE 944 512 944 112 WIRE 944 512 624 512 WIRE -752 544 -752 496 FLAG 544 512 VLneg FLAG 560 -384 VLpos FLAG -752 544 0 SYMBOL diode 48 432 M180 WINDOW 0 24 72 Left 0 WINDOW 3 24 0 Left 0 SYMATTR InstName D1 SYMATTR Value FWD SYMBOL diode 176 432 M180 WINDOW 0 24 72 Left 0 WINDOW 3 24 0 Left 0 SYMATTR InstName D2 SYMATTR Value FWD SYMBOL diode 272 432 M180 WINDOW 0 24 72 Left 0 WINDOW 3 24 0 Left 0 SYMATTR InstName D3 SYMATTR Value FWD SYMBOL diode 48 -224 M180 WINDOW 0 24 72 Left 0 WINDOW 3 24 0 Left 0 SYMATTR InstName D4 SYMATTR Value FWD SYMBOL diode 176 -224 M180 WINDOW 0 24 72 Left 0 WINDOW 3 24 0 Left 0 SYMATTR InstName D5 SYMATTR Value FWD SYMBOL diode 272 -224 M180 WINDOW 0 24 72 Left 0 WINDOW 3 24 0 Left 0 SYMATTR InstName D6 SYMATTR Value FWD SYMBOL ind2 -96 304 M270 WINDOW 0 32 56 VTop 0 WINDOW 3 5 56 VBottom 0 SYMATTR InstName L9 SYMATTR Value 220u SYMATTR Type ind SYMBOL ind2 -80 128 M270 WINDOW 0 32 56 VTop 0 WINDOW 3 5 56 VBottom 0 SYMATTR InstName L10 SYMATTR Value 220u SYMATTR Type ind SYMBOL ind2 -96 -48 M270 WINDOW 0 32 56 VTop 0 WINDOW 3 5 56 VBottom 0 SYMATTR InstName L11 SYMATTR Value 220u SYMATTR Type ind SYMBOL cap 608 32 R0 SYMATTR InstName C1 SYMATTR Value 5600u SYMATTR SpiceLine V=400 Rser=.5 SYMBOL current 944 32 R0 WINDOW 123 0 0 Left 0 WINDOW 39 24 116 Left 0 SYMATTR SpiceLine load SYMATTR InstName I1 SYMATTR Value 0 SYMBOL voltage -688 48 R180 WINDOW 123 0 0 Left 0 WINDOW 39 24 -12 Left 0 SYMATTR SpiceLine Rser=.1 SYMATTR InstName V1 SYMATTR Value SINE(0 163.293 60 0 0 0) SYMBOL voltage -688 240 R180 WINDOW 123 0 0 Left 0 WINDOW 39 24 76 Left 0 SYMATTR SpiceLine Rser=.1 SYMATTR InstName V2 SYMATTR Value SINE(0 163.293 60 0 0 120) SYMBOL voltage -688 464 R180 WINDOW 123 0 0 Left 0 WINDOW 39 24 76 Left 0 SYMATTR SpiceLine Rser=.1 SYMATTR InstName V3 SYMATTR Value SINE(0 163.293 60 0 0 240) SYMBOL res 736 16 R0 SYMATTR InstName R1 SYMATTR Value 5.6k TEXT 416 24 Left 0 !.ic v(VLpos) 140\n.ic v(VLneg) -140 \n *precharge TEXT -680 -344 Left 0 !.model FWD D Ron=10m Roff=100e6 Vfwd=0.35 Vrev=600 TEXT -512 536 Left 0 !.tran 0 1 0 TEXT -512 584 Left 0 !.meas tran TP avg(V(n001)*I(V1)) *True power TEXT -512 640 Left 0 !.meas tran VRMS rms(V(n001)) TEXT -512 688 Left 0 !.meas tran IRMS rms(I(V1)) TEXT -512 744 Left 0 !.meas tran AP avg(VRMS*IRMS) *Apparent power TEXT -512 800 Left 0 !.meas tran PF param TP/AP *Power factor TEXT -616 0 Left 0 ;200V between phases TEXT 768 192 Left 0 !.step I1 0 100 10 TEXT -232 -144 Left 0 !k1 L9 L10 L11 0.5 TEXT 696 576 Left 0 !.meas tran VL avg(v(VLpos)-v(VLneg))\n.meas tran Pout param VL*I(I1) TEXT -200 -184 Left 0 ;Line reactor

File 3phrect.plt

[Transient Analysis] { Npanes: 3 Active Pane: 2 { traces: 1 {34603010,0,"I(V1)"} X: (' ',1,0,0.1,1) Y[0]: (' ',0,-120,20,120) Y[1]: ('_',0,1e+308,0,-1e+308) Amps: (' ',0,0,0,-120,20,120) Log: 0 0 0 GridStyle: 1 }, { traces: 1 {524291,0,"V(n001)"} X: (' ',1,0,0.1,1) Y[0]: (' ',0,-180,30,180) Y[1]: ('_',0,1e+308,0,-1e+308) Volts: (' ',0,0,0,-180,30,180) Log: 0 0 0 GridStyle: 1 }, { traces: 1 {524292,0,"V(VLpos,VLneg)"} X: (' ',1,0,0.1,1) Y[0]: (' ',0,225,5,280) Y[1]: ('_',0,1e+308,0,-1e+308) Volts: (' ',0,0,0,225,5,280) Log: 0 0 0 GridStyle: 1 } }

Log file from a run:

Circuit: * H:\Spice\test.asc

.step i1=0 Direct Newton iteration for .op point succeeded. .step i1=10 .step i1=20 .step i1=30 .step i1=40 .step i1=50 .step i1=60 .step i1=70 .step i1=80 .step i1=90 .step i1=100

Measurement: tp step AVG(v(n001)*i(v1)) FROM TO 1 4.92903 0 1 2 870.501 0 1 3 1719.76 0 1 4 2568.47 0 1 5 3406.9 0 1 6 4215.87 0 1 7 5002.64 0 1 8 5809.35 0 1 9 6569.61 0 1 10 7357.99 0 1 11 8134.66 0 1

Measurement: vrms step RMS(v(n001)) FROM TO 1 114.699 0 1 2 114.415 0 1 3 113.542 0 1 4 112.69 0 1 5 111.896 0 1 6 111.095 0 1 7 110.262 0 1 8 109.522 0 1 9 108.701 0 1 10 107.999 0 1 11 107.301 0 1

Measurement: irms step RMS(i(v1)) FROM TO 1 0.165922 0 1 2 10.1219 0 1 3 18.3089 0 1 4 25.879 0 1 5 33.501 0 1 6 41.1342 0 1 7 48.7225 0 1 8 56.68 0 1 9 64.3137 0 1 10 72.3274 0 1 11 80.387 0 1

Measurement: ap step AVG(vrms*irms) FROM TO 1 19.0311 0 1 2 1158.09 0 1 3 2078.83 0 1 4 2916.3 0 1 5 3748.64 0 1 6 4569.8 0 1 7 5372.22 0 1 8 6207.71 0 1 9 6990.94 0 1 10 7811.25 0 1 11 8625.57 0 1

Measurement: pf step tp/ap 1 0.258999 2 0.751669 3 0.827272 4 0.880729 5 0.908837 6 0.92255 7 0.931206 8 0.935827 9 0.939733 10 0.941973 11 0.943087

Measurement: vl step AVG(v(vlpos)-v(vlneg)) FROM TO 1 280.846 0 1 2 269.649 0 1 3 264.674 0 1 4 261.622 0 1 5 259.052 0 1 6 256.417 0 1 7 253.744 0 1 8 251.29 0 1 9 248.669 0 1 10 246.405 0 1 11 244.15 0 1

Measurement: pout step vl*i(i1) 1 0 2 2696.49 3 5293.48 4 7848.67 5 10362.1 6 12820.9 7 15224.6 8 17590.3 9 19893.5 10 22176.5 11 24415

Date: Sat Jan 16 05:28:55 2010 Total elapsed time: 21.350 seconds.

tnom = 27 temp = 27 method = modified trap totiter = 34546 traniter = 34542 tranpoints = 15714 accept = 10511 rejected = 5203 matrix size = 11 fillins = 12 solver = Normal Matrix Compiler1: off Matrix Compiler2: off

--
"Electricity is of two kinds, positive and negative. The difference
is, I presume, that one comes a little more expensive, but is more
durable; the other is a cheaper thing, but the moths get into it."
                                             (Stephen Leacock)
Reply to
Fred Abse

Vrev=3D600

Pout param VL*I(I1)

Thanks Fred. I am learning some stuff about spice from this. It seems the power factor is not so bad as the harmonics.

Reply to
JosephKK

The way true and apparent power were calculated should include the effect of harmonics.

--
"Electricity is of two kinds, positive and negative. The difference
is, I presume, that one comes a little more expensive, but is more
durable; the other is a cheaper thing, but the moths get into it."
                                             (Stephen Leacock)
Reply to
Fred Abse

the

effect

While is most certainly does include the power in the harmonics, it does = not=20 calculate the spectral power of each of the various harmonics. I am=20 interested in the harmonic power by harmonic number.

Reply to
JosephKK

ms the

t

not

It is often better to start off with knowing the real power. Stripping that out of the waveform makes the wave form you need to process much easier to deal with. Only if the FFT in spice works on exactly an integer number of cycles does it make the FFT into a single spike. The tail of the skirt on the fundamental shifts the other harmonics up.

Reply to
MooseFET

Whilst you are investigating that, it would be interesting to evaluate the effect of different line reactors on harmonic currents in the supply.

--
"Electricity is of two kinds, positive and negative. The difference
is, I presume, that one comes a little more expensive, but is more
durable; the other is a cheaper thing, but the moths get into it."
                                             (Stephen Leacock)
Reply to
Fred Abse

seems the

effect

does not

I studied the impacts of various windowing schemes some 25 years ago.

Reply to
JosephKK

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