CCM boost inductor design

bitrex wrote...
If you use toroids there's no law that you can't
glomp two toroids together, like stacking donuts,
to get more effective core volume and winding
surface area, it's done all the time

Yes, it's an excellent approach.


--
Thanks,
- Win
 
Single inductor progressive wound for 500W PFC is standard
 
On 7/28/19 7:41 PM, Klaus Kragelund wrote:
Single inductor progressive wound for 500W PFC is standard

Oh, I read down looks like OP wants his design to not use electrolytic
capacitors. That clears things up a bit. and also, damn son.
 
On 7/28/19 7:41 PM, Klaus Kragelund wrote:
Single inductor progressive wound for 500W PFC is standard

Right, I've seen single coils used in PC power supplies, at least, up to
750 watts I think so it's a bit puzzling as to why need to do something
much different, unless there are very rigid full-load efficiency
requirements we don't know about. what does "low loss" mean. 80-85%
efficiency is probably standard for a good-quality 500 watt PC PSU.
 
bitrex wrote...
Oh, I read down looks like OP wants his design to not
use electrolytic capacitors. That clears things up ...

He found an awesome Vishay 50uF 900V film cap.
500W at 600V is 0.83A, drawing the 50uF down
by 0.1 volt in 6us. And with its 4-m-ohm esr,
the switched-current ripple is only 33mV, who
needs an electrolytic?


a bit. and also, damn son.


--
Thanks,
- Win
 
On Sunday, July 28, 2019 at 7:00:41 AM UTC-7, Piotr Wyderski wrote:
Hi,

I would like to make a low-loss boost PFC converter for the following
parameters: 150kHz switching frequency, 180-250VAC input, 600V output
at 500W. It should operate in CCM with 20% deltaIL, so the inductor
will be pretty large: 1.2mH at 4.6A_peak. Basically, I am considering
two options of winding it: a gapped low-loss ferrite core (3C95 or
similar material) or an alloy powder E core EMS-0432115-060. The latter
is currently my preferred choice due to its great wide-swing saturation
characteristics (~1.8uH@0A and still a nice value of 600uH at a 10A
surge). Unfortunately, it will require 108 turns, so for a bobbin
27mm wide and relatively thin 1mm diameter wire means 4 layers of
windings. I am afraid this can introduce some nasty resonances and
make the AC resistance worse due to the proximity effect.

OTOH, this is a 20% CCM inductor, so the AC component is only about
800mA in the worst case. So, should I consider winding it with litz
wire (7x0.4mm is probably the thickest braid I can fit there) or
ignore the AC component entirely and go to the lowest DCR achievable,
i.e. a 1.2mm solid wire?

I don't think I can obtain a square 1x1mm magnet wire, the
closest purchasable size is 2x1mm, which for sure will not fit.

The alternative is a planar E58 core wound with 4 layers of 2.5mmx1mm
rectangular wire (54 turns in total). But the inductor would be about
2x the size of the powder core one and have a dangerously sharp
saturation curve.

The boost will be based on a SiC device, but I don't want to go into
the MHz switching range in order to have a physically smaller inductor
-- the parameter I optimize is raw efficiency, not power density.
So I see no point in transforming winding losses into switching and core
losses. Any thoughts, please?

Best regards, Piotr
 
On Sunday, July 28, 2019 at 7:00:41 AM UTC-7, Piotr Wyderski wrote:
Hi,

I would like to make a low-loss boost PFC converter for the following
parameters: 150kHz switching frequency, 180-250VAC input, 600V output
at 500W. It should operate in CCM with 20% deltaIL, so the inductor
will be pretty large: 1.2mH at 4.6A_peak. Basically, I am considering
two options of winding it: a gapped low-loss ferrite core (3C95 or
similar material) or an alloy powder E core EMS-0432115-060. The latter
is currently my preferred choice due to its great wide-swing saturation
characteristics (~1.8uH@0A and still a nice value of 600uH at a 10A
surge). Unfortunately, it will require 108 turns, so for a bobbin
27mm wide and relatively thin 1mm diameter wire means 4 layers of
windings. I am afraid this can introduce some nasty resonances and
make the AC resistance worse due to the proximity effect.

OTOH, this is a 20% CCM inductor, so the AC component is only about
800mA in the worst case. So, should I consider winding it with litz
wire (7x0.4mm is probably the thickest braid I can fit there) or
ignore the AC component entirely and go to the lowest DCR achievable,
i.e. a 1.2mm solid wire?

I don't think I can obtain a square 1x1mm magnet wire, the
closest purchasable size is 2x1mm, which for sure will not fit.

The alternative is a planar E58 core wound with 4 layers of 2.5mmx1mm
rectangular wire (54 turns in total). But the inductor would be about
2x the size of the powder core one and have a dangerously sharp
saturation curve.

The boost will be based on a SiC device, but I don't want to go into
the MHz switching range in order to have a physically smaller inductor
-- the parameter I optimize is raw efficiency, not power density.
So I see no point in transforming winding losses into switching and core
losses. Any thoughts, please?

Best regards, Piotr

Hi Piotr, Normally CCM

On Sunday, July 28, 2019 at 7:00:41 AM UTC-7, Piotr Wyderski wrote:
Hi,

I would like to make a low-loss boost PFC converter for the following
parameters: 150kHz switching frequency, 180-250VAC input, 600V output
at 500W. It should operate in CCM with 20% deltaIL, so the inductor
will be pretty large: 1.2mH at 4.6A_peak. Basically, I am considering
two options of winding it: a gapped low-loss ferrite core (3C95 or
similar material) or an alloy powder E core EMS-0432115-060. The latter
is currently my preferred choice due to its great wide-swing saturation
characteristics (~1.8uH@0A and still a nice value of 600uH at a 10A
surge). Unfortunately, it will require 108 turns, so for a bobbin
27mm wide and relatively thin 1mm diameter wire means 4 layers of
windings. I am afraid this can introduce some nasty resonances and
make the AC resistance worse due to the proximity effect.

OTOH, this is a 20% CCM inductor, so the AC component is only about
800mA in the worst case. So, should I consider winding it with litz
wire (7x0.4mm is probably the thickest braid I can fit there) or
ignore the AC component entirely and go to the lowest DCR achievable,
i.e. a 1.2mm solid wire?

I don't think I can obtain a square 1x1mm magnet wire, the
closest purchasable size is 2x1mm, which for sure will not fit.

The alternative is a planar E58 core wound with 4 layers of 2.5mmx1mm
rectangular wire (54 turns in total). But the inductor would be about
2x the size of the powder core one and have a dangerously sharp
saturation curve.

The boost will be based on a SiC device, but I don't want to go into
the MHz switching range in order to have a physically smaller inductor
-- the parameter I optimize is raw efficiency, not power density.
So I see no point in transforming winding losses into switching and core
losses. Any thoughts, please?

Best regards, Piotr
 
On Sunday, July 28, 2019 at 8:39:42 AM UTC-7, Piotr Wyderski wrote:
bitrex wrote:

Is 1.2 mH the no load or full-load inductance? That sounds like a
mammoth inductor for that spec, even if that's the no-load inductance.

It's at full load. Math is right and you are right as well. CCM boost
inductors just *are* huge. Usually much bigger that the downstream
converters they supply.

Best regards, Piotr

Math is oK when used with SPICE and Breadboarding. If you need high efficiency, then you need many loops of the three magic steps. (MSB) This will reduce the L to about 300uF. At 150KHz your Kool-Mu will be hot-Mu and MPP will be better but any good Ferrite (3F3) tops all. As the power goes up and F goes down, you can drop back to Kool-Mu, (2 stacked donuts.) is a good choice, and save money. 150KHz may be difficult for MOSFETs and magnetics. SiC MOSFETs may be needed but the diode must always be SiC.
The inductor construction is tricky, gap the center post and outside walls equally. Do not go to three layers!
JL, there are some operating points that Kool-Mu cannot touch MPP.
Cheers, Harry D.
 
On 28 Jul 2019 18:18:29 -0700, Winfield Hill <winfieldhill@yahoo.com>
wrote:

bitrex wrote...

Oh, I read down looks like OP wants his design to not
use electrolytic capacitors. That clears things up ...

He found an awesome Vishay 50uF 900V film cap.
500W at 600V is 0.83A, drawing the 50uF down
by 0.1 volt in 6us. And with its 4-m-ohm esr,
the switched-current ripple is only 33mV, who
needs an electrolytic?

Doesn't a PFC booster need milliseconds of holdup, as the AC line
crosses zero?

If it's driving a downstream forward converter or something, a lot of
ripple might be tolerable. But not too much.


--

John Larkin Highland Technology, Inc

lunatic fringe electronics
 
On Sun, 28 Jul 2019 18:09:56 -0700 (PDT), Harry D <td2k99@gmail.com>
wrote:

On Sunday, July 28, 2019 at 8:39:42 AM UTC-7, Piotr Wyderski wrote:
bitrex wrote:

Is 1.2 mH the no load or full-load inductance? That sounds like a
mammoth inductor for that spec, even if that's the no-load inductance.

It's at full load. Math is right and you are right as well. CCM boost
inductors just *are* huge. Usually much bigger that the downstream
converters they supply.

Best regards, Piotr

Math is oK when used with SPICE and Breadboarding. If you need high efficiency, then you need many loops of the three magic steps. (MSB) This will reduce the L to about 300uF. At 150KHz your Kool-Mu will be hot-Mu and MPP will be better but any good Ferrite (3F3) tops all. As the power goes up and F goes down, you can drop back to Kool-Mu, (2 stacked donuts.) is a good choice, and save money. 150KHz may be difficult for MOSFETs and magnetics. SiC MOSFETs may be needed but the diode must always be SiC.
The inductor construction is tricky, gap the center post and outside walls equally. Do not go to three layers!
JL, there are some operating points that Kool-Mu cannot touch MPP.
Cheers, Harry D.

Sure, but mpp is expensive.


--

John Larkin Highland Technology, Inc

lunatic fringe electronics
 
John Larkin wrote:

Doesn't a PFC booster need milliseconds of holdup, as the AC line
crosses zero?

Holdup is for the situation when the AC stays zero for a predefined
time. Typically one line cycle in the case of servers, to allow them to
save critical data (which doesn't happen, anyway...). In this case this
application t_holdup=0, as there will be a battery switchover. The
capacitor is only to provide a reasonable ripple value. I have assumed
deltaV of 60V, which is just 10% of the 600V V_BUS. The downstream LLC
will have no problems with that.

Best regards, Piotr
 
bitrex wrote:

Right, I've seen single coils used in PC power supplies, at least, up to
750 watts I think so it's a bit puzzling as to why need to do something
much different

Just the losses. It is easy to wind the inductor if you don't care much
about them.

unless there are very rigid full-load efficiency
requirements we don't know about.

There are, and this could be inferred from the thermal requirements.
And you are right, the peak efficiency is expected at the full load
and high line, not in the usual middle of the curve. For exactly the
same reason.

what does "low loss" mean. 80-85%
efficiency is probably standard for a good-quality 500 watt PC PSU.

The goal here is 95% end-to-end, including the LLC stage. This makes
things quite interesting. :)

Best regards, Piotr
 
Winfield Hill wrote:

> That's a very nice choice, I like it. Thanks!

Hearing this from you is a huge reward.

In fact, the entire converter is designed around this cap.
The "I am what I am, find a way of using me" LLC transformer
is another such a place. The bottom-up approach sometimes pays off.

Best regards, Piotr
 
Harry D wrote:

> Hi Piotr, Normally CCM

Right, but the low-load region is not a big concern in this application.
I can live happily with DCM or frequency-clamped BCM there. Or switch
the main converter altogether, as I have a 50W auxiliary PSU there.

Best regards, Piotr
 
Harry D wrote:

> Math is oK when used with SPICE and Breadboarding. If you need high efficiency, then you need many loops of the three magic steps. (MSB) This will reduce the L to about 300uF. At 150KHz your Kool-Mu will be hot-Mu

This is for CCM with deltaB=30mT or so. The manufacturer's design tool
as well as the Steinmetz coefficients for the material bolted into a
Matlab script consistently report core losses of about 1W. Winding
losses are higher, but even that bumps the temperature up by at most
35 degrees for the worst design option. It is estimated to be 25.6 deg
in the case I am interested in (Core_loss=1.07W, Winding=2.23W,
deltaB=25.3mT). Not much to save already, a lot to spoil winding it
improperly.

> and MPP will be better

It is extremely stable, but its saturation properties are disappointing.

> but any good Ferrite (3F3) tops all.

Good ferrite is 3C95, used elsewhere in the converter. The main
transformer is (present tense, as it has been prototyped) wound on
an E43 planar core for its tremendous area to volume ratio. And the
40uH resonant inductor is also magnetically integrated within
the structure. Beauty, I'll show it to you later.

> you can drop back to Kool-Mu, (2 stacked donuts.)

This is also an option worth considering, thanks Bitrex, BTW.

> 150KHz may be difficult for MOSFETs and magnetics. SiC MOSFETs may be needed but the diode must always be SiC.

This is going to be an all-SiC design, based on 6xC3M0065090J. And there
will be no diode, I have always been a big fan of synchronous
rectification. SiC would be required in the totem-pole topology anyway,
so there are many reasons to go that way.

> Do not go to three layers!

Yes, this is my biggest concern.

Best regards, Piotr
 
Piotr Wyderski wrote...
In fact, the entire converter is designed around
this cap. The "I am what I am, find a way of
using me" LLC transformer is another such a place.

Is that the one you designed with an intrinsic
series-resonating inductor?

> The bottom-up approach sometimes pays off.

Its sometimes a bit embarrassing to admit it, but
often finding an available capable component can
be the foundation of a push-the-limits design.


--
Thanks,
- Win
 
On Mon, 29 Jul 2019 08:47:14 +0200, Piotr Wyderski
<peter.pan@neverland.mil> wrote:

Harry D wrote:

Math is oK when used with SPICE and Breadboarding. If you need high efficiency, then you need many loops of the three magic steps. (MSB) This will reduce the L to about 300uF. At 150KHz your Kool-Mu will be hot-Mu

This is for CCM with deltaB=30mT or so. The manufacturer's design tool
as well as the Steinmetz coefficients for the material bolted into a
Matlab script consistently report core losses of about 1W. Winding
losses are higher, but even that bumps the temperature up by at most
35 degrees for the worst design option. It is estimated to be 25.6 deg
in the case I am interested in (Core_loss=1.07W, Winding=2.23W,
deltaB=25.3mT). Not much to save already, a lot to spoil winding it
improperly.

and MPP will be better

It is extremely stable, but its saturation properties are disappointing.

but any good Ferrite (3F3) tops all.

Good ferrite is 3C95, used elsewhere in the converter. The main
transformer is (present tense, as it has been prototyped) wound on
an E43 planar core for its tremendous area to volume ratio. And the
40uH resonant inductor is also magnetically integrated within
the structure. Beauty, I'll show it to you later.

you can drop back to Kool-Mu, (2 stacked donuts.)

This is also an option worth considering, thanks Bitrex, BTW.

150KHz may be difficult for MOSFETs and magnetics. SiC MOSFETs may be needed but the diode must always be SiC.

This is going to be an all-SiC design, based on 6xC3M0065090J. And there
will be no diode, I have always been a big fan of synchronous
rectification. SiC would be required in the totem-pole topology anyway,
so there are many reasons to go that way.

Do not go to three layers!

Yes, this is my biggest concern.

Best regards, Piotr

I guess there is a concern for the heat getting out of inner windings.
The path through the copper is long.


--

John Larkin Highland Technology, Inc

lunatic fringe electronics
 
On Mon, 29 Jul 2019 08:05:44 +0200, Piotr Wyderski
<peter.pan@neverland.mil> wrote:

John Larkin wrote:

Doesn't a PFC booster need milliseconds of holdup, as the AC line
crosses zero?

Holdup is for the situation when the AC stays zero for a predefined
time. Typically one line cycle in the case of servers, to allow them to
save critical data (which doesn't happen, anyway...). In this case this
application t_holdup=0, as there will be a battery switchover. The
capacitor is only to provide a reasonable ripple value. I have assumed
deltaV of 60V, which is just 10% of the 600V V_BUS. The downstream LLC
will have no problems with that.

Best regards, Piotr

The AC line around here crosses zero 120 times a second! That's what I
was referring to.

60v p-p ripple sounds about right. If there's a downstream switcher,
its input impedance will be negative so the ripple is exponential in
the downward direction.

"Things don't go to hell in a straight line."


--

John Larkin Highland Technology, Inc

lunatic fringe electronics
 
PFC stage efficiency around 99% is standard:

https://www.infineon.com/dgdl/Infineon-Introduction_to_CoolSiC_Schottky_Diodes_650V_G6-AN-v01_00-EN.pdf?fileId=5546d4625e763904015eb8faeffd5373

Sorry for the brief post, busy days

Cheers

Klaus
 
Klaus Kragelund wrote...
PFC stage efficiency around 99% is standard:

https://www.infineon.com/dgdl/Infineon-Introduction_to_CoolSiC_Schottky_Diodes_650V_G6-AN-v01_00-EN.pdf?fileId=5546d4625e763904015eb8faeffd5373

Maybe you should rather say it's a standard
goal for a manufacturer showing off exceptional
performance, such as the one in the link.

But I wonder what real-world "standard" values
are for power supplies we generally encounter,
for example in a 500-watt PC power supply. This
brings up the issue that it's not easy to make
accurate measurements of AC-in DC-out losses,
especially down at the 1% level. DC-in DC-out,
yes, but PFC boost converters, no, SFAICT. The
Institute's electronics-engineering lab is well
equipped, but I currently cannot be sure of any
high crest-factor AC-power measurements, to
better than 1% to 2%.

For that matter, can we trust Infineon's data,
229.6 volts AC, 4.431 amps AC = 1014.9 watts,
e.g., to the 0.01% level, for a 98.198% result
(PFC boost converter design guide, page 20),
without any indication of how it was measured?
The very fact they give the result to 0.001% is
an indication of careless error-bar evaluation.

OK, one note mentions Yokogawa's WT330 meter,
spec: 0.1% of reading + 0.1% of range (300V),
which is 229 +/- 0.529 volts = 0.23% accuracy.
Hmm, it'd be nice to have one of those, but
we're still talking 0.25% not 0.1% certainty.
That's a 25% error at the 1% loss level.


--
Thanks,
- Win
 

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