EDAboard.com | EDAboard.eu | EDAboard.de | EDAboard.co.uk | RTV forum PL | NewsGroups PL

Heating in 4-1/2 turn inductor

Ask a question - edaboard.com

elektroda.net NewsGroups Forum Index - Electronics Design - Heating in 4-1/2 turn inductor

Goto page Previous  1, 2, 3, 4

coffelt2
Guest

Wed Sep 01, 2010 6:31 am   



I tried reading and understanding most of the posts, but confess not
understanding all of them.
BUT, I cannot resist inserting my "two cents" worth:

In olden days, it was quite common (but unwelcome) to have parasitic
oscillations run away in large RF amplifiers. They would start all by
themselves and quickly begin roasting tubes, coils, even adjacent conductive
surfaces, whatever got in the way. The often encountered case would be a HF
amplifier running away (self-oscillating for the unwashed) at a VHF or UHF
frequency.

One common, but mysterious result was burned parts of RF chokes in the
plate circuit. (you do remember tubes, right?) I think there were a couple
of commercial RF chokes wound on long ceramic (steatite?) cores with
assorted winding spacings on the ceramic core. Burned spots would occur in
only one or two places on the length of the winding. Caused, supposedly by a
high current node on a VHF or UHF resonant portion of the winding.

4 1/2 turns at 600khz must be an awfully low impedance circuit, but
could be right down the alley for VHF.

Brian has my vote for barking up the right tree.

Old Chief Lynn, W7LTQ

amdx
Guest

Fri Sep 03, 2010 4:01 pm   



"JosephKK" <quiettechblue_at_yahoo.com> wrote in message
news:09nr76pocud1tlt20hkkacuu70up65551h_at_4ax.com...
Quote:
On Sun, 29 Aug 2010 14:37:49 -0500, "amdx" <amdx_at_knology.net> wrote:


"JosephKK" <quiettechblue_at_yahoo.com> wrote in message
news:4sok76hb6040167vgd69cr6n7hbe6bdogt_at_4ax.com...
On Fri, 27 Aug 2010 14:23:13 -0700 (PDT), whit3rd <whit3rd_at_gmail.com
wrote:

On Aug 27, 1:30 pm, "Jeff Johnson" <Jeff_John...@Hotmail.com> wrote:
"whit3rd" <whit...@gmail.com> wrote in message

news:69863d94-450f-49b5-bdc0-4428e4f21c20_at_h19g2000yqb.googlegroups.com...

On Aug 27, 10:31 am, "Jeff Johnson" <Jeff_John...@Hotmail.com
wrote:

The theory of ideal inductors does not give any reason why a 1/2
turn
should
at all be important.

Oh, yes, it DOES give a reason. A pot core (or E cores) has a pair
of
return
flux arms flanking the central element, and a '1/2 turn' winding
imbalances
those return fluxes.

In the ideal case the fringe effects are usually ignored.

What 'fringe effects'? This is about the flux contained in the
magnetic arms of the core, not outside somewhere

That means the 3-d flux inside the core is very different in the
two cases, and if one return arm saturates, that flux distribution
alters
considerably during the cycle. That causes (1) the material to heat
due to remagnetization in an asymmetric way, (2) the forces of the
pole pieces to modulate as the field builds. The first effect
(caused
by material hysteresis) might have been expected. The second
effect, though, will cause ultrasonic excitation of the core, maybe
creating cracks by mechanical stress.

...all the effects you describe should heat the central
windings more than the outside and have little to do with the end turn
amount.

Oh, this has nothing to do with ohmic heating in the windings. It
concerns
the B-H curve, which (for a hysteretic material) loops around some
area.
At 600 kHz, the area, multiplied by 6e6, is the power lost when the
magnetic material is forced to traverse that loop.
If part of the material saturates, its loop is of greater area than
the rest of
the material. A core that should handle 2A without overheating, then
would overheat.

You may be on to something. Maybe. At least it make physics sense to
me, but then i are enguneer. It does show a path to have thermal
non-uniformity that is regenreative.

Say Mike just how big is that pot core?

I think it may have been a 3622 but could have been a 4229.
MikeK

I take it that is dimensions in mm. What material? Minimum
"thickness" (cross section)

Here's the pdf on the core I think was used. The material was 3F3.
I don't know the gap size, I thought we generally used the 160 gap,
but I don't even see that listed. I decided it's more likely we used the
4229
than the 3622. It's been 10 years so details have faded.
http://www.ferroxcube.com/prod/assets/p4229.pdf

raypsi
Guest

Sun Sep 05, 2010 2:32 am   



Hey OT:

I stand by my proximity effect.

The Q is equal to Rl/Xc the half turn has twice as much Xc so the Q
for that turn is half as much as the other turns because of proximity
Thus the Pd in the half turn is 4 times the Pd in the other turns.

73 OT
de n8zu



On Aug 25, 12:09 pm, "amdx" <a...@knology.net> wrote:
Quote:
Several years ago while making inductors for tuning a class E amplifier we
end up with a 4-1/2 turn inductor. The inductor used a 3F3 potcore, gapped I
think,
but it has been awhile. The inductor was driven hard but below saturation..
The problem; the 1/2 turn got HOT.  Four turns or five turns were ok.
 My physicist friend had an EE verify the problem 2000 miles away.

So, can anyone tell me why 1/2 turn would make such a difference in the
heating?

                                Thanks, MikeK


JosephKK
Guest

Sun Sep 05, 2010 3:38 am   



On Fri, 3 Sep 2010 10:01:03 -0500, "amdx" <amdx_at_knology.net> wrote:

Quote:

"JosephKK" <quiettechblue_at_yahoo.com> wrote in message
news:09nr76pocud1tlt20hkkacuu70up65551h_at_4ax.com...
On Sun, 29 Aug 2010 14:37:49 -0500, "amdx" <amdx_at_knology.net> wrote:


"JosephKK" <quiettechblue_at_yahoo.com> wrote in message
news:4sok76hb6040167vgd69cr6n7hbe6bdogt_at_4ax.com...
On Fri, 27 Aug 2010 14:23:13 -0700 (PDT), whit3rd <whit3rd_at_gmail.com
wrote:

On Aug 27, 1:30 pm, "Jeff Johnson" <Jeff_John...@Hotmail.com> wrote:
"whit3rd" <whit...@gmail.com> wrote in message

news:69863d94-450f-49b5-bdc0-4428e4f21c20_at_h19g2000yqb.googlegroups.com...

On Aug 27, 10:31 am, "Jeff Johnson" <Jeff_John...@Hotmail.com
wrote:

The theory of ideal inductors does not give any reason why a 1/2
turn
should
at all be important.

Oh, yes, it DOES give a reason. A pot core (or E cores) has a pair
of
return
flux arms flanking the central element, and a '1/2 turn' winding
imbalances
those return fluxes.

In the ideal case the fringe effects are usually ignored.

What 'fringe effects'? This is about the flux contained in the
magnetic arms of the core, not outside somewhere

That means the 3-d flux inside the core is very different in the
two cases, and if one return arm saturates, that flux distribution
alters
considerably during the cycle. That causes (1) the material to heat
due to remagnetization in an asymmetric way, (2) the forces of the
pole pieces to modulate as the field builds. The first effect
(caused
by material hysteresis) might have been expected. The second
effect, though, will cause ultrasonic excitation of the core, maybe
creating cracks by mechanical stress.

...all the effects you describe should heat the central
windings more than the outside and have little to do with the end turn
amount.

Oh, this has nothing to do with ohmic heating in the windings. It
concerns
the B-H curve, which (for a hysteretic material) loops around some
area.
At 600 kHz, the area, multiplied by 6e6, is the power lost when the
magnetic material is forced to traverse that loop.
If part of the material saturates, its loop is of greater area than
the rest of
the material. A core that should handle 2A without overheating, then
would overheat.

You may be on to something. Maybe. At least it make physics sense to
me, but then i are enguneer. It does show a path to have thermal
non-uniformity that is regenreative.

Say Mike just how big is that pot core?

I think it may have been a 3622 but could have been a 4229.
MikeK

I take it that is dimensions in mm. What material? Minimum
"thickness" (cross section)

Here's the pdf on the core I think was used. The material was 3F3.
I don't know the gap size, I thought we generally used the 160 gap,
but I don't even see that listed. I decided it's more likely we used the
4229
than the 3622. It's been 10 years so details have faded.
http://www.ferroxcube.com/prod/assets/p4229.pdf


Thanks, i will have to study some to be able to read that datasheet.


Fred Abse
Guest

Sun Sep 05, 2010 4:57 pm   



On Sat, 04 Sep 2010 16:57:22 -0700, raypsi top posted:

Quote:
The Q is equal to Rl/Xc the half turn has twice as much Xc so the Q
for that turn is half as much as the other turns because of proximity
Thus the Pd in the half turn is 4 times the Pd in the other turns.

Q equals reactance/resistance, not resistance/reactance.
Xc is capacitive reactance, not inductive reactance.
The voltage across an inductor having resistance does not depend on Q
alone, the "4 times" is complete nonsense.

--
"For a successful technology, reality must take precedence
over public relations, for nature cannot be fooled."
(Richard Feynman)

raypsi
Guest

Wed Sep 08, 2010 5:32 am   



Hey OT:

The capacitance of one winding to the next is still present. In this
case a half winding.

More axactly in the 19th edition of Bill Orr's
Radio Hand book page 11.28 if you care to look it up.
We all know Bill Orr won't make such a glaring error.
What you are looking at is RS, Not RL So Q equal to Rl/Xc
it is also equal to wXc/Rs. The DF in the Xc is exactly what you state
So it's still 4 times the power loss in the half turn. But every one
knows DF equals 1/Q
So in essence you agree with me.

Later OM
de n8zu


On Sep 5, 11:57 am, Fred Abse <excretatau...@invalid.invalid> wrot> On
Sat, 04 Sep 2010 16:57:22 -0700, raypsi top poste
Quote:
The Q is equal to Rl/Xc the half turn has twice as much Xc so the Q
for that turn is half  as much as the other turns because of proximity
Thus the Pd in the half turn is 4 times the Pd in the other turns.

Q equals reactance/resistance, not resistance/reactance.
Xc is capacitive reactance, not inductive reactance.
The voltage across an inductor having resistance does not depend on Q
alone, the "4 times" is complete nonsense.

--
"For a successful technology, reality must take precedence
over public relations, for nature cannot be fooled."
                                       (Richard Feynman)


Goto page Previous  1, 2, 3, 4

elektroda.net NewsGroups Forum Index - Electronics Design - Heating in 4-1/2 turn inductor

Ask a question - edaboard.com

Arabic versionBulgarian versionCatalan versionCzech versionDanish versionGerman versionGreek versionEnglish versionSpanish versionFinnish versionFrench versionHindi versionCroatian versionIndonesian versionItalian versionHebrew versionJapanese versionKorean versionLithuanian versionLatvian versionDutch versionNorwegian versionPolish versionPortuguese versionRomanian versionRussian versionSlovak versionSlovenian versionSerbian versionSwedish versionTagalog versionUkrainian versionVietnamese versionChinese version
RTV map EDAboard.com map News map EDAboard.eu map EDAboard.de map EDAboard.co.uk map Opony