Driver to drive?

On 26.3.17 17:35, Joerg wrote:
On 2017-03-25 18:39, rickman wrote:
On 3/25/2017 3:30 PM, Joerg wrote:
On 2017-03-25 10:49, rickman wrote:
On 3/24/2017 4:36 PM, Joerg wrote:
On 2017-03-24 10:59, rickman wrote:
On 3/24/2017 1:14 PM, Joerg wrote:
On 2017-03-20 02:06, Tauno Voipio wrote:

[...]

Please do not use PVC as RF insulation or support pieces.
It is lossy to extremely lossy at RF.


Plasticized PVC ain't stellar but not horrid.

http://g3ynh.info/zdocs/comps/part_6.html

Or do they add a lot of vispipuuro into the mix in Finland? :)

Are you reading the same page? It says PVC Tanδ is 0.04 - 0.14 at 1
MHz. That is in no way acceptable for the sort of high Q circuits
that
are being discussed. That's comparable to wood, 0.059.

This page even lists PVC in the "Lossy" group as defined by Tanδ ≥
0.01.


The losses in ferrite rods are nothing to sneeze at in comparison. I
have used both in ham radio a lot when I was young. I built kilowatt
level RF power amps, impedance matching boxes and similar gear.
Ferrite
rods in transmitters sometimes became so hot that you could barely
touch
them while inductors wound on some random piece of PVC pipe remained
cool. I don't remember the PVC type other than that it was remnants
they
sold for pennies in the plumbing department so that was very likely
well
plasticized.

Maybe I don't recall the context of the ferrite, but the receiving
antennas in much of this thread and described in detail at Kleijer's
web
site showed measurable losses with better plastics than PVC. Even
cardboard was a poor support relatively speaking. Seems he would use a
foam type plastic to get some rigidity with a minimum of loss. Foam
PVC
was not bad, but his Q measurements increased significantly with foam
polypropylene. Obviously foam is better because there is less actual
material. Solid PVC would show more pronounced losses.

He does some amazingly detailed work. You might find it interesting.
The LC experiments were reported in a series of web pages. Page 10
doesn't have a link to page 11, but otherwise they are all chained.


Looks like there isn't a page 11.

That's what I was saying. There *is* a page 11, page 10 just doesn't
have a link to it. Go back to the index.


Indeed. I change the number in the URL by hand by starting with page 11
he change the URL structure. Well, I am not complaining, my web site
design skills aren't that great either.


http://www.crystal-radio.eu/enlctest.htm


He gets good Q with PVC. Worse with cardboard but who knows what kind of
stuff he used. It looks like carton material. That is often
post-consumer recycled and you never know what's in it. Water content is
another factor, got to bake it out and then lacquer it immediately
afterwards.

He gets good Q with FOAM PVC. Totally different from solid PVC, much
less of it and a lot more air. The point is foam anything else worked
even better.


Look at page 7. Very nice Q values except for the dirty pipe yet this is
all on regular PVC pipe.


The huge jump in Q in part 3 shows that he used the wrong measurement
setup until then. You can't do this sort of stuff with a 100:1 scope
probe, it has to be at least a high-end FET probe. However, hat off, he
achieved amazing Q values in his experiments.

Look at the Q values he gets in part 7. Those are all regular plumbing
PVC pipes. L16 has lower Q but that PVC tube isn't even particularly
clean. It is important to keep or make them pristine when building
high-Q stuff.


I found it very illuminating his tests with the variable capacitors.
Even parts like bushings were found to make a difference.


I remember that from my ham radio days. Dirty or oxidized rotor contacts
.... phssssst ... PHUT ... *BANG* and worst case that could take the
tubes into the abyss along with it. I also spent part of a Wenol
polishing paste tube keeping the final Pi-filter inductor shiny so it
wouldn't heat up too badly and unsolder a connection to it (which could
also result in a loud bang).

BTW, while such high Q isn't all that useful in practice if you ever
needed that there are simpler means to achieve it. An old method is the
"Q-multiplier". In essence the resonance circuit sits inside an
amplifier stage that is deliberately pulled very close to oscillation.
That shrinks the bandwidth big time.

How do you accomplish that without an amplifier? You did notice the
site is all about *crystal* radios, right?


You need an amplifier for that. If you want to you can make an
energy-harvesting one, sans battery. I mentioned this method purely as a
hint, in case anyone ever needs high Q without making fancy large coils
and babying them.

Joerg, you seem not understand the innermost sense of the crystal-
radio people. They are closely related to audiophools, and it is
quite impossible to use sensible technical argumentation here.

The question of best MF band coils has been solved already in the
1930's: A honeycomb coil wound with Litz wire (gloves on). The
canonical fixing / insulating material is beeswax.

--

-TV
 
On 3/27/2017 6:57 AM, Tauno Voipio wrote:
On 26.3.17 17:35, Joerg wrote:
On 2017-03-25 18:39, rickman wrote:
On 3/25/2017 3:30 PM, Joerg wrote:
On 2017-03-25 10:49, rickman wrote:
On 3/24/2017 4:36 PM, Joerg wrote:
On 2017-03-24 10:59, rickman wrote:
On 3/24/2017 1:14 PM, Joerg wrote:
On 2017-03-20 02:06, Tauno Voipio wrote:

[...]

Please do not use PVC as RF insulation or support pieces.
It is lossy to extremely lossy at RF.


Plasticized PVC ain't stellar but not horrid.

http://g3ynh.info/zdocs/comps/part_6.html

Or do they add a lot of vispipuuro into the mix in Finland? :)

Are you reading the same page? It says PVC Tanδ is 0.04 - 0.14 at 1
MHz. That is in no way acceptable for the sort of high Q circuits
that
are being discussed. That's comparable to wood, 0.059.

This page even lists PVC in the "Lossy" group as defined by Tanδ ≥
0.01.


The losses in ferrite rods are nothing to sneeze at in comparison. I
have used both in ham radio a lot when I was young. I built kilowatt
level RF power amps, impedance matching boxes and similar gear.
Ferrite
rods in transmitters sometimes became so hot that you could barely
touch
them while inductors wound on some random piece of PVC pipe remained
cool. I don't remember the PVC type other than that it was remnants
they
sold for pennies in the plumbing department so that was very likely
well
plasticized.

Maybe I don't recall the context of the ferrite, but the receiving
antennas in much of this thread and described in detail at Kleijer's
web
site showed measurable losses with better plastics than PVC. Even
cardboard was a poor support relatively speaking. Seems he would
use a
foam type plastic to get some rigidity with a minimum of loss. Foam
PVC
was not bad, but his Q measurements increased significantly with foam
polypropylene. Obviously foam is better because there is less actual
material. Solid PVC would show more pronounced losses.

He does some amazingly detailed work. You might find it interesting.
The LC experiments were reported in a series of web pages. Page 10
doesn't have a link to page 11, but otherwise they are all chained.


Looks like there isn't a page 11.

That's what I was saying. There *is* a page 11, page 10 just doesn't
have a link to it. Go back to the index.


Indeed. I change the number in the URL by hand by starting with page 11
he change the URL structure. Well, I am not complaining, my web site
design skills aren't that great either.


http://www.crystal-radio.eu/enlctest.htm


He gets good Q with PVC. Worse with cardboard but who knows what
kind of
stuff he used. It looks like carton material. That is often
post-consumer recycled and you never know what's in it. Water
content is
another factor, got to bake it out and then lacquer it immediately
afterwards.

He gets good Q with FOAM PVC. Totally different from solid PVC, much
less of it and a lot more air. The point is foam anything else worked
even better.


Look at page 7. Very nice Q values except for the dirty pipe yet this is
all on regular PVC pipe.


The huge jump in Q in part 3 shows that he used the wrong measurement
setup until then. You can't do this sort of stuff with a 100:1 scope
probe, it has to be at least a high-end FET probe. However, hat off, he
achieved amazing Q values in his experiments.

Look at the Q values he gets in part 7. Those are all regular plumbing
PVC pipes. L16 has lower Q but that PVC tube isn't even particularly
clean. It is important to keep or make them pristine when building
high-Q stuff.


I found it very illuminating his tests with the variable capacitors.
Even parts like bushings were found to make a difference.


I remember that from my ham radio days. Dirty or oxidized rotor
contacts
.... phssssst ... PHUT ... *BANG* and worst case that could take the
tubes into the abyss along with it. I also spent part of a Wenol
polishing paste tube keeping the final Pi-filter inductor shiny so it
wouldn't heat up too badly and unsolder a connection to it (which could
also result in a loud bang).

BTW, while such high Q isn't all that useful in practice if you ever
needed that there are simpler means to achieve it. An old method is the
"Q-multiplier". In essence the resonance circuit sits inside an
amplifier stage that is deliberately pulled very close to oscillation.
That shrinks the bandwidth big time.

How do you accomplish that without an amplifier? You did notice the
site is all about *crystal* radios, right?


You need an amplifier for that. If you want to you can make an
energy-harvesting one, sans battery. I mentioned this method purely as a
hint, in case anyone ever needs high Q without making fancy large coils
and babying them.


Joerg, you seem not understand the innermost sense of the crystal-
radio people. They are closely related to audiophools, and it is
quite impossible to use sensible technical argumentation here.

I don't get that at all, can you back that up with any facts?

The question of best MF band coils has been solved already in the
1930's: A honeycomb coil wound with Litz wire (gloves on). The
canonical fixing / insulating material is beeswax.
I don't know have you tried a 6" polystyrene tube with 0.0625 wall
thickness, wound with 660/46 litz wire with 12 turns per inch?

If anyone has an interest, here's a pdf of multiple honeycomb coils
and data. I think it is from the 30's or 40's. I can't seem to get
it to download properly. But what I could see doesn't give Q directly,
so needs to be calculated.
> http://nvlpubs.nist.gov/nistpubs/nbstechnologic/nbstechnologicpapert298.pdf

Mikek


Mikek

---
This email has been checked for viruses by Avast antivirus software.
https://www.avast.com/antivirus
 
Den mandag den 27. marts 2017 kl. 14.25.07 UTC+2 skrev amdx:
On 3/27/2017 6:57 AM, Tauno Voipio wrote:
On 26.3.17 17:35, Joerg wrote:
On 2017-03-25 18:39, rickman wrote:
On 3/25/2017 3:30 PM, Joerg wrote:
On 2017-03-25 10:49, rickman wrote:
On 3/24/2017 4:36 PM, Joerg wrote:
On 2017-03-24 10:59, rickman wrote:
On 3/24/2017 1:14 PM, Joerg wrote:
On 2017-03-20 02:06, Tauno Voipio wrote:

[...]

Please do not use PVC as RF insulation or support pieces.
It is lossy to extremely lossy at RF.


Plasticized PVC ain't stellar but not horrid.

http://g3ynh.info/zdocs/comps/part_6.html

Or do they add a lot of vispipuuro into the mix in Finland? :)

Are you reading the same page? It says PVC Tanδ is 0.04 - 0..14 at 1
MHz. That is in no way acceptable for the sort of high Q circuits
that
are being discussed. That's comparable to wood, 0.059.

This page even lists PVC in the "Lossy" group as defined by Tanδ ≥
0.01.


The losses in ferrite rods are nothing to sneeze at in comparison. I
have used both in ham radio a lot when I was young. I built kilowatt
level RF power amps, impedance matching boxes and similar gear.
Ferrite
rods in transmitters sometimes became so hot that you could barely
touch
them while inductors wound on some random piece of PVC pipe remained
cool. I don't remember the PVC type other than that it was remnants
they
sold for pennies in the plumbing department so that was very likely
well
plasticized.

Maybe I don't recall the context of the ferrite, but the receiving
antennas in much of this thread and described in detail at Kleijer's
web
site showed measurable losses with better plastics than PVC. Even
cardboard was a poor support relatively speaking. Seems he would
use a
foam type plastic to get some rigidity with a minimum of loss. Foam
PVC
was not bad, but his Q measurements increased significantly with foam
polypropylene. Obviously foam is better because there is less actual
material. Solid PVC would show more pronounced losses.

He does some amazingly detailed work. You might find it interesting.
The LC experiments were reported in a series of web pages. Page 10
doesn't have a link to page 11, but otherwise they are all chained.


Looks like there isn't a page 11.

That's what I was saying. There *is* a page 11, page 10 just doesn't
have a link to it. Go back to the index.


Indeed. I change the number in the URL by hand by starting with page 11
he change the URL structure. Well, I am not complaining, my web site
design skills aren't that great either.


http://www.crystal-radio.eu/enlctest.htm


He gets good Q with PVC. Worse with cardboard but who knows what
kind of
stuff he used. It looks like carton material. That is often
post-consumer recycled and you never know what's in it. Water
content is
another factor, got to bake it out and then lacquer it immediately
afterwards.

He gets good Q with FOAM PVC. Totally different from solid PVC, much
less of it and a lot more air. The point is foam anything else worked
even better.


Look at page 7. Very nice Q values except for the dirty pipe yet this is
all on regular PVC pipe.


The huge jump in Q in part 3 shows that he used the wrong measurement
setup until then. You can't do this sort of stuff with a 100:1 scope
probe, it has to be at least a high-end FET probe. However, hat off, he
achieved amazing Q values in his experiments.

Look at the Q values he gets in part 7. Those are all regular plumbing
PVC pipes. L16 has lower Q but that PVC tube isn't even particularly
clean. It is important to keep or make them pristine when building
high-Q stuff.


I found it very illuminating his tests with the variable capacitors..
Even parts like bushings were found to make a difference.


I remember that from my ham radio days. Dirty or oxidized rotor
contacts
.... phssssst ... PHUT ... *BANG* and worst case that could take the
tubes into the abyss along with it. I also spent part of a Wenol
polishing paste tube keeping the final Pi-filter inductor shiny so it
wouldn't heat up too badly and unsolder a connection to it (which could
also result in a loud bang).

BTW, while such high Q isn't all that useful in practice if you ever
needed that there are simpler means to achieve it. An old method is the
"Q-multiplier". In essence the resonance circuit sits inside an
amplifier stage that is deliberately pulled very close to oscillation.
That shrinks the bandwidth big time.

How do you accomplish that without an amplifier? You did notice the
site is all about *crystal* radios, right?


You need an amplifier for that. If you want to you can make an
energy-harvesting one, sans battery. I mentioned this method purely as a
hint, in case anyone ever needs high Q without making fancy large coils
and babying them.


Joerg, you seem not understand the innermost sense of the crystal-
radio people. They are closely related to audiophools, and it is
quite impossible to use sensible technical argumentation here.

I don't get that at all, can you back that up with any facts?


The question of best MF band coils has been solved already in the
1930's: A honeycomb coil wound with Litz wire (gloves on). The
canonical fixing / insulating material is beeswax.

I don't know have you tried a 6" polystyrene tube with 0.0625 wall
thickness, wound with 660/46 litz wire with 12 turns per inch?

sound like it needs more unicorn tears and maturing under a full moon

;)
 
On 2017-03-26 10:15, rickman wrote:
On 3/26/2017 10:35 AM, Joerg wrote:
On 2017-03-25 18:39, rickman wrote:
On 3/25/2017 3:30 PM, Joerg wrote:
On 2017-03-25 10:49, rickman wrote:
On 3/24/2017 4:36 PM, Joerg wrote:
On 2017-03-24 10:59, rickman wrote:
On 3/24/2017 1:14 PM, Joerg wrote:
On 2017-03-20 02:06, Tauno Voipio wrote:

[...]

Please do not use PVC as RF insulation or support pieces.
It is lossy to extremely lossy at RF.


Plasticized PVC ain't stellar but not horrid.

http://g3ynh.info/zdocs/comps/part_6.html

Or do they add a lot of vispipuuro into the mix in Finland? :)

Are you reading the same page? It says PVC Tanδ is 0.04 - 0.14 at 1
MHz. That is in no way acceptable for the sort of high Q circuits
that
are being discussed. That's comparable to wood, 0.059.

This page even lists PVC in the "Lossy" group as defined by Tanδ ≥
0.01.


The losses in ferrite rods are nothing to sneeze at in comparison. I
have used both in ham radio a lot when I was young. I built kilowatt
level RF power amps, impedance matching boxes and similar gear.
Ferrite
rods in transmitters sometimes became so hot that you could barely
touch
them while inductors wound on some random piece of PVC pipe remained
cool. I don't remember the PVC type other than that it was remnants
they
sold for pennies in the plumbing department so that was very likely
well
plasticized.

Maybe I don't recall the context of the ferrite, but the receiving
antennas in much of this thread and described in detail at Kleijer's
web
site showed measurable losses with better plastics than PVC. Even
cardboard was a poor support relatively speaking. Seems he would
use a
foam type plastic to get some rigidity with a minimum of loss. Foam
PVC
was not bad, but his Q measurements increased significantly with foam
polypropylene. Obviously foam is better because there is less actual
material. Solid PVC would show more pronounced losses.

He does some amazingly detailed work. You might find it interesting.
The LC experiments were reported in a series of web pages. Page 10
doesn't have a link to page 11, but otherwise they are all chained.


Looks like there isn't a page 11.

That's what I was saying. There *is* a page 11, page 10 just doesn't
have a link to it. Go back to the index.


Indeed. I change the number in the URL by hand by starting with page 11
he change the URL structure. Well, I am not complaining, my web site
design skills aren't that great either.


http://www.crystal-radio.eu/enlctest.htm


He gets good Q with PVC. Worse with cardboard but who knows what
kind of
stuff he used. It looks like carton material. That is often
post-consumer recycled and you never know what's in it. Water
content is
another factor, got to bake it out and then lacquer it immediately
afterwards.

He gets good Q with FOAM PVC. Totally different from solid PVC, much
less of it and a lot more air. The point is foam anything else worked
even better.


Look at page 7. Very nice Q values except for the dirty pipe yet this is
all on regular PVC pipe.

Compared to what? He is comparing coil winding methods. What would the
Q be with other supports?

The Q is over 500. It was claimed in this thread that PVC is not
suitable as coil winding material and this proves that it is quite
suitable. Which I already knew because I've used it in RF power amps
decades ago.

The huge jump in Q in part 3 shows that he used the wrong measurement
setup until then. You can't do this sort of stuff with a 100:1 scope
probe, it has to be at least a high-end FET probe. However, hat off, he
achieved amazing Q values in his experiments.

Look at the Q values he gets in part 7. Those are all regular plumbing
PVC pipes. L16 has lower Q but that PVC tube isn't even particularly
clean. It is important to keep or make them pristine when building
high-Q stuff.


I found it very illuminating his tests with the variable capacitors.
Even parts like bushings were found to make a difference.


I remember that from my ham radio days. Dirty or oxidized rotor
contacts
.... phssssst ... PHUT ... *BANG* and worst case that could take the
tubes into the abyss along with it. I also spent part of a Wenol
polishing paste tube keeping the final Pi-filter inductor shiny so it
wouldn't heat up too badly and unsolder a connection to it (which could
also result in a loud bang).

BTW, while such high Q isn't all that useful in practice if you ever
needed that there are simpler means to achieve it. An old method is the
"Q-multiplier". In essence the resonance circuit sits inside an
amplifier stage that is deliberately pulled very close to oscillation.
That shrinks the bandwidth big time.

How do you accomplish that without an amplifier? You did notice the
site is all about *crystal* radios, right?


You need an amplifier for that. If you want to you can make an
energy-harvesting one, sans battery. I mentioned this method purely as a
hint, in case anyone ever needs high Q without making fancy large coils
and babying them.

What energy will be harvested?

The energy present in the environment, for example energy from the local
radio transmitters. You can then use that to demodulate the signals of
others.

http://mwrf.com/systems/harvesting-energy-rf-sources

--
Regards, Joerg

http://www.analogconsultants.com/
 
On 2017-03-27 04:57, Tauno Voipio wrote:
On 26.3.17 17:35, Joerg wrote:
On 2017-03-25 18:39, rickman wrote:
On 3/25/2017 3:30 PM, Joerg wrote:
On 2017-03-25 10:49, rickman wrote:

[...]

I found it very illuminating his tests with the variable capacitors.
Even parts like bushings were found to make a difference.


I remember that from my ham radio days. Dirty or oxidized rotor
contacts
.... phssssst ... PHUT ... *BANG* and worst case that could take the
tubes into the abyss along with it. I also spent part of a Wenol
polishing paste tube keeping the final Pi-filter inductor shiny so it
wouldn't heat up too badly and unsolder a connection to it (which could
also result in a loud bang).

BTW, while such high Q isn't all that useful in practice if you ever
needed that there are simpler means to achieve it. An old method is the
"Q-multiplier". In essence the resonance circuit sits inside an
amplifier stage that is deliberately pulled very close to oscillation.
That shrinks the bandwidth big time.

How do you accomplish that without an amplifier? You did notice the
site is all about *crystal* radios, right?


You need an amplifier for that. If you want to you can make an
energy-harvesting one, sans battery. I mentioned this method purely as a
hint, in case anyone ever needs high Q without making fancy large coils
and babying them.


Joerg, you seem not understand the innermost sense of the crystal-
radio people. They are closely related to audiophools, and it is
quite impossible to use sensible technical argumentation here.

I know :)

However, AFAIK Rick is a guy working in digital electronics.


The question of best MF band coils has been solved already in the
1930's: A honeycomb coil wound with Litz wire (gloves on). The
canonical fixing / insulating material is beeswax.

Only when mounted on a polished mohagony slab of wood, with the user
wearing Sundays's best and a bow tie :)

BTW, I have a Loewe radio with the 3NF type. That is probably the first
true integrated circuit from 90 years ago because it contained multiple
tube sections, capacitors and resistors.

http://www.electricstuff.co.uk/loewe.html

--
Regards, Joerg

http://www.analogconsultants.com/
 
On 3/27/2017 10:46 AM, Joerg wrote:
On 2017-03-26 10:15, rickman wrote:
On 3/26/2017 10:35 AM, Joerg wrote:
On 2017-03-25 18:39, rickman wrote:
On 3/25/2017 3:30 PM, Joerg wrote:
On 2017-03-25 10:49, rickman wrote:
On 3/24/2017 4:36 PM, Joerg wrote:
On 2017-03-24 10:59, rickman wrote:
On 3/24/2017 1:14 PM, Joerg wrote:
On 2017-03-20 02:06, Tauno Voipio wrote:

[...]

Please do not use PVC as RF insulation or support pieces.
It is lossy to extremely lossy at RF.


Plasticized PVC ain't stellar but not horrid.

http://g3ynh.info/zdocs/comps/part_6.html

Or do they add a lot of vispipuuro into the mix in Finland? :)

Are you reading the same page? It says PVC Tanδ is 0.04 - 0.14
at 1
MHz. That is in no way acceptable for the sort of high Q circuits
that
are being discussed. That's comparable to wood, 0.059.

This page even lists PVC in the "Lossy" group as defined by Tanδ ≥
0.01.


The losses in ferrite rods are nothing to sneeze at in comparison. I
have used both in ham radio a lot when I was young. I built kilowatt
level RF power amps, impedance matching boxes and similar gear.
Ferrite
rods in transmitters sometimes became so hot that you could barely
touch
them while inductors wound on some random piece of PVC pipe remained
cool. I don't remember the PVC type other than that it was remnants
they
sold for pennies in the plumbing department so that was very likely
well
plasticized.

Maybe I don't recall the context of the ferrite, but the receiving
antennas in much of this thread and described in detail at Kleijer's
web
site showed measurable losses with better plastics than PVC. Even
cardboard was a poor support relatively speaking. Seems he would
use a
foam type plastic to get some rigidity with a minimum of loss. Foam
PVC
was not bad, but his Q measurements increased significantly with foam
polypropylene. Obviously foam is better because there is less actual
material. Solid PVC would show more pronounced losses.

He does some amazingly detailed work. You might find it interesting.
The LC experiments were reported in a series of web pages. Page 10
doesn't have a link to page 11, but otherwise they are all chained.


Looks like there isn't a page 11.

That's what I was saying. There *is* a page 11, page 10 just doesn't
have a link to it. Go back to the index.


Indeed. I change the number in the URL by hand by starting with page 11
he change the URL structure. Well, I am not complaining, my web site
design skills aren't that great either.


http://www.crystal-radio.eu/enlctest.htm


He gets good Q with PVC. Worse with cardboard but who knows what
kind of
stuff he used. It looks like carton material. That is often
post-consumer recycled and you never know what's in it. Water
content is
another factor, got to bake it out and then lacquer it immediately
afterwards.

He gets good Q with FOAM PVC. Totally different from solid PVC, much
less of it and a lot more air. The point is foam anything else worked
even better.


Look at page 7. Very nice Q values except for the dirty pipe yet this is
all on regular PVC pipe.

Compared to what? He is comparing coil winding methods. What would the
Q be with other supports?


The Q is over 500. It was claimed in this thread that PVC is not
suitable as coil winding material and this proves that it is quite
suitable. Which I already knew because I've used it in RF power amps
decades ago.

Again, context. You are living in a different world. PVC is *not*
suitable in the crystal radio world because there are *much* better
materials. If PVC was the only material available it would be a *great*
coil support. If mud was the only material available it would be a
*great* coil support.


The huge jump in Q in part 3 shows that he used the wrong measurement
setup until then. You can't do this sort of stuff with a 100:1 scope
probe, it has to be at least a high-end FET probe. However, hat
off, he
achieved amazing Q values in his experiments.

Look at the Q values he gets in part 7. Those are all regular plumbing
PVC pipes. L16 has lower Q but that PVC tube isn't even particularly
clean. It is important to keep or make them pristine when building
high-Q stuff.


I found it very illuminating his tests with the variable capacitors.
Even parts like bushings were found to make a difference.


I remember that from my ham radio days. Dirty or oxidized rotor
contacts
.... phssssst ... PHUT ... *BANG* and worst case that could take the
tubes into the abyss along with it. I also spent part of a Wenol
polishing paste tube keeping the final Pi-filter inductor shiny so it
wouldn't heat up too badly and unsolder a connection to it (which
could
also result in a loud bang).

BTW, while such high Q isn't all that useful in practice if you ever
needed that there are simpler means to achieve it. An old method is
the
"Q-multiplier". In essence the resonance circuit sits inside an
amplifier stage that is deliberately pulled very close to oscillation.
That shrinks the bandwidth big time.

How do you accomplish that without an amplifier? You did notice the
site is all about *crystal* radios, right?


You need an amplifier for that. If you want to you can make an
energy-harvesting one, sans battery. I mentioned this method purely as a
hint, in case anyone ever needs high Q without making fancy large coils
and babying them.

What energy will be harvested?


The energy present in the environment, for example energy from the local
radio transmitters. You can then use that to demodulate the signals of
others.

http://mwrf.com/systems/harvesting-energy-rf-sources

I understand the concept, I'm asking specifically. Have you built
anything like this?

--

Rick C
 
On 2017-03-27 07:59, rickman wrote:
On 3/27/2017 10:46 AM, Joerg wrote:
On 2017-03-26 10:15, rickman wrote:
On 3/26/2017 10:35 AM, Joerg wrote:
On 2017-03-25 18:39, rickman wrote:
On 3/25/2017 3:30 PM, Joerg wrote:
On 2017-03-25 10:49, rickman wrote:
On 3/24/2017 4:36 PM, Joerg wrote:
On 2017-03-24 10:59, rickman wrote:
On 3/24/2017 1:14 PM, Joerg wrote:
On 2017-03-20 02:06, Tauno Voipio wrote:

[...]

Please do not use PVC as RF insulation or support pieces.
It is lossy to extremely lossy at RF.


Plasticized PVC ain't stellar but not horrid.

http://g3ynh.info/zdocs/comps/part_6.html

Or do they add a lot of vispipuuro into the mix in Finland? :)

Are you reading the same page? It says PVC Tanδ is 0.04 - 0.14
at 1
MHz. That is in no way acceptable for the sort of high Q circuits
that
are being discussed. That's comparable to wood, 0.059.

This page even lists PVC in the "Lossy" group as defined by Tanδ ≥
0.01.


The losses in ferrite rods are nothing to sneeze at in
comparison. I
have used both in ham radio a lot when I was young. I built
kilowatt
level RF power amps, impedance matching boxes and similar gear.
Ferrite
rods in transmitters sometimes became so hot that you could barely
touch
them while inductors wound on some random piece of PVC pipe
remained
cool. I don't remember the PVC type other than that it was remnants
they
sold for pennies in the plumbing department so that was very likely
well
plasticized.

Maybe I don't recall the context of the ferrite, but the receiving
antennas in much of this thread and described in detail at Kleijer's
web
site showed measurable losses with better plastics than PVC. Even
cardboard was a poor support relatively speaking. Seems he would
use a
foam type plastic to get some rigidity with a minimum of loss. Foam
PVC
was not bad, but his Q measurements increased significantly with
foam
polypropylene. Obviously foam is better because there is less
actual
material. Solid PVC would show more pronounced losses.

He does some amazingly detailed work. You might find it
interesting.
The LC experiments were reported in a series of web pages. Page 10
doesn't have a link to page 11, but otherwise they are all chained.


Looks like there isn't a page 11.

That's what I was saying. There *is* a page 11, page 10 just doesn't
have a link to it. Go back to the index.


Indeed. I change the number in the URL by hand by starting with page 11
he change the URL structure. Well, I am not complaining, my web site
design skills aren't that great either.


http://www.crystal-radio.eu/enlctest.htm


He gets good Q with PVC. Worse with cardboard but who knows what
kind of
stuff he used. It looks like carton material. That is often
post-consumer recycled and you never know what's in it. Water
content is
another factor, got to bake it out and then lacquer it immediately
afterwards.

He gets good Q with FOAM PVC. Totally different from solid PVC, much
less of it and a lot more air. The point is foam anything else worked
even better.


Look at page 7. Very nice Q values except for the dirty pipe yet
this is
all on regular PVC pipe.

Compared to what? He is comparing coil winding methods. What would the
Q be with other supports?


The Q is over 500. It was claimed in this thread that PVC is not
suitable as coil winding material and this proves that it is quite
suitable. Which I already knew because I've used it in RF power amps
decades ago.

Again, context. You are living in a different world. PVC is *not*
suitable in the crystal radio world because there are *much* better
materials. If PVC was the only material available it would be a *great*
coil support. If mud was the only material available it would be a
*great* coil support.

Can you explain why one even want a Q in excess of 500 in the AM band?

The huge jump in Q in part 3 shows that he used the wrong measurement
setup until then. You can't do this sort of stuff with a 100:1 scope
probe, it has to be at least a high-end FET probe. However, hat
off, he
achieved amazing Q values in his experiments.

Look at the Q values he gets in part 7. Those are all regular
plumbing
PVC pipes. L16 has lower Q but that PVC tube isn't even particularly
clean. It is important to keep or make them pristine when building
high-Q stuff.


I found it very illuminating his tests with the variable capacitors.
Even parts like bushings were found to make a difference.


I remember that from my ham radio days. Dirty or oxidized rotor
contacts
.... phssssst ... PHUT ... *BANG* and worst case that could take the
tubes into the abyss along with it. I also spent part of a Wenol
polishing paste tube keeping the final Pi-filter inductor shiny so it
wouldn't heat up too badly and unsolder a connection to it (which
could
also result in a loud bang).

BTW, while such high Q isn't all that useful in practice if you ever
needed that there are simpler means to achieve it. An old method is
the
"Q-multiplier". In essence the resonance circuit sits inside an
amplifier stage that is deliberately pulled very close to
oscillation.
That shrinks the bandwidth big time.

How do you accomplish that without an amplifier? You did notice the
site is all about *crystal* radios, right?


You need an amplifier for that. If you want to you can make an
energy-harvesting one, sans battery. I mentioned this method purely
as a
hint, in case anyone ever needs high Q without making fancy large coils
and babying them.

What energy will be harvested?


The energy present in the environment, for example energy from the local
radio transmitters. You can then use that to demodulate the signals of
others.

http://mwrf.com/systems/harvesting-energy-rf-sources

I understand the concept, I'm asking specifically. Have you built
anything like this?

Yes, similar but not at liberty to reveal details as this was paid
client work.

--
Regards, Joerg

http://www.analogconsultants.com/
 
On 27.3.17 15:25, amdx wrote:

The question of best MF band coils has been solved already in the
1930's: A honeycomb coil wound with Litz wire (gloves on). The
canonical fixing / insulating material is beeswax.

I don't know have you tried a 6" polystyrene tube with 0.0625 wall
thickness, wound with 660/46 litz wire with 12 turns per inch?

The point with a multilayer coil is better magnetic
coupling between the turns. Honeycomb winding keeps
distributed capacitances better controlled.

--

-TV
 
On 3/27/2017 7:25 AM, amdx wrote:
On 3/27/2017 6:57 AM, Tauno Voipio wrote:
On 26.3.17 17:35, Joerg wrote:
On 2017-03-25 18:39, rickman wrote:
On 3/25/2017 3:30 PM, Joerg wrote:
On 2017-03-25 10:49, rickman wrote:
On 3/24/2017 4:36 PM, Joerg wrote:
On 2017-03-24 10:59, rickman wrote:
On 3/24/2017 1:14 PM, Joerg wrote:
On 2017-03-20 02:06, Tauno Voipio wrote:

[...]

Please do not use PVC as RF insulation or support pieces.
It is lossy to extremely lossy at RF.


Plasticized PVC ain't stellar but not horrid.

http://g3ynh.info/zdocs/comps/part_6.html

Or do they add a lot of vispipuuro into the mix in Finland? :)

Are you reading the same page? It says PVC Tanδ is 0.04 - 0.14
at 1
MHz. That is in no way acceptable for the sort of high Q circuits
that
are being discussed. That's comparable to wood, 0.059.

This page even lists PVC in the "Lossy" group as defined by Tanδ ≥
0.01.


The losses in ferrite rods are nothing to sneeze at in comparison. I
have used both in ham radio a lot when I was young. I built kilowatt
level RF power amps, impedance matching boxes and similar gear.
Ferrite
rods in transmitters sometimes became so hot that you could barely
touch
them while inductors wound on some random piece of PVC pipe remained
cool. I don't remember the PVC type other than that it was remnants
they
sold for pennies in the plumbing department so that was very likely
well
plasticized.

Maybe I don't recall the context of the ferrite, but the receiving
antennas in much of this thread and described in detail at Kleijer's
web
site showed measurable losses with better plastics than PVC. Even
cardboard was a poor support relatively speaking. Seems he would
use a
foam type plastic to get some rigidity with a minimum of loss. Foam
PVC
was not bad, but his Q measurements increased significantly with foam
polypropylene. Obviously foam is better because there is less actual
material. Solid PVC would show more pronounced losses.

He does some amazingly detailed work. You might find it interesting.
The LC experiments were reported in a series of web pages. Page 10
doesn't have a link to page 11, but otherwise they are all chained.


Looks like there isn't a page 11.

That's what I was saying. There *is* a page 11, page 10 just doesn't
have a link to it. Go back to the index.


Indeed. I change the number in the URL by hand by starting with page 11
he change the URL structure. Well, I am not complaining, my web site
design skills aren't that great either.


http://www.crystal-radio.eu/enlctest.htm


He gets good Q with PVC. Worse with cardboard but who knows what
kind of
stuff he used. It looks like carton material. That is often
post-consumer recycled and you never know what's in it. Water
content is
another factor, got to bake it out and then lacquer it immediately
afterwards.

He gets good Q with FOAM PVC. Totally different from solid PVC, much
less of it and a lot more air. The point is foam anything else worked
even better.


Look at page 7. Very nice Q values except for the dirty pipe yet this is
all on regular PVC pipe.


The huge jump in Q in part 3 shows that he used the wrong measurement
setup until then. You can't do this sort of stuff with a 100:1 scope
probe, it has to be at least a high-end FET probe. However, hat
off, he
achieved amazing Q values in his experiments.

Look at the Q values he gets in part 7. Those are all regular plumbing
PVC pipes. L16 has lower Q but that PVC tube isn't even particularly
clean. It is important to keep or make them pristine when building
high-Q stuff.


I found it very illuminating his tests with the variable capacitors.
Even parts like bushings were found to make a difference.


I remember that from my ham radio days. Dirty or oxidized rotor
contacts
.... phssssst ... PHUT ... *BANG* and worst case that could take the
tubes into the abyss along with it. I also spent part of a Wenol
polishing paste tube keeping the final Pi-filter inductor shiny so it
wouldn't heat up too badly and unsolder a connection to it (which
could
also result in a loud bang).

BTW, while such high Q isn't all that useful in practice if you ever
needed that there are simpler means to achieve it. An old method is
the
"Q-multiplier". In essence the resonance circuit sits inside an
amplifier stage that is deliberately pulled very close to oscillation.
That shrinks the bandwidth big time.

How do you accomplish that without an amplifier? You did notice the
site is all about *crystal* radios, right?


You need an amplifier for that. If you want to you can make an
energy-harvesting one, sans battery. I mentioned this method purely as a
hint, in case anyone ever needs high Q without making fancy large coils
and babying them.


Joerg, you seem not understand the innermost sense of the crystal-
radio people. They are closely related to audiophools, and it is
quite impossible to use sensible technical argumentation here.

I don't get that at all, can you back that up with any facts?


The question of best MF band coils has been solved already in the
1930's: A honeycomb coil wound with Litz wire (gloves on). The
canonical fixing / insulating material is beeswax.

I don't know have you tried a 6" polystyrene tube with 0.0625 wall
thickness, wound with 660/46 litz wire with 12 turns per inch?

If anyone has an interest, here's a pdf of multiple honeycomb coils and
data. I think it is from the 30's or 40's. I can't seem to get
it to download properly. But what I could see doesn't give Q directly,
so needs to be calculated.
http://nvlpubs.nist.gov/nistpubs/nbstechnologic/nbstechnologicpapert298.pdf


Mikek
Anyone get that pdf to load properly, the graphs I want see are only
half there, left side or right side.
Mikek
 
Den tirsdag den 28. marts 2017 kl. 01.25.23 UTC+2 skrev Jim Thompson:
On Sun, 26 Mar 2017 15:36:06 +1100, Sylvia Else
sylvia@not.at.this.address> wrote:

I'm using this circuit to provide 250V pulses to an ignition coil.

https://www.dropbox.com/s/1w33uss3eedem05/ignition2.pdf?dl=0

The IC is a Linear Technology LT1243.

12V is provided on G$1 to the left. G$2 accepts a trigger pulse, and G$3
is ground.

LTSpice says that this works, and indeed the real implementation does.
Mostly.

The difference is that after the circuit has been triggered once, it
won't charge the capacitor again (above about 25 volts) for a varying
period that can be up to half a minute. It's as if the wrong level is
being used internally to compare with the feedback pin. In that regard,
I'll mention that Q3 is used to pull FB up so that the circuit stops
driving the FET, since otherwise the SCR never turns off. I've checked,
and the problem is not that Q3 remains on, nor is it that the SCR fails
to turn off. In any case, the 1.5uF capacitor C1 does get charged
somewhat, as I mentioned above.

When the issue resolves, it does so rapidly, within a fraction of a second.

Connecting an oscilloscope probe to the RT/CT pin of the IC restores
function, but only if the scope is set to DC coupling - not AC coupling
- and functioning continues only as long as the probe remains connected
- until the aforesaid varying period has elapsed. Touching the pin with
a finger has a similar effect.

That is, connect probe; works. Disconnect; stops working. Reconnect;
works, etc. until eventually it starts working continuously.

This cannot be capacitive loading - there's already a significant
capacitance between RT/CT and ground.

The fact that the coupling has to be DC made me think that some small
current was flowing to ground through the scope, so I bridged C4 with a
100K resistor. It didn't make any difference.

I tried changing the IC (a pain, given that it's surface mounted), but
again it made no difference.

Any other ideas about what might be happening here.

Sylvia.

Using a PIC when you should have gone analog >:-}

http://www.analog-innovations.com/SED/CD-Ignition-Basic.pdf

http://www.analog-innovations.com/SED/CDI_Inductor.jpg

why even bother with CDI? most car do fine with regular coils, many coils even have the driver igbt buildin all you need is a 5V driver for a few ms of
dwell time
 
On 3/27/2017 1:21 PM, amdx wrote:
On 3/27/2017 7:25 AM, amdx wrote:
On 3/27/2017 6:57 AM, Tauno Voipio wrote:
On 26.3.17 17:35, Joerg wrote:
On 2017-03-25 18:39, rickman wrote:
On 3/25/2017 3:30 PM, Joerg wrote:
On 2017-03-25 10:49, rickman wrote:
On 3/24/2017 4:36 PM, Joerg wrote:
On 2017-03-24 10:59, rickman wrote:
On 3/24/2017 1:14 PM, Joerg wrote:
On 2017-03-20 02:06, Tauno Voipio wrote:

[...]

Please do not use PVC as RF insulation or support pieces.
It is lossy to extremely lossy at RF.


Plasticized PVC ain't stellar but not horrid.

http://g3ynh.info/zdocs/comps/part_6.html

Or do they add a lot of vispipuuro into the mix in Finland? :)

Are you reading the same page? It says PVC Tanδ is 0.04 - 0.14
at 1
MHz. That is in no way acceptable for the sort of high Q circuits
that
are being discussed. That's comparable to wood, 0.059.

This page even lists PVC in the "Lossy" group as defined by Tanδ ≥
0.01.


The losses in ferrite rods are nothing to sneeze at in
comparison. I
have used both in ham radio a lot when I was young. I built
kilowatt
level RF power amps, impedance matching boxes and similar gear.
Ferrite
rods in transmitters sometimes became so hot that you could barely
touch
them while inductors wound on some random piece of PVC pipe
remained
cool. I don't remember the PVC type other than that it was remnants
they
sold for pennies in the plumbing department so that was very likely
well
plasticized.

Maybe I don't recall the context of the ferrite, but the receiving
antennas in much of this thread and described in detail at Kleijer's
web
site showed measurable losses with better plastics than PVC. Even
cardboard was a poor support relatively speaking. Seems he would
use a
foam type plastic to get some rigidity with a minimum of loss. Foam
PVC
was not bad, but his Q measurements increased significantly with
foam
polypropylene. Obviously foam is better because there is less
actual
material. Solid PVC would show more pronounced losses.

He does some amazingly detailed work. You might find it
interesting.
The LC experiments were reported in a series of web pages. Page 10
doesn't have a link to page 11, but otherwise they are all chained.


Looks like there isn't a page 11.

That's what I was saying. There *is* a page 11, page 10 just doesn't
have a link to it. Go back to the index.


Indeed. I change the number in the URL by hand by starting with page 11
he change the URL structure. Well, I am not complaining, my web site
design skills aren't that great either.


http://www.crystal-radio.eu/enlctest.htm


He gets good Q with PVC. Worse with cardboard but who knows what
kind of
stuff he used. It looks like carton material. That is often
post-consumer recycled and you never know what's in it. Water
content is
another factor, got to bake it out and then lacquer it immediately
afterwards.

He gets good Q with FOAM PVC. Totally different from solid PVC, much
less of it and a lot more air. The point is foam anything else worked
even better.


Look at page 7. Very nice Q values except for the dirty pipe yet
this is
all on regular PVC pipe.


The huge jump in Q in part 3 shows that he used the wrong measurement
setup until then. You can't do this sort of stuff with a 100:1 scope
probe, it has to be at least a high-end FET probe. However, hat
off, he
achieved amazing Q values in his experiments.

Look at the Q values he gets in part 7. Those are all regular
plumbing
PVC pipes. L16 has lower Q but that PVC tube isn't even particularly
clean. It is important to keep or make them pristine when building
high-Q stuff.


I found it very illuminating his tests with the variable capacitors.
Even parts like bushings were found to make a difference.


I remember that from my ham radio days. Dirty or oxidized rotor
contacts
.... phssssst ... PHUT ... *BANG* and worst case that could take the
tubes into the abyss along with it. I also spent part of a Wenol
polishing paste tube keeping the final Pi-filter inductor shiny so it
wouldn't heat up too badly and unsolder a connection to it (which
could
also result in a loud bang).

BTW, while such high Q isn't all that useful in practice if you ever
needed that there are simpler means to achieve it. An old method is
the
"Q-multiplier". In essence the resonance circuit sits inside an
amplifier stage that is deliberately pulled very close to
oscillation.
That shrinks the bandwidth big time.

How do you accomplish that without an amplifier? You did notice the
site is all about *crystal* radios, right?


You need an amplifier for that. If you want to you can make an
energy-harvesting one, sans battery. I mentioned this method purely
as a
hint, in case anyone ever needs high Q without making fancy large coils
and babying them.


Joerg, you seem not understand the innermost sense of the crystal-
radio people. They are closely related to audiophools, and it is
quite impossible to use sensible technical argumentation here.

I don't get that at all, can you back that up with any facts?


The question of best MF band coils has been solved already in the
1930's: A honeycomb coil wound with Litz wire (gloves on). The
canonical fixing / insulating material is beeswax.

I don't know have you tried a 6" polystyrene tube with 0.0625 wall
thickness, wound with 660/46 litz wire with 12 turns per inch?

If anyone has an interest, here's a pdf of multiple honeycomb coils and
data. I think it is from the 30's or 40's. I can't seem to get
it to download properly. But what I could see doesn't give Q directly,
so needs to be calculated.
http://nvlpubs.nist.gov/nistpubs/nbstechnologic/nbstechnologicpapert298.pdf



Mikek

Anyone get that pdf to load properly, the graphs I want see are only
half there, left side or right side.

If you are talking about the graph on page 10, that isn't loading
correctly for me either. But it appears to be the same graph on page
12. Likewise the bad image on page 14 is the same as the image on page
16, etc. Even in a PDF viewer not in the browser the pages render
*very* slowly. Even just scrolling back a couple of pages makes it
start all over again. Very hard to view. I think this document needs
to be recovered by re-imaging it and turning it into a new PDF file.

--

Rick C
 
On 27/03/17 23:25, amdx wrote:
On 3/27/2017 6:57 AM, Tauno Voipio wrote:
Joerg, you seem not understand the innermost sense of the crystal-
radio people. They are closely related to audiophools, and it is
quite impossible to use sensible technical argumentation here.

I don't get that at all, can you back that up with any facts?

~1MHz, Q=500, bandwidth ~ 2KHz. Remind me why you need Q>1500?
More voltage does not create better audio.
 
On Sun, 26 Mar 2017 15:36:06 +1100, Sylvia Else
<sylvia@not.at.this.address> wrote:

I'm using this circuit to provide 250V pulses to an ignition coil.

https://www.dropbox.com/s/1w33uss3eedem05/ignition2.pdf?dl=0

The IC is a Linear Technology LT1243.

12V is provided on G$1 to the left. G$2 accepts a trigger pulse, and G$3
is ground.

LTSpice says that this works, and indeed the real implementation does.
Mostly.

The difference is that after the circuit has been triggered once, it
won't charge the capacitor again (above about 25 volts) for a varying
period that can be up to half a minute. It's as if the wrong level is
being used internally to compare with the feedback pin. In that regard,
I'll mention that Q3 is used to pull FB up so that the circuit stops
driving the FET, since otherwise the SCR never turns off. I've checked,
and the problem is not that Q3 remains on, nor is it that the SCR fails
to turn off. In any case, the 1.5uF capacitor C1 does get charged
somewhat, as I mentioned above.

When the issue resolves, it does so rapidly, within a fraction of a second.

Connecting an oscilloscope probe to the RT/CT pin of the IC restores
function, but only if the scope is set to DC coupling - not AC coupling
- and functioning continues only as long as the probe remains connected
- until the aforesaid varying period has elapsed. Touching the pin with
a finger has a similar effect.

That is, connect probe; works. Disconnect; stops working. Reconnect;
works, etc. until eventually it starts working continuously.

This cannot be capacitive loading - there's already a significant
capacitance between RT/CT and ground.

The fact that the coupling has to be DC made me think that some small
current was flowing to ground through the scope, so I bridged C4 with a
100K resistor. It didn't make any difference.

I tried changing the IC (a pain, given that it's surface mounted), but
again it made no difference.

Any other ideas about what might be happening here.

Sylvia.

Using a PIC when you should have gone analog >:-}

<http://www.analog-innovations.com/SED/CD-Ignition-Basic.pdf>

<http://www.analog-innovations.com/SED/CDI_Inductor.jpg>

...Jim Thompson
--
| James E.Thompson | mens |
| Analog Innovations | et |
| Analog/Mixed-Signal ASIC's and Discrete Systems | manus |
| STV, Queen Creek, AZ 85142 Skype: skypeanalog | |
| Voice:(480)460-2350 Fax: Available upon request | Brass Rat |
| E-mail Icon at http://www.analog-innovations.com | 1962 |

Thinking outside the box... producing elegant solutions.
 
On Mon, 27 Mar 2017 16:31:19 -0700 (PDT), Lasse Langwadt Christensen
<langwadt@fonz.dk> wrote:

Den tirsdag den 28. marts 2017 kl. 01.25.23 UTC+2 skrev Jim Thompson:
On Sun, 26 Mar 2017 15:36:06 +1100, Sylvia Else
sylvia@not.at.this.address> wrote:

I'm using this circuit to provide 250V pulses to an ignition coil.

https://www.dropbox.com/s/1w33uss3eedem05/ignition2.pdf?dl=0

The IC is a Linear Technology LT1243.

12V is provided on G$1 to the left. G$2 accepts a trigger pulse, and G$3
is ground.

LTSpice says that this works, and indeed the real implementation does.
Mostly.

The difference is that after the circuit has been triggered once, it
won't charge the capacitor again (above about 25 volts) for a varying
period that can be up to half a minute. It's as if the wrong level is
being used internally to compare with the feedback pin. In that regard,
I'll mention that Q3 is used to pull FB up so that the circuit stops
driving the FET, since otherwise the SCR never turns off. I've checked,
and the problem is not that Q3 remains on, nor is it that the SCR fails
to turn off. In any case, the 1.5uF capacitor C1 does get charged
somewhat, as I mentioned above.

When the issue resolves, it does so rapidly, within a fraction of a second.

Connecting an oscilloscope probe to the RT/CT pin of the IC restores
function, but only if the scope is set to DC coupling - not AC coupling
- and functioning continues only as long as the probe remains connected
- until the aforesaid varying period has elapsed. Touching the pin with
a finger has a similar effect.

That is, connect probe; works. Disconnect; stops working. Reconnect;
works, etc. until eventually it starts working continuously.

This cannot be capacitive loading - there's already a significant
capacitance between RT/CT and ground.

The fact that the coupling has to be DC made me think that some small
current was flowing to ground through the scope, so I bridged C4 with a
100K resistor. It didn't make any difference.

I tried changing the IC (a pain, given that it's surface mounted), but
again it made no difference.

Any other ideas about what might be happening here.

Sylvia.

Using a PIC when you should have gone analog >:-}

http://www.analog-innovations.com/SED/CD-Ignition-Basic.pdf

http://www.analog-innovations.com/SED/CDI_Inductor.jpg

why even bother with CDI? most car do fine with regular coils, many coils even have the driver igbt buildin all you need is a 5V driver for a few ms of
dwell time

But can it saw Plexiglas ?>:-}

...Jim Thompson
--
| James E.Thompson | mens |
| Analog Innovations | et |
| Analog/Mixed-Signal ASIC's and Discrete Systems | manus |
| STV, Queen Creek, AZ 85142 Skype: skypeanalog | |
| Voice:(480)460-2350 Fax: Available upon request | Brass Rat |
| E-mail Icon at http://www.analog-innovations.com | 1962 |

Thinking outside the box... producing elegant solutions.
 
On 2017-03-27 16:16, Clifford Heath wrote:
On 27/03/17 23:25, amdx wrote:
On 3/27/2017 6:57 AM, Tauno Voipio wrote:
Joerg, you seem not understand the innermost sense of the crystal-
radio people. They are closely related to audiophools, and it is
quite impossible to use sensible technical argumentation here.

I don't get that at all, can you back that up with any facts?

~1MHz, Q=500, bandwidth ~ 2KHz. Remind me why you need Q>1500?
More voltage does not create better audio.

That's what I was wondering all the time. In the ranges tested there are
largely just AM stations, no CW or morse code. Even at 10kHz BW the
audio experience will not be very pleasing, it'll sound more like on a
telephone.

Then there is the tempco. Someone opens a window and whoops the resonant
frequency goes somewhere else.

However, the crystal radio guys I've met were more down-to-earth and
unlike audiophools did not spend $199.98 for a few feet of gold-plated
cable with individual electron spin control and all that.

--
Regards, Joerg

http://www.analogconsultants.com/
 
On 28/03/2017 1:16 AM, dagmargoodboat@yahoo.com wrote:
On Sunday, March 26, 2017 at 2:33:13 AM UTC-4, Sylvia Else wrote:

Finally got the engine running today, using this ignition circuit, and
LPG, after many hours spent cursing a PIC32MX that I was temporarily
using to generate the trigger pulse - got caught out by yet another PIC
errata - input capture doesn't work when the processor is in the idle state.

Sylvia.

Was that PIC quirk the problem? Otherwise, I'd ask
o Whether C4 might be bad, open, or the wrong value?

No, and I even replaced it. Its value is far from critical anyway.
Or, that not being the case, maybe the LT1243's upset about having its
FB pin pulled all the way to +5v (wind-up?)?

It's within spec. Another possibility is that the LT1243 is interpreting
the sudden drop in FB as an indicator of an output short, but if so, I'd
expect it to object to every such occurrence, not just the first.

Is the LT1243's Vref getting glitched from your reset circuit, upsetting
the LT?

Just some wild ideas. From your description it really sounds like it's
RT/CT pin-related, and you've already put your finger on it (so to speak :).

The IC is not really designed with this application in mind. Perhaps it
just plain doesn't like being used this way.

Sylvia.
 
On 28/03/2017 10:25 AM, Jim Thompson wrote:
On Sun, 26 Mar 2017 15:36:06 +1100, Sylvia Else
sylvia@not.at.this.address> wrote:

I'm using this circuit to provide 250V pulses to an ignition coil.

https://www.dropbox.com/s/1w33uss3eedem05/ignition2.pdf?dl=0

The IC is a Linear Technology LT1243.

12V is provided on G$1 to the left. G$2 accepts a trigger pulse,
and G$3 is ground.

LTSpice says that this works, and indeed the real implementation
does. Mostly.

The difference is that after the circuit has been triggered once,
it won't charge the capacitor again (above about 25 volts) for a
varying period that can be up to half a minute. It's as if the
wrong level is being used internally to compare with the feedback
pin. In that regard, I'll mention that Q3 is used to pull FB up so
that the circuit stops driving the FET, since otherwise the SCR
never turns off. I've checked, and the problem is not that Q3
remains on, nor is it that the SCR fails to turn off. In any case,
the 1.5uF capacitor C1 does get charged somewhat, as I mentioned
above.

When the issue resolves, it does so rapidly, within a fraction of a
second.

Connecting an oscilloscope probe to the RT/CT pin of the IC
restores function, but only if the scope is set to DC coupling -
not AC coupling - and functioning continues only as long as the
probe remains connected - until the aforesaid varying period has
elapsed. Touching the pin with a finger has a similar effect.

That is, connect probe; works. Disconnect; stops working.
Reconnect; works, etc. until eventually it starts working
continuously.

This cannot be capacitive loading - there's already a significant
capacitance between RT/CT and ground.

The fact that the coupling has to be DC made me think that some
small current was flowing to ground through the scope, so I bridged
C4 with a 100K resistor. It didn't make any difference.

I tried changing the IC (a pain, given that it's surface mounted),
but again it made no difference.

Any other ideas about what might be happening here.

Sylvia.

Using a PIC when you should have gone analog >:-}

Nah! Used a boost converter chip when I should have used a PIC. A 28 pin
PIC32MX seems a bit over the top for this, but what the hell? It's not
even more expensive.

http://www.analog-innovations.com/SED/CD-Ignition-Basic.pdf

http://www.analog-innovations.com/SED/CDI_Inductor.jpg> ...Jim
Thompson

Don't quite see how that works - does it rely on the reverse breakdown
of D3?

Sylvia.
 
On 28/03/2017 10:31 AM, Lasse Langwadt Christensen wrote:
Den tirsdag den 28. marts 2017 kl. 01.25.23 UTC+2 skrev Jim
Thompson:
On Sun, 26 Mar 2017 15:36:06 +1100, Sylvia Else
sylvia@not.at.this.address> wrote:

I'm using this circuit to provide 250V pulses to an ignition
coil.

https://www.dropbox.com/s/1w33uss3eedem05/ignition2.pdf?dl=0

The IC is a Linear Technology LT1243.

12V is provided on G$1 to the left. G$2 accepts a trigger pulse,
and G$3 is ground.

LTSpice says that this works, and indeed the real implementation
does. Mostly.

The difference is that after the circuit has been triggered once,
it won't charge the capacitor again (above about 25 volts) for a
varying period that can be up to half a minute. It's as if the
wrong level is being used internally to compare with the feedback
pin. In that regard, I'll mention that Q3 is used to pull FB up
so that the circuit stops driving the FET, since otherwise the
SCR never turns off. I've checked, and the problem is not that Q3
remains on, nor is it that the SCR fails to turn off. In any
case, the 1.5uF capacitor C1 does get charged somewhat, as I
mentioned above.

When the issue resolves, it does so rapidly, within a fraction of
a second.

Connecting an oscilloscope probe to the RT/CT pin of the IC
restores function, but only if the scope is set to DC coupling -
not AC coupling - and functioning continues only as long as the
probe remains connected - until the aforesaid varying period has
elapsed. Touching the pin with a finger has a similar effect.

That is, connect probe; works. Disconnect; stops working.
Reconnect; works, etc. until eventually it starts working
continuously.

This cannot be capacitive loading - there's already a
significant capacitance between RT/CT and ground.

The fact that the coupling has to be DC made me think that some
small current was flowing to ground through the scope, so I
bridged C4 with a 100K resistor. It didn't make any difference.

I tried changing the IC (a pain, given that it's surface
mounted), but again it made no difference.

Any other ideas about what might be happening here.

Sylvia.

Using a PIC when you should have gone analog >:-}

http://www.analog-innovations.com/SED/CD-Ignition-Basic.pdf

http://www.analog-innovations.com/SED/CDI_Inductor.jpg

why even bother with CDI? most car do fine with regular coils, many
coils even have the driver igbt buildin all you need is a 5V driver
for a few ms of dwell time

My application is a backup "portable" generator. One useful feature of
CDI in this application is that it doesn't require a large input
current, meaning that I can start the generator using cheap dry cells,
and then let it power itself. No need for limited life failure prone
rechargeable batteries that need to be kept topped up lest they die.

Sylvia.
 
On 3/27/2017 12:22 PM, Joerg wrote:
On 2017-03-27 07:59, rickman wrote:
On 3/27/2017 10:46 AM, Joerg wrote:

The Q is over 500. It was claimed in this thread that PVC is not
suitable as coil winding material and this proves that it is quite
suitable. Which I already knew because I've used it in RF power amps
decades ago.

Again, context. You are living in a different world. PVC is *not*
suitable in the crystal radio world because there are *much* better
materials. If PVC was the only material available it would be a *great*
coil support. If mud was the only material available it would be a
*great* coil support.


Can you explain why one even want a Q in excess of 500 in the AM band?

Q is a measure of the losses. Having a high Q in the coil means the
coil has lower losses. Having a higher Q in the tuning capacitor means
it has lower losses. The lower the losses the more power that ends up
in the headphones.

The Q of the radio won't be the same as the Q of the components because
you are sucking off power to drive the headphones. Besides, the number
you came up with (10 kHz) would be perfect for AM radio if you can get
that, that is the channel spacing. Great selectivity.

--

Rick C
 

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