Help with high input impedance amp....

  • Thread starter Lamont Cranston
  • Start date
On 2022-11-06 22:48, Lamont Cranston wrote:
On Sunday, November 6, 2022 at 2:59:07 PM UTC-6, Leo Baumann wrote:
Am 06.11.2022 um 21:54 schrieb Lamont Cranston:
Because there is no data on the BF256C, and this fellow says there is a 17 x attenuation,
that would make it 5.1pf of gate capacitance.
The gate-capacitance of a sFET BF256C is about 0.8 pF.

Do you have a reference for that?

I get 15.4 attenuation ratio, input to the source of the fet @1MHz.
https://www.dropbox.com/s/5oud5mbdu45o73i/Kleijer%27s%20input%20circuit.jpg?dl=0
The fet source goes to a 100nF cap and about 500Ω to ground.
Mikek

I see no reason why this wouldn\'t work, if constructed correctly.
It\'s a source follower followed by an emitter follower, so we
expect a gain a little below unity. The gate is biased to 9V
or so, but you shouldn\'t try to measure that directly because
the DC impedance is too high.

The source should be a little above that, 11v maybe, and the NPN
emitter about 0.7V below that. You *can* measure that: The impedance
there is low enough. The drain resistor drops about 11V, same as the
source resistor, so that Vds ends up about 8V, a tad high, but
acceptable. There\'s 200mW dissipated in the NPN, so it will get hot,
probably too hot. Increasing the emitter resistor would help.
Adding a resistor in the collector lead would help too. Bypass the
collector to GND if you do that.

With a 30V overall supply voltage, I\'d probably make it rise gently,
to prevent transients stressing the semiconductors.

The two capacitors going back from the NPN emitter are bootstraps,
the top one reducing the effect of Cgd of the JFET, and the bottom
one increasing the effective impedance of the gate resistor.

I\'d expect the input impedance to be in the 100 MOhm ballpark in
parallel with a fraction of a pF. Any additional capacitive stuff
hanging on the input, tracks, pads, connectors, cables, whatnot,
adds to that, of course.

It should easily reach a -3dB bandwidth of a few tens of MHz,
though of course, beyond a few kHz, the input impedance is
dominated by the input capacitance.

Jeroen Belleman
 
Jeroen Belleman wrote:
------------------------------------
The two capacitors going back from the NPN emitter are bootstraps,
the top one reducing the effect of Cgd of the JFET, and the bottom
one increasing the effective impedance of the gate resistor.

I\'d expect the input impedance to be in the 100 MOhm ballpark in
parallel with a fraction of a pF. Any additional capacitive stuff
hanging on the input, tracks, pads, connectors, cables, whatnot,
adds to that, of course.

It should easily reach a -3dB bandwidth of a few tens of MHz,
though of course, beyond a few kHz, the input impedance is
dominated by the input capacitance.

** Bootstrapping the gate resistor on a JFET might seem like a neat way to get a very high input resistance.

A common application for such is a pre-amp for a condenser mic capsule - which is essentially a charged 50pF capacitor.
Flat response down to below 20Hz means the input resistance needs to be about 500Mohms.
Back in the day I tried the idea out in practice and found a major drawback - noise !
Positive feedback adds lots of it to the boostrapped resistor.
Secondly, compared to using a 500M or 1Gohm resistor, the capacitance of the capsule cannot attenuate noise at the JFET gate near as well. Though thermal noise increases with resistor value, the -6dB / oct attenuation by a parallel capacitor attenuates it more.



...... Phil
 
On 06/11/2022 14:22, Lamont Cranston wrote:
On Sunday, November 6, 2022 at 7:22:24 AM UTC-6, Fred Bloggs wrote:
On Saturday, November 5, 2022 at 8:59:49 PM UTC-4, Lamont Cranston wrote:
Years ago on this group, someone worked this circuit out for me and I have finally built it. It has two problems. The input impedance is about 30kΩ not 500MΩ, and it rolls of way to early.
I may have created the problems, I don\'t have the FET and transistor recommended, 2N4416 and MMBTH10. I used a BF256C and a MPSH10 through hole parts. Although I doubt that created the low input impedance.
https://www.dropbox.com/s/kdwhcxmbk53ugqm/Dagmar%27s%20Fast%20high%20Imp%20amp%20with%20voltage%20labelsand%20RF%20voltages.jpg?dl=0
Anyone care to tell me why such low input impedance and how to make the frequency flat to 30MHz?
Mikek
You have something in the drain of T1 introducing excessive negative feedback on the gate drive. That\'s only way to explain the combination low input impedance and low frequency gain rolloff. If you can\'t do better with your layout, install a high frequency decoupling capacitor at T1 drain to ground there.

I installed a small cap right at the drain to ground, no change.
I\'m posting a picture of the PCB, to learn, not for harassment. :) Tempted to shrink the the picture, but no.
Note: I have changed semi conductors about 6 times.
https://www.dropbox.com/s/w8psnbud9b6z2se/PCB.jpg?dl=0
I have had the A, B, and C dc voltages vary over the various T1, Q2 changes, as I write I get A=2.4, B= 6.5 and C=5.8.
My first dc measurements were A=1.48 B=8.55 and C=7.83. I have also had A=1.0, B= 5.24, and C=4.63. (A is altered by the 10MΩ meter impedance.)
This doesn\'t have much effect on Gain.

You can avoid getting silly numbers for the reading at A by comparing it
with a reference voltage taken off a potentiometer in the classic bridge
fashion. No current flows (= no voltage difference) when Vref = Vtest.

Why do you actually want a very high impedance front end amplifier if
your signal source is 50ohm?

--
Regards,
Martin Brown
 
On Monday, November 7, 2022 at 4:30:30 AM UTC-6, Martin Brown wrote:

Why do you actually want a very high impedance front end amplifier if
your signal source is 50ohm?

--
Regards,
Martin Brown

I just did* the math and it works out. 20MΩ in series with the 10MΩ meter is 30MΩ,
the is in parallel with 2.2MΩ, so 2.081MΩ. So, we have a 10MΩ, 2.081MΩ voltage divider with a 24.91V supply,
has 4.291V at the node. Now we have a 4.291V source feeding a series 20MΩ and 10MΩ meter.
Again a voltage divider with 4.291V source feeding 20MΩ and 10MΩ, that leaves 1.43V at the node.
If I recall correctly, I posted 1.5V and my notes say 1.48V. Close enough.
The 50Ω source is just for testing.
Mikek
*did the math, I use online calculators,
https://www.digikey.com/en/resources/conversion-calculators/conversion-calculator-parallel-and-series-resistor
https://ohmslawcalculator.com/voltage-divider-calculator

 
On Sunday, November 6, 2022 at 5:06:22 PM UTC-6, Jeroen Belleman wrote:
On 2022-11-06 22:48, Lamont Cranston wrote:
On Sunday, November 6, 2022 at 2:59:07 PM UTC-6, Leo Baumann wrote:
Am 06.11.2022 um 21:54 schrieb Lamont Cranston:
Because there is no data on the BF256C, and this fellow says there is a 17 x attenuation,
that would make it 5.1pf of gate capacitance.
The gate-capacitance of a sFET BF256C is about 0.8 pF.

Do you have a reference for that?

I get 15.4 attenuation ratio, input to the source of the fet @1MHz.
https://www.dropbox.com/s/5oud5mbdu45o73i/Kleijer%27s%20input%20circuit..jpg?dl=0
The fet source goes to a 100nF cap and about 500Ω to ground.
Mikek

I see no reason why this wouldn\'t work, if constructed correctly.
It\'s a source follower followed by an emitter follower, so we
expect a gain a little below unity. The gate is biased to 9V
or so, but you shouldn\'t try to measure that directly because
the DC impedance is too high.

The source should be a little above that, 11v maybe, and the NPN
emitter about 0.7V below that. You *can* measure that: The impedance
there is low enough. The drain resistor drops about 11V, same as the
source resistor, so that Vds ends up about 8V, a tad high, but
acceptable. There\'s 200mW dissipated in the NPN, so it will get hot,
probably too hot. Increasing the emitter resistor would help.
Adding a resistor in the collector lead would help too. Bypass the
collector to GND if you do that.

With a 30V overall supply voltage, I\'d probably make it rise gently,
to prevent transients stressing the semiconductors.

The two capacitors going back from the NPN emitter are bootstraps,
the top one reducing the effect of Cgd of the JFET, and the bottom
one increasing the effective impedance of the gate resistor.

I\'d expect the input impedance to be in the 100 MOhm ballpark in
parallel with a fraction of a pF. Any additional capacitive stuff
hanging on the input, tracks, pads, connectors, cables, whatnot,
adds to that, of course.

It should easily reach a -3dB bandwidth of a few tens of MHz,
though of course, beyond a few kHz, the input impedance is
dominated by the input capacitance.

Jeroen Belleman

I\'m assuming the schematic is drawn correctly and the transistor is an NPN.
Can I use aluminum polarized 1uf capacitors? If not, what would I use.
Should both caps have the positive terminal connected to the emitter of the transistor?
Seems kinda close, but what happens when it starts swinging? Maybe I should I have non-polarised 1uF caps.
What kind?
The schematic,
https://www.dropbox.com/s/6n78s84gd9kaouu/High%20impedance%20input%20-%20Copy.jpg?dl=0

Thanks, Mikek
 
On 2022-11-07 18:43, Lamont Cranston wrote:
On Sunday, November 6, 2022 at 5:06:22 PM UTC-6, Jeroen Belleman wrote:
On 2022-11-06 22:48, Lamont Cranston wrote:
On Sunday, November 6, 2022 at 2:59:07 PM UTC-6, Leo Baumann wrote:
Am 06.11.2022 um 21:54 schrieb Lamont Cranston:
Because there is no data on the BF256C, and this fellow says there is a 17 x attenuation,
that would make it 5.1pf of gate capacitance.
The gate-capacitance of a sFET BF256C is about 0.8 pF.

Do you have a reference for that?

I get 15.4 attenuation ratio, input to the source of the fet @1MHz.
https://www.dropbox.com/s/5oud5mbdu45o73i/Kleijer%27s%20input%20circuit.jpg?dl=0
The fet source goes to a 100nF cap and about 500Ω to ground.
Mikek

I see no reason why this wouldn\'t work, if constructed correctly.
It\'s a source follower followed by an emitter follower, so we
expect a gain a little below unity. The gate is biased to 9V
or so, but you shouldn\'t try to measure that directly because
the DC impedance is too high.

The source should be a little above that, 11v maybe, and the NPN
emitter about 0.7V below that. You *can* measure that: The impedance
there is low enough. The drain resistor drops about 11V, same as the
source resistor, so that Vds ends up about 8V, a tad high, but
acceptable. There\'s 200mW dissipated in the NPN, so it will get hot,
probably too hot. Increasing the emitter resistor would help.
Adding a resistor in the collector lead would help too. Bypass the
collector to GND if you do that.

With a 30V overall supply voltage, I\'d probably make it rise gently,
to prevent transients stressing the semiconductors.

The two capacitors going back from the NPN emitter are bootstraps,
the top one reducing the effect of Cgd of the JFET, and the bottom
one increasing the effective impedance of the gate resistor.

I\'d expect the input impedance to be in the 100 MOhm ballpark in
parallel with a fraction of a pF. Any additional capacitive stuff
hanging on the input, tracks, pads, connectors, cables, whatnot,
adds to that, of course.

It should easily reach a -3dB bandwidth of a few tens of MHz,
though of course, beyond a few kHz, the input impedance is
dominated by the input capacitance.

Jeroen Belleman

I\'m assuming the schematic is drawn correctly and the transistor is an NPN.
Can I use aluminum polarized 1uf capacitors? If not, what would I use.
Should both caps have the positive terminal connected to the emitter of the transistor?
Seems kinda close, but what happens when it starts swinging? Maybe I should I have non-polarised 1uF caps.
What kind?
The schematic,
https://www.dropbox.com/s/6n78s84gd9kaouu/High%20impedance%20input%20-%20Copy.jpg?dl=0

Thanks, Mikek

There are no 1uF capacitors in that schematic. They are 0.1uF, but the decimal
dot is all but vanishing. It wouldn\'t make much difference though. Either should
work. If you really want to use polarized capacitors, the NPN emitter has the
lowest DC potential of the three junctions, so the negative terminals of the
caps should be connected there. For AC, the three nodes swing the same way,
near enough, thanks to those two capacitors. That\'s what bootstraps are
*intended* to do.

That said, it\'s about time you Americans drop the silly .1u. Dots *do* vanish.
Use 100n. This schematic breaks the point, if you\'ll excuse me the pun.

The schematic is otherwise correct, it\'s an NPN alright.

Jeroen Belleman
 
On 07/11/2022 5:43 pm, Lamont Cranston wrote:
On Sunday, November 6, 2022 at 5:06:22 PM UTC-6, Jeroen Belleman wrote:
On 2022-11-06 22:48, Lamont Cranston wrote:
On Sunday, November 6, 2022 at 2:59:07 PM UTC-6, Leo Baumann wrote:
Am 06.11.2022 um 21:54 schrieb Lamont Cranston:
Because there is no data on the BF256C, and this fellow says there is a 17 x attenuation,
that would make it 5.1pf of gate capacitance.
The gate-capacitance of a sFET BF256C is about 0.8 pF.

Do you have a reference for that?

I get 15.4 attenuation ratio, input to the source of the fet @1MHz.
https://www.dropbox.com/s/5oud5mbdu45o73i/Kleijer%27s%20input%20circuit.jpg?dl=0
The fet source goes to a 100nF cap and about 500Ω to ground.
Mikek

I see no reason why this wouldn\'t work, if constructed correctly.
It\'s a source follower followed by an emitter follower, so we
expect a gain a little below unity. The gate is biased to 9V
or so, but you shouldn\'t try to measure that directly because
the DC impedance is too high.

The source should be a little above that, 11v maybe, and the NPN
emitter about 0.7V below that. You *can* measure that: The impedance
there is low enough. The drain resistor drops about 11V, same as the
source resistor, so that Vds ends up about 8V, a tad high, but
acceptable. There\'s 200mW dissipated in the NPN, so it will get hot,
probably too hot. Increasing the emitter resistor would help.
Adding a resistor in the collector lead would help too. Bypass the
collector to GND if you do that.

With a 30V overall supply voltage, I\'d probably make it rise gently,
to prevent transients stressing the semiconductors.

The two capacitors going back from the NPN emitter are bootstraps,
the top one reducing the effect of Cgd of the JFET, and the bottom
one increasing the effective impedance of the gate resistor.

I\'d expect the input impedance to be in the 100 MOhm ballpark in
parallel with a fraction of a pF. Any additional capacitive stuff
hanging on the input, tracks, pads, connectors, cables, whatnot,
adds to that, of course.

It should easily reach a -3dB bandwidth of a few tens of MHz,
though of course, beyond a few kHz, the input impedance is
dominated by the input capacitance.

Jeroen Belleman

I\'m assuming the schematic is drawn correctly and the transistor is an NPN.
Can I use aluminum polarized 1uf capacitors? If not, what would I use.
Should both caps have the positive terminal connected to the emitter of the transistor?
Seems kinda close, but what happens when it starts swinging? Maybe I should I have non-polarised 1uF caps.
What kind?
The schematic,
https://www.dropbox.com/s/6n78s84gd9kaouu/High%20impedance%20input%20-%20Copy.jpg?dl=0

Thanks, Mikek

The BJT is a jelly bean NPN, I suspect typo for the once popular 2N3643
(I found some in my junk box even!). Use 2N3904 or 2N2222 or BC548
whatever. The BF256 you used in the first version should be a fine
substitute for 2N4416 - they are both listed as process 50 parts.

1uF is crazy too big unless do infrasound. Electrolytic leakage would be
terrible at the front end. For the gate bias bootstrap even 1nF is
massive, you can probably omit that part since even 10meg from the
unbootstrapped resistor is more than you are aiming at. For the drain
bootstrap a capacitor of 0.01uF would be OK down to a few kHz. I think
your range is 0.5-30MHz?

Everything between your Zin input test resistance and the gate should
have minimal stray capacity - i.e. built up in the air a few mm above
the board.

piglet
 
On Monday, November 7, 2022 at 1:11:45 PM UTC-6, Jeroen Belleman wrote:

Thanks, Mikek

There are no 1uF capacitors in that schematic. They are 0.1uF, but the decimal
dot is all but vanishing. It wouldn\'t make much difference though. Either should
work. If you really want to use polarized capacitors, the NPN emitter has the
lowest DC potential of the three junctions, so the negative terminals of the
caps should be connected there. For AC, the three nodes swing the same way,
near enough, thanks to those two capacitors. That\'s what bootstraps are
*intended* to do.

That said, it\'s about time you Americans drop the silly .1u. Dots *do* vanish.
Use 100n. This schematic breaks the point, if you\'ll excuse me the pun.

The schematic is otherwise correct, it\'s an NPN alright.

Jeroen Belleman

We have success!
I laid out a pcb in Paint last night and etched it this morning.
https://www.dropbox.com/s/fu53nx078daub2u/Linear%20high%20input%20impedance%20complete%20pcb.jpg?dl=0
No ground plane under the parts on either side.
I used the 1uF, may have to change them, but it works, flat down to 1kHz, maybe lower I didn\'t test.
AND, it is flat to 17MHz, then the output has a slight increase in level at 32Mhz (10%, 1.415Vpp to 1.565Vpp)
although it has a peak at 29Mhz that is 15%.
The output cap is a 0.1uF WITH A 1kΩ load.
I need to add a couple of bypass caps I forgot about.
It goes all the way to 90MHz before it starts to drop again.
Any thought about knocking down the gain a little from 17MHz to 30MHz?
I left the semi conductor leads long, any reason the shorten them.
Thanks for the help, Mikek
 
On Monday, November 7, 2022 at 1:37:09 PM UTC-6, erichp...@hotmail.com wrote:

Thanks, Mikek
The BJT is a jelly bean NPN, I suspect typo for the once popular 2N3643
(I found some in my junk box even!). Use 2N3904 or 2N2222 or BC548
whatever. The BF256 you used in the first version should be a fine
substitute for 2N4416 - they are both listed as process 50 parts.

1uF is crazy too big unless do infrasound. Electrolytic leakage would be
terrible at the front end. For the gate bias bootstrap even 1nF is
massive, you can probably omit that part since even 10meg from the
unbootstrapped resistor is more than you are aiming at. For the drain
bootstrap a capacitor of 0.01uF would be OK down to a few kHz. I think
your range is 0.5-30MHz?

Everything between your Zin input test resistance and the gate should
have minimal stray capacity - i.e. built up in the air a few mm above
the board.

piglet

If you haven\'t read my previous post, IT WORKS!
I used the BF256C and MPHS10.
I understand the 1uF is wrong, and it should be 0.1uF.
I\'ll be changing both.
I had some internal debate, on how to place the 2.2MΩ, 1MΩ voltage divider that drives the 10MΩ gate resistor.
So, I ended up running the input under the 2.2MΩ resistor, I have removed the ground plane from both sides
of the pcb in that area.
Thank, Mikek
 
On 2022-11-07 21:53, Lamont Cranston wrote:
On Monday, November 7, 2022 at 1:11:45 PM UTC-6, Jeroen Belleman wrote:

Thanks, Mikek

There are no 1uF capacitors in that schematic. They are 0.1uF, but the decimal
dot is all but vanishing. It wouldn\'t make much difference though. Either should
work. If you really want to use polarized capacitors, the NPN emitter has the
lowest DC potential of the three junctions, so the negative terminals of the
caps should be connected there. For AC, the three nodes swing the same way,
near enough, thanks to those two capacitors. That\'s what bootstraps are
*intended* to do.

That said, it\'s about time you Americans drop the silly .1u. Dots *do* vanish.
Use 100n. This schematic breaks the point, if you\'ll excuse me the pun.

The schematic is otherwise correct, it\'s an NPN alright.

Jeroen Belleman

We have success!
I laid out a pcb in Paint last night and etched it this morning.
https://www.dropbox.com/s/fu53nx078daub2u/Linear%20high%20input%20impedance%20complete%20pcb.jpg?dl=0
No ground plane under the parts on either side.
I used the 1uF, may have to change them, but it works, flat down to 1kHz, maybe lower I didn\'t test.
AND, it is flat to 17MHz, then the output has a slight increase in level at 32Mhz (10%, 1.415Vpp to 1.565Vpp)
although it has a peak at 29Mhz that is 15%.
The output cap is a 0.1uF WITH A 1kΩ load.
I need to add a couple of bypass caps I forgot about.
It goes all the way to 90MHz before it starts to drop again.
Any thought about knocking down the gain a little from 17MHz to 30MHz?
I left the semi conductor leads long, any reason the shorten them.
Thanks for the help, Mikek

Good! Congratulations.

First finish adding the bypass caps. Followers with even slightly capacitive
loads can have a region with negative input resistance. Maybe you\'re getting
close to such conditions.Try a ferrite bead in the gate lead, maybe. You
may also try out what happens if you remove either or both of the bootstraps.
Shortening the leads of parts, making the circuit more compact, might help too.

Jeroen Belleman
 
On 07/11/2022 9:04 pm, Lamont Cranston wrote:
On Monday, November 7, 2022 at 1:37:09 PM UTC-6, erichp...@hotmail.com wrote:

Thanks, Mikek
The BJT is a jelly bean NPN, I suspect typo for the once popular 2N3643
(I found some in my junk box even!). Use 2N3904 or 2N2222 or BC548
whatever. The BF256 you used in the first version should be a fine
substitute for 2N4416 - they are both listed as process 50 parts.

1uF is crazy too big unless do infrasound. Electrolytic leakage would be
terrible at the front end. For the gate bias bootstrap even 1nF is
massive, you can probably omit that part since even 10meg from the
unbootstrapped resistor is more than you are aiming at. For the drain
bootstrap a capacitor of 0.01uF would be OK down to a few kHz. I think
your range is 0.5-30MHz?

Everything between your Zin input test resistance and the gate should
have minimal stray capacity - i.e. built up in the air a few mm above
the board.

piglet

If you haven\'t read my previous post, IT WORKS!
I used the BF256C and MPHS10.
I understand the 1uF is wrong, and it should be 0.1uF.
I\'ll be changing both.
I had some internal debate, on how to place the 2.2MΩ, 1MΩ voltage divider that drives the 10MΩ gate resistor.
So, I ended up running the input under the 2.2MΩ resistor, I have removed the ground plane from both sides
of the pcb in that area.
Thank, Mikek

I am very pleased for you. Thanks for letting us know. My first reply
mentioned bootstrapping away the drain capacity and that seems (along
with minimising wiring strays) to have been one of the factors.

You might be able to get rid of the gate bias bootstrap since at your
frequencies it won\'t be helping much?

piglet
 
I have added the bypass caps and changed the 1uF to 0.1uF.
Also fixed the lack of ground on the input, it was soldered but
I had cut the foil to that section of ground plane. grounding the input
made it susceptible to a 200MHz oscillation, comes and goes depending position,
if I\'m reaching to adjust the sig gen and maybe how I\'m holding my tongue.
I\"ll try the bead and if the doesn\'t help, I\'ll shorten the FET leads.
After the changes it is a lot tamer, it is a very gradual rise in amplitude as frequency increase,
no peak (at least to 30MHz) and only 6% from 1MHz to 30MHz.

Ok, I just added a piece of aluminum foil on the underside of the pcb to act as a ground plane
That makes takes away the level rise with frequency, much better. Also no more 200MHz oscillation seen.
I\'ll try a more permanent underside ground plane, I have some wide copper tape, I\'ll apply and solder.

I added a underside groundplane, it tamed the 200MHz oscillation and flattened the response.
Here\'s a picture at ~1MHz and 30MHz, only a 2% rise at 30MHz.
https://www.dropbox.com/s/svdhh7mmr52hxcj/Linear%20freq%20response.jpg?dl=0

Mikek
 
Years ago, I built this Kleijer High input impedance amp.
http://www.crystal-radio.eu/fetamp/enfetamp.htm
The input impedance test:
I put an inductor on my Q meter and resonated it at 1MHz.
Tuning cap 151.1pf, Xc = 1,053Ω, Q = 1068
Rp of the LC is ,Rp = Q x Xc, so, 1,068 x 1,053 =1,124,604Ω =Rp.
Then I put the Kleijer amp input in parallel with the tuning capacitor.
I had to reduce the Q meter tuning capacitor by 1.1pf to get back to resonance.
The new Q with the Kleijer amp attached dropped to 1,062. So Rp= 1062 x 1053 = 1,118,286Ω
To get 1,118,286 Ω I need to parallel the original (unloaded) 1,124,604 Ω with 200,000,000 Ω.
i.e. 1,124,604Ω // 200,000,000Ω = 1,118,286Ω
So, I think the input R of the amp is 200MΩ.
Does this sound like a correct method?
Does the input capacitance matter, (as a load) if I\'m resonating it out.
Mikek
P.S. Kleijer uses an air input cap, I used a tiny dot of roger 5880 pcb as my capacitor,
it would be interesting to make mine an air cap and see if there is a difference.
 
On Thursday, November 10, 2022 at 5:59:56 AM UTC-6, Lamont Cranston wrote:
Years ago, I built this Kleijer High input impedance amp.
http://www.crystal-radio.eu/fetamp/enfetamp.htm
The input impedance test:
I put an inductor on my Q meter and resonated it at 1MHz.
Tuning cap 151.1pf, Xc = 1,053Ω, Q = 1068
Rp of the LC is ,Rp = Q x Xc, so, 1,068 x 1,053 =1,124,604Ω =Rp.
Then I put the Kleijer amp input in parallel with the tuning capacitor.
I had to reduce the Q meter tuning capacitor by 1.1pf to get back to resonance.
The new Q with the Kleijer amp attached dropped to 1,062. So Rp= 1062 x 1053 = 1,118,286Ω
To get 1,118,286 Ω I need to parallel the original (unloaded) 1,124,604 Ω with 200,000,000 Ω.
i.e. 1,124,604Ω // 200,000,000Ω = 1,118,286Ω
So, I think the input R of the amp is 200MΩ.
Does this sound like a correct method?
Does the input capacitance matter, (as a load) if I\'m resonating it out.
Mikek
P.S. Kleijer uses an air input cap, I used a tiny dot of roger 5880 pcb as my capacitor,
it would be interesting to make mine an air cap and see if there is a difference.

Seems to be a problem with the amp from the data book.
I did the same experimant shown above but with the databook amp.
Instead of it loading the LC, the Q more than doubles, instead of 1,000 it\'s 2500!
What\'s the fix for that? :)
Mikek
 
On 10/11/2022 5:53 pm, Lamont Cranston wrote:
On Thursday, November 10, 2022 at 5:59:56 AM UTC-6, Lamont Cranston wrote:
Years ago, I built this Kleijer High input impedance amp.
http://www.crystal-radio.eu/fetamp/enfetamp.htm
The input impedance test:
I put an inductor on my Q meter and resonated it at 1MHz.
Tuning cap 151.1pf, Xc = 1,053Ω, Q = 1068
Rp of the LC is ,Rp = Q x Xc, so, 1,068 x 1,053 =1,124,604Ω =Rp.
Then I put the Kleijer amp input in parallel with the tuning capacitor.
I had to reduce the Q meter tuning capacitor by 1.1pf to get back to resonance.
The new Q with the Kleijer amp attached dropped to 1,062. So Rp= 1062 x 1053 = 1,118,286Ω
To get 1,118,286 Ω I need to parallel the original (unloaded) 1,124,604 Ω with 200,000,000 Ω.
i.e. 1,124,604Ω // 200,000,000Ω = 1,118,286Ω
So, I think the input R of the amp is 200MΩ.
Does this sound like a correct method?
Does the input capacitance matter, (as a load) if I\'m resonating it out.
Mikek
P.S. Kleijer uses an air input cap, I used a tiny dot of roger 5880 pcb as my capacitor,
it would be interesting to make mine an air cap and see if there is a difference.

Seems to be a problem with the amp from the data book.
I did the same experimant shown above but with the databook amp.
Instead of it loading the LC, the Q more than doubles, instead of 1,000 it\'s 2500!
What\'s the fix for that? :)
Mikek

Perhaps some of all that bootstrapping is getting back into the LC tuned
circuit - you have recreated the old-time Q-multiplier. Or the input
levels are so high the buffer is overdriven?

Padding down the input with a capacitive attentuator like Kleijer did
could be a good way to reduce interaction. Also I guess at resonance the
volatge is pretty high so overdriving is a real risk.

piglet
 
On 08/11/2022 10:05 pm, Lamont Cranston wrote:
Anyone care to look at this Chinese design for a high input impedance amp,
and give me their thoughts about it?
Two FETs, two transistors, a little different than I have been looking at.
https://www.dropbox.com/s/ypvmq9ushs4d2cf/High%20input%20impedance%20amp%20Chinese%20Crystal%20Radio%20Forum.jpg?dl=0

Thanks, Mikek

It is fundamentally the same as the one you did yesterday. T3 and C2
bootstrap away the FET drain capacitance, the other circuit didn\'t
bother with the T3 follower using merely an RC. Not sure if the added
complexity is worthwhile or risks more instability. Behavior with large
signals may be different but at first glance can\'t say which is better
or worse, need further thought!

In the real world performance will be dominated by physical layout
strays. If you build it please let us know.

piglet
 
On Thursday, November 10, 2022 at 3:11:28 PM UTC-6, erichp...@hotmail.com wrote:

Seems to be a problem with the amp from the data book.
I did the same experiment shown above but with the databook amp.
Instead of it loading the LC, the Q more than doubles, instead of 1,000 it\'s 2500!
What\'s the fix for that? :)
Mikek
Perhaps some of all that bootstrapping is getting back into the LC tuned
circuit - you have recreated the old-time Q-multiplier. Or the input
levels are so high the buffer is overdriven?

Padding down the input with a capacitive attentuator like Kleijer did
could be a good way to reduce interaction. Also I guess at resonance the
voltage is pretty high so overdriving is a real risk.

piglet

I\'ll try a tiny input capacitor. If I create a 10x capacitive divider, I\'ll need a 10X amp to get back to
a gain of almost 1.
I put a series 0.3pf cap in series with the input. Same as the Kleijer amp.
Turns out that is a 10x was close it\'s 9.8 to 1, the output drops by a factor 9.8.
The input capacitance is 0.45pf and the input resistance measures 180MΩ.
This compares to the 200MΩ of the Kleijer amp, a little surprising sense the databook amp
has bootstrapping and the Kleijer amp doesn\'t.
I need to get some or make some smaller inductors so I can do these tests at 1, 10, 20, and 30MHz,
to see if or how much the input impedance drops.
Thanks, Mikek
 
On 09/11/2022 7:53 am, piglet wrote:
On 08/11/2022 10:05 pm, Lamont Cranston wrote:
Anyone care to look at this Chinese design for a high input impedance
amp,
  and give me their thoughts about it?
  Two FETs, two transistors, a little different than I have been
looking at.
https://www.dropbox.com/s/ypvmq9ushs4d2cf/High%20input%20impedance%20amp%20Chinese%20Crystal%20Radio%20Forum.jpg?dl=0


                          Thanks, Mikek

It is fundamentally the same as the one you did yesterday. T3 and C2
bootstrap away the FET drain capacitance, the other circuit didn\'t
bother with the T3 follower using merely an RC. Not sure if the added
complexity is worthwhile or risks more instability. Behavior with large
signals may be different but at first glance can\'t say which is better
or worse, need further thought!

In the real world performance will be dominated by physical layout
strays. If you build it please let us know.

piglet

Followup #2 - both give roughly similar results - if you can afford the
higher supply voltage of the simpler circuit use that, if you want to
operate from 9V use the more complex circuit?

piglet
 
On 2022-11-08 23:05, Lamont Cranston wrote:
Anyone care to look at this Chinese design for a high input impedance amp,
and give me their thoughts about it?
Two FETs, two transistors, a little different than I have been looking at.
https://www.dropbox.com/s/ypvmq9ushs4d2cf/High%20input%20impedance%20amp%20Chinese%20Crystal%20Radio%20Forum.jpg?dl=0

Thanks, Mikek

It\'s very similar to your previous circuit. Again there is the JFET
follower T1, followed by an NPN follower T4. T2 is a current source,
so that the gain of follower T1 will be very close to unity. There will
be virtually no AC voltage across R2, nor across R1, multiplying the
apparent resistance of the latter a lot.

C2 applies the output signal to follower T3 which bootstraps the
drain of T1, reducing the effect of Cgd of that JFET.

In conclusion, it should work fine.

Jeroen Belleman
 
In the real world performance will be dominated by physical layout
strays.

There is the rub, proper layout, on iteration 3, I followed a couple of the ideas given here,
removing the ground plane and getting the parts raised above the board, although
without the ground plane I don\'t think raising the parts mattered. I suspect removing the ground plane
from the enter circuit was,

not as important as for the high impedance FET area?

I used long leads to keep the parts physically separated, but I know that leads to inductive strays,
so...
l \'ll be reading up on how to mitigate pcb strays before my next build.
If anyone has a favorite site on the subject of stray mitigation, please post.

Is there any advantage using smd components?

I thought there was, but the last build did pretty well with leaded components.

Is it worth using a pcb software program, so I could make thinner tracks to help minimize strays?

If you build it please let us know.
piglet

I did order the transistors and FETs last night, so there is a possibility,
but other projects first.

I can think of only one way to test the input impedance, that is with my Q meter.
Set up a LC at resonance and then add the high input impedance circuit across the
tuning capacitor. Then read out the change of the tuning capacitor and how
much the Q drops, then do the math on the Q change.

With the input current so low, is there another way?
Thanks, Mikek
 

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