Re: Topband: Hi Z amplifiers for 160m

2020-03-14 Thread Grant Saviers
More power to make up for my 10db excess noise = xxx Kw - whoopee!  Need 
to get some 3 phase.


Remote Rx, eg 100km makes a lot more sense.  Clubs could put up shared 
facilities.


With direct sampling synchronous receivers and down sampling of say the 
bottom 50Khz of 160, every user could reconstruct their own pattern out 
of a 4 or 8 square.  Residential internet bandwidth is commonly several 
hundred Mbit/sec. The supercomputer on every desk is up to the 
arithmetic. If you live in the boonies without 200Mbit you don't need 
the remote Rx anyway.


Just a small matter of software  ;) ;)  Haven't the radio telescope guys 
done this in GHz bands?


Grant KZ1W

On 3/13/2020 09:42, Jim Thomson wrote:

Date: Thu, 12 Mar 2020 20:25:16 -0700
From: Jim Brown 
To: topband@contesting.com
Subject: Re: Topband: Hi Z amplifiers for 160m

  
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Re: Topband: Hi Z amplifiers for 160m

2020-03-13 Thread Richard (Rick) Karlquist



On 3/13/2020 12:34 PM, Richard (Rick) Karlquist wrote:



On 3/12/2020 4:29 PM, Mikek wrote:

   I'll stick my neck out and suggest Dallas Lankford's '2 FET amp'.



  If anyone has an interest, I have some more files in my computer.


https://www.okdxf.eu/lankford/Hi%20Z%20PPL%20Loop%20And%20Flag%20Arrays.pdf 



I
  Mikek KF4ITA
_




I didn't look at this circuit carefully; Mikek pointed out that
the JFET's are complementary, not in parallel.  (Thanks Mikek
for correcting me).  I also see that Lankford writes that his circuit is 
derived from Trask's circuit. In any event, the following reference by 
Chris Trask, N7ZWY gives a bunch of different versions of this circuit.


http://home.earthlink.net/~christrask/Complementary Push-Pull Amplifiers.pdf

Chris points out that this idea goes back to at least 1982.

Rick N6RK

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Re: Topband: Hi Z amplifiers for 160m

2020-03-13 Thread Richard (Rick) Karlquist



On 3/12/2020 4:29 PM, Mikek wrote:

   I'll stick my neck out and suggest Dallas Lankford's '2 FET amp'.



  If anyone has an interest, I have some more files in my computer.


https://www.okdxf.eu/lankford/Hi%20Z%20PPL%20Loop%20And%20Flag%20Arrays.pdf 



I
  Mikek KF4ITA
_


This seems to be the same old JFET source follower
that has been around forever, except it uses two FET's in
parallel.  Why not 3 or 4?

I completely fail to see why this amp would be superior to similar
designs already being widely used.  Can someone enlighten me as to
what is special about it, if anything?

My approach to the amplifier noise issue is to abandon 102 inch CB 
whips, however elegant, and instead use 30 foot monopoles with top 
loading, as a brute force tool.  MUCH more signal coming in, in the 
first place.


Rick N6RK
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Re: Topband: Hi Z amplifiers for 160m

2020-03-13 Thread Mike Waters
Me neither.

On Fri, Mar 13, 2020, 12:22 PM Wes  wrote:

> It's not clear to me.
>
> Wes  N7WS
>
> On 3/13/2020 9:42 AM, Jim Thomson wrote:
> > ##  Clearly  whats  required  is a long  overdue  increase  in TX
> power  limits  on  160  band...and  also  80+40.
> > That  or  arrl legal  remote  RXs.  pick  one.
> >
> > Jim VE7RF
>
> _
> Searchable Archives: http://www.contesting.com/_topband - Topband
> Reflector
>
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Re: Topband: Hi Z amplifiers for 160m

2020-03-13 Thread Wes

It's not clear to me.

Wes  N7WS

On 3/13/2020 9:42 AM, Jim Thomson wrote:

##  Clearly  whats  required  is a long  overdue  increase  in TX  power  
limits  on  160  band...and  also  80+40.
That  or  arrl legal  remote  RXs.  pick  one.

Jim VE7RF


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Re: Topband: Hi Z amplifiers for 160m

2020-03-13 Thread Mike Waters
On Thu, Mar 12, 2020, 3:48 PM Michael Tope  wrote:

> There are a lot of SMT to DIP adapter boards out there which would allow
> newer SMD op-amps to be used in older through-hole PWB layouts.
>
>
> https://www.digikey.com/product-detail/en/aries-electronics/LCQT-SOIC8-8/A880AR-ND/4754588


This is great advice, which I think a lot of folks are too quick to dismiss
in this era of vanishing through-hole DIP ICs and transistors with wire
leads.

I successfully did just that with an SO-23 (VERY tiny SMD package) J310
transistor. It was not only my very first attempt at soldering with solder
paste and hot air, but it was the easiest thing that I ever soldered! (And
I've soldered north of two million connections.)

Squirt a *small,* even line of solder paste through both rows of bright
copper pads, place the SMD device onto the paste, and a heat gun from the
underside of the (level) adapter board will make the solder flow exactly
where it should. It'll look like it was professionally machine-soldered.

FORGET trying to solder an SMD device using the regular method! Even with a
bright light and a magnifying headband, it just makes a mess, pushes the
SMD device around, and the solder bridges are difficult to clear.

Mine did not have the DIP plugs as this one does, just holes for small wire
leads.

Solder paste (a powdered solder and flux mix) can be somewhat expensive,
and IIRC it has a shelf life of less than 5 years. But I found a guy on
eBay who repackages a big jar of solder paste into small syringes for
cheap. He even included two different size nozzles. Don't know if he's
still in business, but there was a nice instructional video that will make
believers out of any "Well, I couldn't do that" skeptics reading this.
Sorry that I don't have a link handy. Last time I looked, YouTube had
several very good videos on this method of soldering. Qrz.com has threads
about this method, you might search there also.

Keeping the paste in your refrigerator in a small Ziploc bag will lengthen
its useful life.

It would take very fine wires indeed to solder small tinned wires directly
to those tiny devices. Just get an adapter board. Trust me. :-)

73, Mike
W0BTU
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Re: Topband: Hi Z amplifiers for 160m (LONG)

2020-03-13 Thread John Kaufmann via Topband
Hi Mike,

Yes, the math can get tricky and cause you to get lost in the forest.  I'm not 
afraid of doing math (I did a mathematics minor in graduate school) but as an 
engineer, I prefer to seek the simplest possible solutions to engineering 
problems.  This is a case where you can avoid messy math by falling back on 
basic principles.

First, I have invoked a passive, lossless phase combiner circuit for the array. 
 There is no loss in generality in doing so.  Gain or loss are just scaling 
factors that affect everything equally.  This is why I said the total amplifier 
circuit noise power coming out of the combiner is exactly equal to the sum of 
the individual amplifier noise powers entering the combiner.  There is no 
combining loss and energy is conserved.  For circuit noise it doesn't matter 
what phases are used in the combiner because random noise is incoherent.  Phase 
only matters for coherent signals.

Next I fix the gain of a single vertical at 0 dB.  Antenna gain is just another 
scaling factor and here were are only interested in relative gain (a single 
vertical vs. a phased array) when determining S/N ratios coming out of the 
combiner.  When I say the received atmospheric power is one "atmospheric noise 
power unit", the gain is imbedded in that quantity but there is no need to 
actually calculate the absolute gain for our purposes.

Next we invoke the principle that the spatially-averaged gain of a single 
vertical and a phased vertical array are exactly the same.  This allows us to 
determine the atmospheric noise power coming out of the combiner without 
actually doing any phasing calculations.  For our combiner the total combined 
atmospheric noise for the array is exactly the same as the total atmospheric 
noise received by a single vertical.  

For signals of interest, again we don't need to do any brute-force mathematical 
phasing calculations.  We can fall back on antenna modeling programs.  Of 
course you can do the math, but modeling programs will spare you the effort.  
Because we have already fixed the gain of a single vertical (at 0 dB), we can 
use EZNEC (or your favorite modeling program) to determine how much additional 
gain the array provides on the signal of interest, based on its direction of 
arrival.  We have already established the array gain for atmospheric noise is 
the same for the array and the single vertical.  Therefore the S/N improvement 
of the array vs. the single vertical (assuming atmospheric noise is the 
dominant noise) is just the difference between the signal gain of the array and 
the single vertical.  Antenna modeling gives you that number.  No ugly math is 
needed.

Getting back to my earlier e-mail about circuit noise vs. atmospheric noise, we 
do need to keep track of the actual amplifier circuit noise relative to the 
atmospheric noise to insure that the circuit noise doesn't degrade the overall 
noise performance of the system.   That will guide us in the design of a 
low-noise amplifier.  To put numbers on these noise quantities, we need to 
either calculate circuit noise power, as others have already started to do, or 
to measure it (as I have done for different amplifiers).  Similarly for 
atmospheric noise, we need to calculate it or measure it.  I leave that for 
others to do.  For an array of N amplified elements, we need to insure that N 
times the circuit noise power of a single amplifier remains well below the 
atmospheric received by the array.

73, John W1FV


-Original Message-
From: Topband [mailto:topband-bounces+john.kaufmann=verizon@contesting.com] 
On Behalf Of Michael Tope
Sent: Friday, March 13, 2020 7:34 AM
To: topband@contesting.com
Subject: Re: Topband: Hi Z amplifiers for 160m (LONG)

I agree with your conclusions regarding the case of isotropic 
atmospheric noise. This is the same reason that cold space looks like 3 
Kelvin regardless of how high the antenna gain. As the antenna gain goes 
up you reinforce to a greater degree a lesser slice of the overall pie. 
This ends up being a wash.

Where I think you may be mistaken, is the relationship between the 
number of amplified elements (N), the gain of the antenna, and properly 
book keeping combining losses. If I have N amplified elements and I  
mathematically sum the amplifiers outputs with zero combining loss (this 
would be equivalent to digitizing the output of each amplifier and then 
summing the results in digital processing), then the uncorrelated noise 
from the amplifiers (as you correctly point out) sum to 10*log(N). 
Double the number of amplified elements and you double the noise power 
due to the amplifiers (i.e. 3dB amplifier noise increase). So far we agree.

Where it gets tricky is when you consider the mathematical addition of 
the over-the-air contributions. If I have a linear broadside array and I 
double the number of elements from N to 2*N, the mathematical sum of the 
components of the signal-of-interest in the bore site o

Re: Topband: Hi Z amplifiers for 160m

2020-03-13 Thread Jim Thomson
Date: Thu, 12 Mar 2020 20:25:16 -0700
From: Jim Brown 
To: topband@contesting.com
Subject: Re: Topband: Hi Z amplifiers for 160m

http://www.contesting.com/_topband - Topband Reflector


Re: Topband: Hi Z amplifiers for 160m

2020-03-13 Thread Dave Cuthbert
The document was published last year so we might assume the noise graph is
up to date. To put this in perspective,

To put the ITU-R P.372-14 claimed noise in perspective here's the
calculated antenna terminal voltage for a 100% efficient 1/4 wavelength
vertical in 500 Hz bandwidth. S-units are also shown.
Quiet receiving site -- 4.7 nV/m, vert 1.3 uV, S-4
Median city noise --  66 nV/m, vert 19 uV, S-8

Dave KH6AQ (formerly WX7G)


>
>
>
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Re: Topband: Hi Z amplifiers for 160m (LONG)

2020-03-13 Thread Michael Tope
r throughput
loss imparted by the combiner circuit).

To determine the total atmospheric noise coming out of the combiner circuit,
let's assume the atmospheric noise has a completely uniform distribution in
3-dimensional space.  That is, the strength of the atmospheric noise is the
same in every direction.  This is an idealized assumption, but is often a
reasonable approximation to reality.  Under these assumptions, the total
atmospheric noise out of the combiner turns out to be just one "atmospheric
noise unit"!  In other words, it is exactly the same as the atmospheric
noise coming out of a single vertical.  This is because the total
atmospheric noise power picked up by the array is just the gain of the array
(relative to a single vertical) averaged over all of 3-dimensional space
times one "atmospheric noise unit" (the noise picked up by a single
vertical).  That average gain is exactly 0 dB, so the total atmospheric
noise doesn't change in our idealized system.  It doesn't matter what the
antenna pattern is; the average gain is always 0 dB, which is why we did not
need to be concerned with details of how signals are phased up to form a
beam pattern.  Of course, a different gain applies to actual signals that
are coming from a specific direction and are not uniformly distributed like
atmospheric noise, which is why we see a S/N improvement when the array is
aimed at a signal of interest.

So, we have demonstrated that in relative terms, the amplifier circuit noise
power in an array of N amplified antennas goes up by a factor N whereas the
atmospheric noise does not change.  That increase in the amplifier noise
contribution relative to atmospheric noise degrades the overall noise figure
of the system.  However, as long as we keep the amplifier noise contribution
small enough, the noise figure degradation can also be kept to a minimum.
That is why having more amplified elements makes it more important to design
the antenna amplifiers for low circuit noise.

73, John W1FV






-Original Message-
From: Topband
[mailto:topband-bounces+john.kaufmann=verizon@contesting.com] On Behalf
Of Michael Tope
Sent: Thursday, March 12, 2020 4:37 PM
To: topband@contesting.com
Subject: Re: Topband: Hi Z amplifiers for 160m

Hi Lee,

Yes, if you are combining coherent signals that are not in phase, then
the each of the voltage vectors is weighted by cos(phi-i) where phi-i is
the angle between the i-th voltage vector and the 1st vector. If phi=0,
then you have the case I described previously. I can see how this can
get tricky, however, with an electrically short baseline where you are
striving for cancellation in the rearward looking direction. It's like
you cancel in the rearward direction and almost cancel in the preferred
direction :-). This degrades the SNR not because the noise is adding up,
but because the signals are subtracting down.

73, Mike W4EF.


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Re: Topband: Hi Z amplifiers for 160m

2020-03-12 Thread Jim Brown

On 3/12/2020 7:44 PM, Dave Cuthbert wrote:

Feel free to review my method/math and make corrections as needed.


Didn't review your math, but the more important question is, "how old is 
your noise data?"  In my experience trying to work EU on Topband now as 
compared to c.a. 2007-8 is vastly more difficult thanks to higher noise 
levels on both ends. Back then I could work EU on CW; now, with better 
antennas, I need the 10 dB advantage of FT8. In the past six seasons 
I've heard six EU/U.K. stations on CW, two were able to hear me. And 
those were all during one of this season's contest.


Bottom line -- if your noise data is ten years old, I'd add 10 dB to it; 
if it's older, probably more.


73, Jim K9YC
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Re: Topband: Hi Z amplifiers for 160m

2020-03-12 Thread Dave Cuthbert
*Amp/antenna noise *-- is the AD8045 noise low enough for a 3-meter
monopole? *0.26 uV amp noise vs. 0.16 uV man-made rural noise and 2.3 uV
city with a 3-meter monopole. *

Feel free to review my method/math and make corrections as needed.

*Rural Noise*, ITU-R P.372-14 (link below)
Working thru formula (7) on page 4 using Figure 7 the man-made noise (quiet
receiving site) E-field at 1.8 MHz is *4.8 nV/m* in a 1 Hz BW. In a *500 Hz*
bandwidth this is *107 nV/m*. Given that a 3-meter (circle array) monopole
has an effective height of 1.5 meters the antenna terminal voltage is *0.16
uV*. Median city noise is 23 dB higher at *2.3 uV.*

*Noise Calculation Inputs*
6-meter monopole source impedance -j3700 ohms
AD8034 voltage noise 3 nV/Hz^0.5 @ 1.8 MHz
AD8045 current noise 3.2 pA/Hz^0.5 @ 1.8 MHz, thru the 3700 ohm antenna
reactance is 12 nV/Hz^0.5

Total noise voltage is the RSS of 3.0 nV and 11.8 nV = *12 nV/Hz^0.5*

https://www.analog.com/media/en/technical-documentation/data-sheets/AD8045.pdf


https://www.itu.int/dms_pubrec/itu-r/rec/p/R-REC-P.372-14-201908-I!!PDF-E.pdf


Dave KH6AQ

On Thu, Mar 12, 2020 at 6:18 AM Dave Cuthbert 
wrote:

> *JFET op amp vs bipolar op amps, *LTSpice simulations connected to a 3
> meter monopole
>
> A bipolar op amp doesn't always give the lowest noise with a short
> monopole at 1.8 MHz because the op amp current noise creates noise voltage
> across the antenna capacitive reactance. Additonally, op amps can be
> connected in parallel for lower voltage noise at the expense of higher
> input capacitance (which loads down the antenna signal voltage).
>
> Simulations of the YCCC amp with a bipolar op amp and a JFET op amp were
> performed. Next, preamps having 2, 4 and 6 JFET op amps were modeled. As
> the number of op amps goes up the antenna voltage goes down with optimum
> S/N ratio, in this case, with 4 op amps. It shows 4.5 dB better S/N than
> the bipolar op amp. The bipolar op circuit is modeled with an LTC6228
> rather than an AD8045 because I didn't have to import the AD8045 model into
> LTSpice. I can try to import the AD8045 later if anyone is interested. The
> LTC6228 op amp has 1/3 the voltage noise and the same current noise with
> Bias Current Compensation disabled, so it should show lower noise than the
> AD8045. The JFET op amp is the ADA4637 and IMD simulations were run with it
> looking better than the bipolar.
>
>
> *YCCC amp with bipolar vs JFET op amp for a 3 meter monopole at 1.8 MHz*
> LTC6228 bipolar op amp, 9.5 nV/Hz^0.5, loaded sig 0.93, relative S/N ratio
> 0 dB
> ADA4637 JFET op amp, 6.7 nV/Hz^0.5, loaded sig 0.85, relative S/N ratio
> 2.2 dB
> 2 X JFET op amp, 4.8 nV/Hz^0.5, loaded sig 0.74, relative S/N ratio 3.9
> dB
> 4 X JFET op amp, 3.6 nV/Hz^0.5, loaded sig 0.59, relative S/N ratio *4.5
> dB*
> 6 X JFET op amp, 3.1 nV/Hz^0.5, loaded sig 0.49, relative S/N ratio 4.2 dB
>
>Dave KH6AQ
>
> On Wed, Mar 11, 2020 at 1:49 AM Chris Moulding <
> chr...@crosscountrywireless.net> wrote:
>
>> As well as being a radio amateur (G4HYG) I also run a small business
>> designing and making radio equipment (Cross Country Wireless).
>>
>> Recently I've been asked by a radio contest group to see if I can
>> redesign the YCCC Hi Z amplifier using modern components and using
>> similar mounting arrangements to our Loop Antenna Amplifier.
>>
>> The first prototype using surface mount components is working well.
>>
>> So far I've not build an array of antennas but that will come later when
>> the production boards arrive.
>>
>> The prototype uses a unity voltage gain amplifier and a BNC connector.
>>
>> I've a couple of questions for others on the list with experience of
>> running vertical receive arrays:
>>
>> Is a unity voltage gain amplifier OK or do you think it needs more gain
>> for long coax runs?
>>
>> At present I'm using a BNC male connector for the output. Would an F
>> type connector be more compatible with existing antenna arrays.
>>
>> 73, Chris G4HYG
>>
>> _
>> Searchable Archives: http://www.contesting.com/_topband - Topband
>> Reflector
>>
>
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Re: Topband: Hi Z amplifiers for 160m

2020-03-12 Thread Ralph Matheny
Lankford's stuff works great.

I have used his antenna which does NOT use
a preamp.it's only suitable for situations
where match to the feedline isn't critical, but
it sure is great to not have any preamp outside.

de K8RYU



From: Topband  on behalf 
of Mikek 
Sent: Thursday, March 12, 2020 7:29 PM
To: topband@contesting.com 
Subject: Topband: Hi Z amplifiers for 160m

  I'll stick my neck out and suggest Dallas Lankford's '2 FET amp'.
  He designed it for phased loop antennas for the MW band.
  I believe it will work to at least to 9 MHz and maybe to 30 MHz.
The specs High input Z, ~100 ohm output Z. He lists input intercepts:
IIP2 = ~ +88dbm and IIP3 = ~+41dbm in the MW band.
  The webpage has some noise measurements on pages 3, 4, and 5 that were
over my head.


   This page has more than just his amp but enough so you can understand it.
  If anyone has an interest, I have some more files in my computer.


> https://www.okdxf.eu/lankford/Hi%20Z%20PPL%20Loop%20And%20Flag%20Arrays.pdf

I have a plan to put a matching transformer and a Hi Z amp on my antenna
with relay switching,
so I can do a real A, B, comparison. If you have any advice on
implementing that or advice about
common mode filtering, I'm listening. Better relay suggestions would be
appreciated.

  Mikek KF4ITA
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Re: Topband: Hi Z amplifiers for 160m (LONG)

2020-03-12 Thread John Kaufmann via Topband
To assess the impact of amplifier circuit noise in "active" receive arrays,
we only need to be concerned with the contribution of amplifier circuit
noise relative to atmospheric noise.   The details of how signals are phased
in any particular array do not matter.  The objective is to keep the total
contribution of amplifier noise far below the atmospheric noise so as not to
degrade the overall system noise floor in any significant way.  However, we
need to understand that the combiner circuit that phases up the signals in a
receive phased array responds very differently to amplifier noise and
atmospheric noise.  This makes it less obvious how to determine whether the
circuit noise of a particular amplifier is "low enough".  Fortunately, there
is a simple way to determine that using basic principles.

Let's start with a single amplified vertical antenna.  To simplify the
analysis, we just set the gain of the vertical to 0 dB.  In practice we can
do a NEC analysis to calculate absolute gain in dBi, factoring in real
losses but that is not necessary and does not change the conclusions.  The
antenna feedpoint amplifier adds its own noise to whatever signal plus
atmospheric noise is received by the vertical.  Let's set the circuit noise
power equal to one "circuit noise unit" and the atmospheric noise power to
one "atmospheric noise unit".  Of course we can put voltage (or power)
numbers on those units, based on properties of the amplifier, the
atmospheric noise, the actual antenna gain, and the measurement bandwidth.
However, that makes things unnecessarily complicated, so we won't do that.

Next we create an array of N amplified vertical antennas, each one identical
to the single vertical we started out with.  We feed the signals from all
the antenna amplifiers into an ideal combiner circuit that does not add its
own noise.  The combiner circuit phases up signals to create a directive
beam pattern.  Now we ask how much atmospheric noise appears in the phased
up sum compared to the amount of total amplifier circuit noise.  

The atmospheric noises received at the various verticals are all correlated.
The correlation comes about because the atmospheric noise is the same at
each vertical except for time delay differences caused by geometric path
length differences to each antenna element.  However, as I described in an
earlier e-mail, the amplifier circuit noises coming from each of the antenna
amplifiers are all uncorrelated.

For uncorrelated noises, the combiner simply adds the circuit noise powers
of the individual amplifiers as I described previously.  For N elements with
N amplifiers, the total circuit noise power out of the combiner is then N
times one "circuit noise unit" (ignoring any additional gain or throughput
loss imparted by the combiner circuit).

To determine the total atmospheric noise coming out of the combiner circuit,
let's assume the atmospheric noise has a completely uniform distribution in
3-dimensional space.  That is, the strength of the atmospheric noise is the
same in every direction.  This is an idealized assumption, but is often a
reasonable approximation to reality.  Under these assumptions, the total
atmospheric noise out of the combiner turns out to be just one "atmospheric
noise unit"!  In other words, it is exactly the same as the atmospheric
noise coming out of a single vertical.  This is because the total
atmospheric noise power picked up by the array is just the gain of the array
(relative to a single vertical) averaged over all of 3-dimensional space
times one "atmospheric noise unit" (the noise picked up by a single
vertical).  That average gain is exactly 0 dB, so the total atmospheric
noise doesn't change in our idealized system.  It doesn't matter what the
antenna pattern is; the average gain is always 0 dB, which is why we did not
need to be concerned with details of how signals are phased up to form a
beam pattern.  Of course, a different gain applies to actual signals that
are coming from a specific direction and are not uniformly distributed like
atmospheric noise, which is why we see a S/N improvement when the array is
aimed at a signal of interest.

So, we have demonstrated that in relative terms, the amplifier circuit noise
power in an array of N amplified antennas goes up by a factor N whereas the
atmospheric noise does not change.  That increase in the amplifier noise
contribution relative to atmospheric noise degrades the overall noise figure
of the system.  However, as long as we keep the amplifier noise contribution
small enough, the noise figure degradation can also be kept to a minimum.
That is why having more amplified elements makes it more important to design
the antenna amplifiers for low circuit noise.

73, John W1FV






-Original Message-
From: Topband
[mailto:topband-bounces+john.kaufmann=verizon@contesting.com] On Behalf
Of Michael Tope
Sent: Thursday, March 

Re: Topband: Hi Z amplifiers for 160m

2020-03-12 Thread Jim Brown

On 3/12/2020 4:13 AM, John Kaufmann via Topband wrote:

I think you are confusing voltage and power.  For incoherent sources like 
amplifier noise, the voltages of multiple incoherent sources add in a 
root-sum-squared (RSS) fashion.  The voltage of the sum of eight incoherent 
sources is square root of eight times a single noise source, assuming equal 
combining ratios.  However, because power is proportional to the square of 
voltage, then the*power*  of the combined sum is the sum of the individual 
noise powers.


As long as they are measured at the same point in any given circuit, dB 
computations for power and for voltage yield the same result provided 
that the nature of the signals, their frequencies, and phase 
relationships are taken into account. It's important to remember that 
the fundamental definition of dB is the log of a POWER ratio; it gets 
tied to voltage when circuit impedance is defined. And that PHASE has 
meaning only at a single frequency.


The above computations can get messy when impedances vary with 
frequency, and as the phase relationship between coherent signals vary 
with frequency, position, and time offsets.


73, Jim K9YC
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Re: Topband: Hi Z amplifiers for 160m

2020-03-12 Thread Michael Tope
There are a lot of SMT to DIP adapter boards out there which would allow 
newer SMD op-amps to be used in older through-hole PWB layouts.


https://www.digikey.com/product-detail/en/aries-electronics/LCQT-SOIC8-8/A880AR-ND/4754588

73, Mike W4EF.


On 3/12/2020 1:15 PM, Lee STRAHAN wrote:

John,
Yes of course you are quite correct. I stand corrected.  I should not have 
used the word power. My thinking was along the line of what Mike W4EF posted.
Just did not say it right. Also, I have never disagreed with your choice of the 
8055 as I was aware of why you made that decision. Fortunately for us there are 
some op-amps now that show some really great specs. Unfortunately for us a lot 
of the older through the hole mount parts are disappearing quickly. Surface 
mount seems here to stay.
Lee  K7TJR

From: John Kaufmann 
Sent: Thursday, March 12, 2020 4:14 AM
To: k7...@msn.com; topband@contesting.com
Subject: Re: Topband: Hi Z amplifiers for 160m

Lee,

I think you are confusing voltage and power.  For incoherent sources like 
amplifier noise, the voltages of multiple incoherent sources add in a 
root-sum-squared (RSS) fashion.  The voltage of the sum of eight incoherent 
sources is square root of eight times a single noise source, assuming equal 
combining ratios.  However, because power is proportional to the square of 
voltage, then the *power* of the combined sum is the sum of the individual 
noise powers.  This is well known in the theory of random processes, which is 
the basis of communications theory.  So, what I said earlier is correct.  For a 
system with eight amplifiers, the effective total noise power in the sum is 
eight times the individual noise powers when the sources are combined with 
equal weights.  The YCCC array does not use equal weights, so the powers have 
be weighted when combining them to get the total noise power.

73, John W1FV


-Original Message-
From: Lee STRAHAN mailto:k7...@msn.com>>
To: topband@contesting.com<mailto:topband@contesting.com> 
mailto:topband@contesting.com>>
Sent: Wed, Mar 11, 2020 10:22 pm
Subject: Re: Topband: Hi Z amplifiers for 160m
   Hello John and all,
   Concerning the adding the noise in a typical array. If the noise was 
coherent or exactly the same signal from each element/amp the summed noise 
would indeed be 8 times. However circuit noise is always random and incoherent 
which causes the summation to be a single noise power times the square root of 
the number of elements assuming equal levels from each amp. In the case of 8 
elements 4.5 dB increase which is no small matter as well. In the case of the 
three elements the noise summation would be about 2.4 dB higher than a single 
element.
Lee  K7TJR  OR

As the designer of the YCCC high impedance feedpoint amplifier, let me address 
some issues related to the design of the YCCC amplifier as well as feedpoint 
amplifiers in general.  If you don't want to read a lot of technical 
gobbledygook, please disregard this message.

The YCCC uses an AD8055 RF amp as the gain element.  As Lee, K7TJF, points out, there are most 
certainly better op amps out there.  However, the AD8055 was the "best" part I could find 
in a DIP-8 package.  The "better" op amps are all SMT parts but given that the YCCC 
preamp was a kit, I intentionally limited the selection to DIP-8 parts that kit builders could work 
with relatively easily on a PCB.  Not everyone is able to do a competent job soldering tiny SMT 
parts.

Within the universe of available RF op amps, tradeoffs must be made in terms of 
noise, linearity, and bandwidth.  The AD8055 is not the lowest noise part but 
it has excellent linearity and plenty of bandwidth for HF use.  At my QTH there 
is an AM BCB station 3 miles away, which makes it a somewhat challenging EMI 
environment.  The decision to run the op amp in a unity gain configuration 
comes down to linear dynamic range.  It is easy to design for more gain, but it 
is also easily demonstrated that you will begin to suffer in terms of unwanted 
intermods.  With the YCCC preamp, I get absolutely zero BCB intermods or 
distortion products in the 160m band at my QTH.

In general I do not like to use an outboard preamplifier between the output of 
the phased array combiner circuit and my receiver because it degrades the 
linear dynamic range of the system.  The YCCC system user's manual (Section
12.1) does specify several outboard preamps that could be used.  In a low EMI 
environment, I think they all work fine.  However, at my QTH, with the nearby 
AM BCB station, all of them, without exception, generate increased distortion 
and intermod, which I find unacceptable.

It is always desirable to apply RF gain with a roofing filter in front, which 
is becoming common practice in high performance receivers.  With my K3S 
receiver, the use of a unity gain antenna feedpoint preamplifier is perfectly 
fine if you also turn on the preamp in the K3S

Re: Topband: Hi Z amplifiers for 160m

2020-03-12 Thread Michael Tope

Hi Lee,

Yes, if you are combining coherent signals that are not in phase, then 
the each of the voltage vectors is weighted by cos(phi-i) where phi-i is 
the angle between the i-th voltage vector and the 1st vector. If phi=0, 
then you have the case I described previously. I can see how this can 
get tricky, however, with an electrically short baseline where you are 
striving for cancellation in the rearward looking direction. It's like 
you cancel in the rearward direction and almost cancel in the preferred 
direction :-). This degrades the SNR not because the noise is adding up, 
but because the signals are subtracting down.


73, Mike W4EF.

On 3/11/2020 10:23 PM, Lee STRAHAN wrote:

Mike and all,
   Well stated Mike. It's been a long time since we have conversed. The 
modifier to this is when the signals coming into the combiner are no longer in 
phase or coherent. This as a result of delay lines and time of signal arrival 
at the many elements. Most often in our small portion of a wavelength low 
frequency arrays the combination of signals is subtractive to form a given 
pattern per array dimension. This then lowers the signal to noise ratio. It 
gets pretty complicated to arrive at a noise figure. The only way we have been 
able to do this with amplified arrays is to simulate the array in NEC being 
excited with a known signal many wavelengths away. We can extract the actual 
amplitude and phase of these multi element array signals and then combine them 
mathematically as you have done by example to arrive at a signal gain number 
from signal combination. The noise gain is easy. I say we because I have a 
retired very smart Ham friend in Finland that has helped me through this. I

t h

  as caused me to rethink gain distribution in some of my arrays.
Lee   K7TJR  OR

What matters is the signal-to-noise ratio (SNR). Take the canonical example of 
an ideal 2-port Wilkinson power combiner with in-phase coherent signals of 10 
Vrms applied to each input along with 1 Vrms random thermal noise from the 
respective element amplifiers applied to each input (i.e. each input signal has 
a 20*log(10 Vrms/1 Vrms) = 20dB SNR).

The power loss of the combiner is 3.01 dB [i.e. 10*log(2)], so voltage of each 
signal is attenuated by 1/sqrt(2) = 0.707. Thus, the components of each input 
signal appearing at the output are 7.07 Vrms each and
0.707 for each of the noise inputs.

The signal components add coherently at the combiner output yielding a total 
signal voltage of 14.14 Volts rms. The noise voltages are incoherent, so they 
add as root-sum-square at the output of the combiner. This yields a total noise 
voltage of sqrt(0.707^2 + 0.707^2) =
sqrt(1) = 1.0 Vrms. Thus, the combined noise voltage is unchanged, but the 
signal voltage goes up by sqrt(2).

The SNR of the combined output = 20*log(14.14Vrms/1Vrms) = 23dB, a 3dB 
improvement.

The same things holds for an ideal N-way combiner with equals noise components 
at each input. The noise power at the combined output equals the noise power of 
any of the equal input components (i.e. 0dB gain).

73, Mike W4EF..



On 3/11/2020 7:22 PM, Lee STRAHAN wrote:

 Hello John and all,
 Concerning the adding the noise in a typical array. If the noise was 
coherent or exactly the same signal from each element/amp the summed noise 
would indeed be 8 times. However circuit noise is always random and incoherent 
which causes the summation to be a single noise power times the square root of 
the number of elements assuming equal levels from each amp. In the case of 8 
elements 4.5 dB increase which is no small matter as well. In the case of the 
three elements the noise summation would be about 2.4 dB higher than a single 
element.
Lee  K7TJR  OR

As the designer of the YCCC high impedance feedpoint amplifier, let me address 
some issues related to the design of the YCCC amplifier as well as feedpoint 
amplifiers in general.  If you don't want to read a lot of technical 
gobbledygook, please disregard this message.

The YCCC uses an AD8055 RF amp as the gain element.  As Lee, K7TJF, points out, there are most 
certainly better op amps out there.  However, the AD8055 was the "best" part I could find 
in a DIP-8 package.  The "better" op amps are all SMT parts but given that the YCCC 
preamp was a kit, I intentionally limited the selection to DIP-8 parts that kit builders could work 
with relatively easily on a PCB.  Not everyone is able to do a competent job soldering tiny SMT 
parts.

Within the universe of available RF op amps, tradeoffs must be made in terms of 
noise, linearity, and bandwidth.  The AD8055 is not the lowest noise part but 
it has excellent linearity and plenty of bandwidth for HF use.  At my QTH there 
is an AM BCB station 3 miles away, which makes it a somewhat challenging EMI 
environment.  The decision to run the op amp in a unity gain configuration 
comes down to linear dynamic range.  It is easy to design 

Re: Topband: Hi Z amplifiers for 160m

2020-03-12 Thread Lee STRAHAN
John,
   Yes of course you are quite correct. I stand corrected.  I should not have 
used the word power. My thinking was along the line of what Mike W4EF posted.
Just did not say it right. Also, I have never disagreed with your choice of the 
8055 as I was aware of why you made that decision. Fortunately for us there are 
some op-amps now that show some really great specs. Unfortunately for us a lot 
of the older through the hole mount parts are disappearing quickly. Surface 
mount seems here to stay.
Lee  K7TJR

From: John Kaufmann 
Sent: Thursday, March 12, 2020 4:14 AM
To: k7...@msn.com; topband@contesting.com
Subject: Re: Topband: Hi Z amplifiers for 160m

Lee,

I think you are confusing voltage and power.  For incoherent sources like 
amplifier noise, the voltages of multiple incoherent sources add in a 
root-sum-squared (RSS) fashion.  The voltage of the sum of eight incoherent 
sources is square root of eight times a single noise source, assuming equal 
combining ratios.  However, because power is proportional to the square of 
voltage, then the *power* of the combined sum is the sum of the individual 
noise powers.  This is well known in the theory of random processes, which is 
the basis of communications theory.  So, what I said earlier is correct.  For a 
system with eight amplifiers, the effective total noise power in the sum is 
eight times the individual noise powers when the sources are combined with 
equal weights.  The YCCC array does not use equal weights, so the powers have 
be weighted when combining them to get the total noise power.

73, John W1FV


-Original Message-
From: Lee STRAHAN mailto:k7...@msn.com>>
To: topband@contesting.com<mailto:topband@contesting.com> 
mailto:topband@contesting.com>>
Sent: Wed, Mar 11, 2020 10:22 pm
Subject: Re: Topband: Hi Z amplifiers for 160m
  Hello John and all,
  Concerning the adding the noise in a typical array. If the noise was coherent 
or exactly the same signal from each element/amp the summed noise would indeed 
be 8 times. However circuit noise is always random and incoherent which causes 
the summation to be a single noise power times the square root of the number of 
elements assuming equal levels from each amp. In the case of 8 elements 4.5 dB 
increase which is no small matter as well. In the case of the three elements 
the noise summation would be about 2.4 dB higher than a single element.
Lee  K7TJR  OR

As the designer of the YCCC high impedance feedpoint amplifier, let me address 
some issues related to the design of the YCCC amplifier as well as feedpoint 
amplifiers in general.  If you don't want to read a lot of technical 
gobbledygook, please disregard this message.

The YCCC uses an AD8055 RF amp as the gain element.  As Lee, K7TJF, points out, 
there are most certainly better op amps out there.  However, the AD8055 was the 
"best" part I could find in a DIP-8 package.  The "better" op amps are all SMT 
parts but given that the YCCC preamp was a kit, I intentionally limited the 
selection to DIP-8 parts that kit builders could work with relatively easily on 
a PCB.  Not everyone is able to do a competent job soldering tiny SMT parts.

Within the universe of available RF op amps, tradeoffs must be made in terms of 
noise, linearity, and bandwidth.  The AD8055 is not the lowest noise part but 
it has excellent linearity and plenty of bandwidth for HF use.  At my QTH there 
is an AM BCB station 3 miles away, which makes it a somewhat challenging EMI 
environment.  The decision to run the op amp in a unity gain configuration 
comes down to linear dynamic range.  It is easy to design for more gain, but it 
is also easily demonstrated that you will begin to suffer in terms of unwanted 
intermods.  With the YCCC preamp, I get absolutely zero BCB intermods or 
distortion products in the 160m band at my QTH.

In general I do not like to use an outboard preamplifier between the output of 
the phased array combiner circuit and my receiver because it degrades the 
linear dynamic range of the system.  The YCCC system user's manual (Section
12.1) does specify several outboard preamps that could be used.  In a low EMI 
environment, I think they all work fine.  However, at my QTH, with the nearby 
AM BCB station, all of them, without exception, generate increased distortion 
and intermod, which I find unacceptable.

It is always desirable to apply RF gain with a roofing filter in front, which 
is becoming common practice in high performance receivers.  With my K3S 
receiver, the use of a unity gain antenna feedpoint preamplifier is perfectly 
fine if you also turn on the preamp in the K3S.  This gives the best overall 
linear dynamic range with a preamplified short vertical system.
There is no loss in noise performance because the noise on 160 and 80 is 
totally dominated by atmospheric noise.  In measurements I made at my QTH, the 
internal noise of the YCCC preamp is about 10 dB lower than my d

Re: Topband: Hi Z amplifiers for 160m

2020-03-12 Thread GEORGE WALLNER

Chris,
Good choice.
Perhaps one note of caution. With a BJT input like this the input current 
noise may be more dominant, unless the input impedance is kept low.


Would be great to see the final design.

GL and 73,
George,
AA7JV


 
On Thu, 12 Mar 2020 10:10:44 +

 Chris Moulding  wrote:

Thanks again for all the comments. Very interesting especially the reasoning 
behind the designs.

The device I've picked for my design is the LTC6228. This is a new device by 
Analog Devices that only came out late last year. The voltage noise is 0.88 
uV/sqrt Hz and the current noise is 3 pA/sqrt Hz. Claimed output IP product 
performance is <-100 dBc at 4V peak to peak output.

The device is available in SOT-23 package from DigiKey and Mouser.

I'm planning to use the imminent coronavirus lockdown over here in the UK to 
get some PCB designs done.

73, Chris G4HYG

_
Searchable Archives: http://www.contesting.com/_topband - Topband Reflector


_
Searchable Archives: http://www.contesting.com/_topband - Topband Reflector


Re: Topband: Hi Z amplifiers for 160m

2020-03-12 Thread Dave Cuthbert
*JFET op amp vs bipolar op amps, *LTSpice simulations connected to a 3
meter monopole

A bipolar op amp doesn't always give the lowest noise with a short monopole
at 1.8 MHz because the op amp current noise creates noise voltage across
the antenna capacitive reactance. Additonally, op amps can be connected in
parallel for lower voltage noise at the expense of higher input capacitance
(which loads down the antenna signal voltage).

Simulations of the YCCC amp with a bipolar op amp and a JFET op amp were
performed. Next, preamps having 2, 4 and 6 JFET op amps were modeled. As
the number of op amps goes up the antenna voltage goes down with optimum
S/N ratio, in this case, with 4 op amps. It shows 4.5 dB better S/N than
the bipolar op amp. The bipolar op circuit is modeled with an LTC6228
rather than an AD8045 because I didn't have to import the AD8045 model into
LTSpice. I can try to import the AD8045 later if anyone is interested. The
LTC6228 op amp has 1/3 the voltage noise and the same current noise with
Bias Current Compensation disabled, so it should show lower noise than the
AD8045. The JFET op amp is the ADA4637 and IMD simulations were run with it
looking better than the bipolar.


*YCCC amp with bipolar vs JFET op amp for a 3 meter monopole at 1.8 MHz*
LTC6228 bipolar op amp, 9.5 nV/Hz^0.5, loaded sig 0.93, relative S/N ratio
0 dB
ADA4637 JFET op amp, 6.7 nV/Hz^0.5, loaded sig 0.85, relative S/N ratio 2.2
dB
2 X JFET op amp, 4.8 nV/Hz^0.5, loaded sig 0.74, relative S/N ratio 3.9 dB
4 X JFET op amp, 3.6 nV/Hz^0.5, loaded sig 0.59, relative S/N ratio *4.5 dB*
6 X JFET op amp, 3.1 nV/Hz^0.5, loaded sig 0.49, relative S/N ratio 4.2 dB

   Dave KH6AQ

On Wed, Mar 11, 2020 at 1:49 AM Chris Moulding <
chr...@crosscountrywireless.net> wrote:

> As well as being a radio amateur (G4HYG) I also run a small business
> designing and making radio equipment (Cross Country Wireless).
>
> Recently I've been asked by a radio contest group to see if I can
> redesign the YCCC Hi Z amplifier using modern components and using
> similar mounting arrangements to our Loop Antenna Amplifier.
>
> The first prototype using surface mount components is working well.
>
> So far I've not build an array of antennas but that will come later when
> the production boards arrive.
>
> The prototype uses a unity voltage gain amplifier and a BNC connector.
>
> I've a couple of questions for others on the list with experience of
> running vertical receive arrays:
>
> Is a unity voltage gain amplifier OK or do you think it needs more gain
> for long coax runs?
>
> At present I'm using a BNC male connector for the output. Would an F
> type connector be more compatible with existing antenna arrays.
>
> 73, Chris G4HYG
>
> _
> Searchable Archives: http://www.contesting.com/_topband - Topband
> Reflector
>
_
Searchable Archives: http://www.contesting.com/_topband - Topband Reflector


Re: Topband: Hi Z amplifiers for 160m

2020-03-12 Thread John Kaufmann via Topband
Lee,
I think you are confusing voltage and power.  For incoherent sources like 
amplifier noise, the voltages of multiple incoherent sources add in a 
root-sum-squared (RSS) fashion.  The voltage of the sum of eight incoherent 
sources is square root of eight times a single noise source, assuming equal 
combining ratios.  However, because power is proportional to the square of 
voltage, then the *power* of the combined sum is the sum of the individual 
noise powers.  This is well known in the theory of random processes, which is 
the basis of communications theory.  So, what I said earlier is correct.  For a 
system with eight amplifiers, the effective total noise power in the sum is 
eight times the individual noise powers when the sources are combined with 
equal weights.  The YCCC array does not use equal weights, so the powers have 
be weighted when combining them to get the total noise power.
73, John W1FV


-Original Message-
From: Lee STRAHAN 
To: topband@contesting.com 
Sent: Wed, Mar 11, 2020 10:22 pm
Subject: Re: Topband: Hi Z amplifiers for 160m

  Hello John and all,
  Concerning the adding the noise in a typical array. If the noise was coherent 
or exactly the same signal from each element/amp the summed noise would indeed 
be 8 times. However circuit noise is always random and incoherent which causes 
the summation to be a single noise power times the square root of the number of 
elements assuming equal levels from each amp. In the case of 8 elements 4.5 dB 
increase which is no small matter as well. In the case of the three elements 
the noise summation would be about 2.4 dB higher than a single element.
Lee  K7TJR  OR

As the designer of the YCCC high impedance feedpoint amplifier, let me address 
some issues related to the design of the YCCC amplifier as well as feedpoint 
amplifiers in general.  If you don't want to read a lot of technical 
gobbledygook, please disregard this message.

The YCCC uses an AD8055 RF amp as the gain element.  As Lee, K7TJF, points out, 
there are most certainly better op amps out there.  However, the AD8055 was the 
"best" part I could find in a DIP-8 package.  The "better" op amps are all SMT 
parts but given that the YCCC preamp was a kit, I intentionally limited the 
selection to DIP-8 parts that kit builders could work with relatively easily on 
a PCB.  Not everyone is able to do a competent job soldering tiny SMT parts.

Within the universe of available RF op amps, tradeoffs must be made in terms of 
noise, linearity, and bandwidth.  The AD8055 is not the lowest noise part but 
it has excellent linearity and plenty of bandwidth for HF use.  At my QTH there 
is an AM BCB station 3 miles away, which makes it a somewhat challenging EMI 
environment.  The decision to run the op amp in a unity gain configuration 
comes down to linear dynamic range.  It is easy to design for more gain, but it 
is also easily demonstrated that you will begin to suffer in terms of unwanted 
intermods.  With the YCCC preamp, I get absolutely zero BCB intermods or 
distortion products in the 160m band at my QTH.

In general I do not like to use an outboard preamplifier between the output of 
the phased array combiner circuit and my receiver because it degrades the 
linear dynamic range of the system.  The YCCC system user's manual (Section
12.1) does specify several outboard preamps that could be used.  In a low EMI 
environment, I think they all work fine.  However, at my QTH, with the nearby 
AM BCB station, all of them, without exception, generate increased distortion 
and intermod, which I find unacceptable.  

It is always desirable to apply RF gain with a roofing filter in front, which 
is becoming common practice in high performance receivers.  With my K3S 
receiver, the use of a unity gain antenna feedpoint preamplifier is perfectly 
fine if you also turn on the preamp in the K3S.  This gives the best overall 
linear dynamic range with a preamplified short vertical system.
There is no loss in noise performance because the noise on 160 and 80 is 
totally dominated by atmospheric noise.  In measurements I made at my QTH, the 
internal noise of the YCCC preamp is about 10 dB lower than my daytime 
atmospheric noise on 160m when using a vertical about 20 feet high.

You must also consider the number of active elements in an amplified antenna 
array when evaluating overall system noise performance.  This is because the 
amplifier circuit noise power of all the feedpoint amplifiers is added together 
when the elements are phased up in a combiner.  If you have N elements in your 
array, the effective circuit noise contribution gets multiplied by N.  The YCCC 
array has 3 active elements at a time.  However, the YCCC design is somewhat 
unusual in that maximum RDF is achieved when the signals from the elements are 
combined in unequal ratios.  As a result the effective amplifier circuit noise 
contribution is less than 3 times (or 4.8
dB) the noise o

Re: Topband: Hi Z amplifiers for 160m

2020-03-12 Thread Chris Moulding
Thanks again for all the comments. Very interesting especially the 
reasoning behind the designs.


The device I've picked for my design is the LTC6228. This is a new 
device by Analog Devices that only came out late last year. The voltage 
noise is 0.88 uV/sqrt Hz and the current noise is 3 pA/sqrt Hz. Claimed 
output IP product performance is <-100 dBc at 4V peak to peak output.


The device is available in SOT-23 package from DigiKey and Mouser.

I'm planning to use the imminent coronavirus lockdown over here in the 
UK to get some PCB designs done.


73, Chris G4HYG

_
Searchable Archives: http://www.contesting.com/_topband - Topband Reflector


Re: Topband: Hi Z amplifiers for 160m

2020-03-11 Thread Lee STRAHAN
   Mike and all,
  Well stated Mike. It's been a long time since we have conversed. The 
modifier to this is when the signals coming into the combiner are no longer in 
phase or coherent. This as a result of delay lines and time of signal arrival 
at the many elements. Most often in our small portion of a wavelength low 
frequency arrays the combination of signals is subtractive to form a given 
pattern per array dimension. This then lowers the signal to noise ratio. It 
gets pretty complicated to arrive at a noise figure. The only way we have been 
able to do this with amplified arrays is to simulate the array in NEC being 
excited with a known signal many wavelengths away. We can extract the actual 
amplitude and phase of these multi element array signals and then combine them 
mathematically as you have done by example to arrive at a signal gain number 
from signal combination. The noise gain is easy. I say we because I have a 
retired very smart Ham friend in Finland that has helped me through this. It h
 as caused me to rethink gain distribution in some of my arrays.
Lee   K7TJR  OR

What matters is the signal-to-noise ratio (SNR). Take the canonical example of 
an ideal 2-port Wilkinson power combiner with in-phase coherent signals of 10 
Vrms applied to each input along with 1 Vrms random thermal noise from the 
respective element amplifiers applied to each input (i.e. each input signal has 
a 20*log(10 Vrms/1 Vrms) = 20dB SNR).

The power loss of the combiner is 3.01 dB [i.e. 10*log(2)], so voltage of each 
signal is attenuated by 1/sqrt(2) = 0.707. Thus, the components of each input 
signal appearing at the output are 7.07 Vrms each and
0.707 for each of the noise inputs.

The signal components add coherently at the combiner output yielding a total 
signal voltage of 14.14 Volts rms. The noise voltages are incoherent, so they 
add as root-sum-square at the output of the combiner. This yields a total noise 
voltage of sqrt(0.707^2 + 0.707^2) =
sqrt(1) = 1.0 Vrms. Thus, the combined noise voltage is unchanged, but the 
signal voltage goes up by sqrt(2).

The SNR of the combined output = 20*log(14.14Vrms/1Vrms) = 23dB, a 3dB 
improvement.

The same things holds for an ideal N-way combiner with equals noise components 
at each input. The noise power at the combined output equals the noise power of 
any of the equal input components (i.e. 0dB gain).

73, Mike W4EF..



On 3/11/2020 7:22 PM, Lee STRAHAN wrote:
> Hello John and all,
> Concerning the adding the noise in a typical array. If the noise was 
> coherent or exactly the same signal from each element/amp the summed noise 
> would indeed be 8 times. However circuit noise is always random and 
> incoherent which causes the summation to be a single noise power times the 
> square root of the number of elements assuming equal levels from each amp. In 
> the case of 8 elements 4.5 dB increase which is no small matter as well. In 
> the case of the three elements the noise summation would be about 2.4 dB 
> higher than a single element.
> Lee  K7TJR  OR
>
> As the designer of the YCCC high impedance feedpoint amplifier, let me 
> address some issues related to the design of the YCCC amplifier as well as 
> feedpoint amplifiers in general.  If you don't want to read a lot of 
> technical gobbledygook, please disregard this message.
>
> The YCCC uses an AD8055 RF amp as the gain element.  As Lee, K7TJF, points 
> out, there are most certainly better op amps out there.  However, the AD8055 
> was the "best" part I could find in a DIP-8 package.  The "better" op amps 
> are all SMT parts but given that the YCCC preamp was a kit, I intentionally 
> limited the selection to DIP-8 parts that kit builders could work with 
> relatively easily on a PCB.  Not everyone is able to do a competent job 
> soldering tiny SMT parts.
>
> Within the universe of available RF op amps, tradeoffs must be made in terms 
> of noise, linearity, and bandwidth.  The AD8055 is not the lowest noise part 
> but it has excellent linearity and plenty of bandwidth for HF use.  At my QTH 
> there is an AM BCB station 3 miles away, which makes it a somewhat 
> challenging EMI environment.  The decision to run the op amp in a unity gain 
> configuration comes down to linear dynamic range.  It is easy to design for 
> more gain, but it is also easily demonstrated that you will begin to suffer 
> in terms of unwanted intermods.  With the YCCC preamp, I get absolutely zero 
> BCB intermods or distortion products in the 160m band at my QTH.
>
> In general I do not like to use an outboard preamplifier between the 
> output of the phased array combiner circuit and my receiver because it 
> degrades the linear dynamic range of the system.  The YCCC system 
> user's manual (Section
> 12.1) does specify several outboard preamps that could be used.  In a low EMI 
> environment, I think they all work fine.  However, at my QTH, with the nearby 
> AM BCB station, all of 

Re: Topband: Hi Z amplifiers for 160m

2020-03-11 Thread Jim Brown

On 3/11/2020 9:39 PM, Michael Tope wrote:
The signal components add coherently at the combiner output yielding a 
total signal voltage of 14.14 Volts rms. The noise voltages are 
incoherent, so they add as root-sum-square at the output of the 
combiner. This yields a total noise voltage of sqrt(0.707^2 + 0.707^2) = 
sqrt(1) = 1.0 Vrms. Thus, the combined noise voltage is unchanged, but 
the signal voltage goes up by sqrt(2).


This is also why averaging in measurement systems and spectral displays 
improves their signal to noise ratio. As the number of averages is 
increased, signal to noise increases using the same math as above. I set 
averaging on my P3 to the max, the noise averages out, adjust the 
display reference level so that the noise is at the bottom of the 
display, causing even the weakest carriers (or CW) to be seen above the 
noise (and as faint traces in the waterfall).


We used averaging extensively in pro audio measurement systems, 
beginning with Time Delay Spectrometry around 1982. Which, by the way, 
was invented about ten years earlier by the late Richard Heyser, was was 
at JPL at the time. In this AES Paper, I buried a TDS sweep in a music 
track at a level that was nearly inaudible and fed it through a popular 
broadcast audio processor to study it's dynamic frequency response at 
high levels of compression. The sweep was nearly inaudible, the the 
system was able to recover it by 64X averaging, combined with TDS's 
inherent noise rejection.


http://k9yc.com/AESPaper-TDS.pdf

73, Jim K9YC
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Re: Topband: Hi Z amplifiers for 160m

2020-03-11 Thread Michael Tope
What matters is the signal-to-noise ratio (SNR). Take the canonical 
example of an ideal 2-port Wilkinson power combiner with in-phase 
coherent signals of 10 Vrms applied to each input along with 1 Vrms 
random thermal noise from the respective element amplifiers applied to 
each input (i.e. each input signal has a 20*log(10 Vrms/1 Vrms) = 20dB 
SNR).


The power loss of the combiner is 3.01 dB [i.e. 10*log(2)], so voltage 
of each signal is attenuated by 1/sqrt(2) = 0.707. Thus, the components 
of each input signal appearing at the output are 7.07 Vrms each and 
0.707 for each of the noise inputs.


The signal components add coherently at the combiner output yielding a 
total signal voltage of 14.14 Volts rms. The noise voltages are 
incoherent, so they add as root-sum-square at the output of the 
combiner. This yields a total noise voltage of sqrt(0.707^2 + 0.707^2) = 
sqrt(1) = 1.0 Vrms. Thus, the combined noise voltage is unchanged, but 
the signal voltage goes up by sqrt(2).


The SNR of the combined output = 20*log(14.14Vrms/1Vrms) = 23dB, a 3dB 
improvement.


The same things holds for an ideal N-way combiner with equals noise 
components at each input. The noise power at the combined output equals 
the noise power of any of the equal input components (i.e. 0dB gain).


73, Mike W4EF..



On 3/11/2020 7:22 PM, Lee STRAHAN wrote:

Hello John and all,
Concerning the adding the noise in a typical array. If the noise was 
coherent or exactly the same signal from each element/amp the summed noise 
would indeed be 8 times. However circuit noise is always random and incoherent 
which causes the summation to be a single noise power times the square root of 
the number of elements assuming equal levels from each amp. In the case of 8 
elements 4.5 dB increase which is no small matter as well. In the case of the 
three elements the noise summation would be about 2.4 dB higher than a single 
element.
Lee  K7TJR  OR

As the designer of the YCCC high impedance feedpoint amplifier, let me address 
some issues related to the design of the YCCC amplifier as well as feedpoint 
amplifiers in general.  If you don't want to read a lot of technical 
gobbledygook, please disregard this message.

The YCCC uses an AD8055 RF amp as the gain element.  As Lee, K7TJF, points out, there are most 
certainly better op amps out there.  However, the AD8055 was the "best" part I could find 
in a DIP-8 package.  The "better" op amps are all SMT parts but given that the YCCC 
preamp was a kit, I intentionally limited the selection to DIP-8 parts that kit builders could work 
with relatively easily on a PCB.  Not everyone is able to do a competent job soldering tiny SMT 
parts.

Within the universe of available RF op amps, tradeoffs must be made in terms of 
noise, linearity, and bandwidth.  The AD8055 is not the lowest noise part but 
it has excellent linearity and plenty of bandwidth for HF use.  At my QTH there 
is an AM BCB station 3 miles away, which makes it a somewhat challenging EMI 
environment.  The decision to run the op amp in a unity gain configuration 
comes down to linear dynamic range.  It is easy to design for more gain, but it 
is also easily demonstrated that you will begin to suffer in terms of unwanted 
intermods.  With the YCCC preamp, I get absolutely zero BCB intermods or 
distortion products in the 160m band at my QTH.

In general I do not like to use an outboard preamplifier between the output of 
the phased array combiner circuit and my receiver because it degrades the 
linear dynamic range of the system.  The YCCC system user's manual (Section
12.1) does specify several outboard preamps that could be used.  In a low EMI 
environment, I think they all work fine.  However, at my QTH, with the nearby 
AM BCB station, all of them, without exception, generate increased distortion 
and intermod, which I find unacceptable.

It is always desirable to apply RF gain with a roofing filter in front, which 
is becoming common practice in high performance receivers.  With my K3S 
receiver, the use of a unity gain antenna feedpoint preamplifier is perfectly 
fine if you also turn on the preamp in the K3S.  This gives the best overall 
linear dynamic range with a preamplified short vertical system.
There is no loss in noise performance because the noise on 160 and 80 is 
totally dominated by atmospheric noise.  In measurements I made at my QTH, the 
internal noise of the YCCC preamp is about 10 dB lower than my daytime 
atmospheric noise on 160m when using a vertical about 20 feet high.

You must also consider the number of active elements in an amplified antenna 
array when evaluating overall system noise performance.  This is because the 
amplifier circuit noise power of all the feedpoint amplifiers is added together 
when the elements are phased up in a combiner.  If you have N elements in your 
array, the effective circuit noise contribution gets multiplied by N.  The YCCC 
array has 3 active 

Re: Topband: Hi Z amplifiers for 160m

2020-03-11 Thread GEORGE WALLNER

Here is an example at Digikey:

ACX1545-ND

Expensive, but...

73,
George



On Wed, 11 Mar 2020 13:33:08 -0400
 DXer  wrote:

>>>Use an F connector (a high quality one that can be torqued.)

Can you point to a place that sells them. I became a 'fan' of F termination, 
but have recently had second thoughts because of the bulkhead connector's 
quality.

Thanks and 73.

Vince, VA3VF
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Re: Topband: Hi Z amplifiers for 160m

2020-03-11 Thread Lee STRAHAN
   Hello John and all,
   Concerning the adding the noise in a typical array. If the noise was 
coherent or exactly the same signal from each element/amp the summed noise 
would indeed be 8 times. However circuit noise is always random and incoherent 
which causes the summation to be a single noise power times the square root of 
the number of elements assuming equal levels from each amp. In the case of 8 
elements 4.5 dB increase which is no small matter as well. In the case of the 
three elements the noise summation would be about 2.4 dB higher than a single 
element.
Lee  K7TJR  OR

As the designer of the YCCC high impedance feedpoint amplifier, let me address 
some issues related to the design of the YCCC amplifier as well as feedpoint 
amplifiers in general.  If you don't want to read a lot of technical 
gobbledygook, please disregard this message.

The YCCC uses an AD8055 RF amp as the gain element.  As Lee, K7TJF, points out, 
there are most certainly better op amps out there.  However, the AD8055 was the 
"best" part I could find in a DIP-8 package.  The "better" op amps are all SMT 
parts but given that the YCCC preamp was a kit, I intentionally limited the 
selection to DIP-8 parts that kit builders could work with relatively easily on 
a PCB.  Not everyone is able to do a competent job soldering tiny SMT parts.

Within the universe of available RF op amps, tradeoffs must be made in terms of 
noise, linearity, and bandwidth.  The AD8055 is not the lowest noise part but 
it has excellent linearity and plenty of bandwidth for HF use.  At my QTH there 
is an AM BCB station 3 miles away, which makes it a somewhat challenging EMI 
environment.  The decision to run the op amp in a unity gain configuration 
comes down to linear dynamic range.  It is easy to design for more gain, but it 
is also easily demonstrated that you will begin to suffer in terms of unwanted 
intermods.  With the YCCC preamp, I get absolutely zero BCB intermods or 
distortion products in the 160m band at my QTH.

In general I do not like to use an outboard preamplifier between the output of 
the phased array combiner circuit and my receiver because it degrades the 
linear dynamic range of the system.  The YCCC system user's manual (Section
12.1) does specify several outboard preamps that could be used.  In a low EMI 
environment, I think they all work fine.  However, at my QTH, with the nearby 
AM BCB station, all of them, without exception, generate increased distortion 
and intermod, which I find unacceptable.  

It is always desirable to apply RF gain with a roofing filter in front, which 
is becoming common practice in high performance receivers.  With my K3S 
receiver, the use of a unity gain antenna feedpoint preamplifier is perfectly 
fine if you also turn on the preamp in the K3S.  This gives the best overall 
linear dynamic range with a preamplified short vertical system.
There is no loss in noise performance because the noise on 160 and 80 is 
totally dominated by atmospheric noise.  In measurements I made at my QTH, the 
internal noise of the YCCC preamp is about 10 dB lower than my daytime 
atmospheric noise on 160m when using a vertical about 20 feet high.

You must also consider the number of active elements in an amplified antenna 
array when evaluating overall system noise performance.  This is because the 
amplifier circuit noise power of all the feedpoint amplifiers is added together 
when the elements are phased up in a combiner.  If you have N elements in your 
array, the effective circuit noise contribution gets multiplied by N.  The YCCC 
array has 3 active elements at a time.  However, the YCCC design is somewhat 
unusual in that maximum RDF is achieved when the signals from the elements are 
combined in unequal ratios.  As a result the effective amplifier circuit noise 
contribution is less than 3 times (or 4.8
dB) the noise of a single amplifier.  In fact because of the unequal combining 
ratios, the actual effective noise goes up by a bit less than 2 dB compared to 
a single amplifier.  An array like the Hi-Z array with 8 active elements 
combines the elements in equal proportion so the effective amplifier circuit 
noise of the system is 8 times (or 9 dB) higher than the noise of a single 
amplifier.  For this reason, the YCCC array can tolerate noisier amplifiers 
without degrading system noise performance.  The objective is to keep circuit 
noise well under atmospheric noise.

On the subject of op amp noise specs, you must consider *both* input voltage 
noise and input current noise because, in general, both contribute to the total 
output amplifier noise.  It is not good enough to pick an op amp with low input 
voltage noise without also considering the input current noise.
For a good noise analysis, download a copy of the datasheet for the CLC425 op 
amp:  http://www.elektronikjk.pl/elementy_czynne/IC/CLC425.pdf.  Refer to pages 
8-10.  (The CLC425 is a very good RF op amp but has been obsoleted by 

Re: Topband: Hi Z amplifiers for 160m

2020-03-11 Thread John Kaufmann via Topband
As the designer of the YCCC high impedance feedpoint amplifier, let me
address some issues related to the design of the YCCC amplifier as well as
feedpoint amplifiers in general.  If you don't want to read a lot of
technical gobbledygook, please disregard this message.

The YCCC uses an AD8055 RF amp as the gain element.  As Lee, K7TJF, points
out, there are most certainly better op amps out there.  However, the AD8055
was the "best" part I could find in a DIP-8 package.  The "better" op amps
are all SMT parts but given that the YCCC preamp was a kit, I intentionally
limited the selection to DIP-8 parts that kit builders could work with
relatively easily on a PCB.  Not everyone is able to do a competent job
soldering tiny SMT parts.

Within the universe of available RF op amps, tradeoffs must be made in terms
of noise, linearity, and bandwidth.  The AD8055 is not the lowest noise part
but it has excellent linearity and plenty of bandwidth for HF use.  At my
QTH there is an AM BCB station 3 miles away, which makes it a somewhat
challenging EMI environment.  The decision to run the op amp in a unity gain
configuration comes down to linear dynamic range.  It is easy to design for
more gain, but it is also easily demonstrated that you will begin to suffer
in terms of unwanted intermods.  With the YCCC preamp, I get absolutely zero
BCB intermods or distortion products in the 160m band at my QTH.

In general I do not like to use an outboard preamplifier between the output
of the phased array combiner circuit and my receiver because it degrades the
linear dynamic range of the system.  The YCCC system user's manual (Section
12.1) does specify several outboard preamps that could be used.  In a low
EMI environment, I think they all work fine.  However, at my QTH, with the
nearby AM BCB station, all of them, without exception, generate increased
distortion and intermod, which I find unacceptable.  

It is always desirable to apply RF gain with a roofing filter in front,
which is becoming common practice in high performance receivers.  With my
K3S receiver, the use of a unity gain antenna feedpoint preamplifier is
perfectly fine if you also turn on the preamp in the K3S.  This gives the
best overall linear dynamic range with a preamplified short vertical system.
There is no loss in noise performance because the noise on 160 and 80 is
totally dominated by atmospheric noise.  In measurements I made at my QTH,
the internal noise of the YCCC preamp is about 10 dB lower than my daytime
atmospheric noise on 160m when using a vertical about 20 feet high.

You must also consider the number of active elements in an amplified antenna
array when evaluating overall system noise performance.  This is because the
amplifier circuit noise power of all the feedpoint amplifiers is added
together when the elements are phased up in a combiner.  If you have N
elements in your array, the effective circuit noise contribution gets
multiplied by N.  The YCCC array has 3 active elements at a time.  However,
the YCCC design is somewhat unusual in that maximum RDF is achieved when the
signals from the elements are combined in unequal ratios.  As a result the
effective amplifier circuit noise contribution is less than 3 times (or 4.8
dB) the noise of a single amplifier.  In fact because of the unequal
combining ratios, the actual effective noise goes up by a bit less than 2 dB
compared to a single amplifier.  An array like the Hi-Z array with 8 active
elements combines the elements in equal proportion so the effective
amplifier circuit noise of the system is 8 times (or 9 dB) higher than the
noise of a single amplifier.  For this reason, the YCCC array can tolerate
noisier amplifiers without degrading system noise performance.  The
objective is to keep circuit noise well under atmospheric noise.

On the subject of op amp noise specs, you must consider *both* input voltage
noise and input current noise because, in general, both contribute to the
total output amplifier noise.  It is not good enough to pick an op amp with
low input voltage noise without also considering the input current noise.
For a good noise analysis, download a copy of the datasheet for the CLC425
op amp:  http://www.elektronikjk.pl/elementy_czynne/IC/CLC425.pdf.  Refer to
pages 8-10.  (The CLC425 is a very good RF op amp but has been obsoleted by
newer parts).  I put the noise equations into an Excel spreadsheet, which
allowed me to compare many different op amps in terms of total noise
performance, using their input current noise and voltage noise specs.

Not all op amps publish specs on linearity.  It is safe to assume that if no
specs are given, the linearity is not particularly outstanding.  Look for
harmonic distortion (HD2 and HD3) as well as TOI (third-order intercept)
data.  You do have to be careful in interpreting the data because the
linearity is directly tied to the amplifier gain configuration.

If I were to recommend a particularly outstanding RF op amp, it would 

Re: Topband: Hi Z amplifiers for 160m

2020-03-11 Thread Lloyd - N9LB
Lee,
Can you recommend an improved device to replace/upgrade the Analog Devices #
AD8055AN chip?  
Any chance it would be a "drop-in replacement" ( pin-for-pin ) ?
I've got nine of the YCCC that I'd like to upgrade.
Or maybe I should just wait for Chris to complete his whole new design.
73
Lloyd - N9LB

-Original Message-
From: Topband [mailto:topband-bounces+lloydberg=tds@contesting.com] On
Behalf Of Lee STRAHAN
Sent: Wednesday, March 11, 2020 12:17 PM
To: topband@contesting.com
Subject: Re: Topband: Hi Z amplifiers for 160m

Greetings all,
   George has some very pertinent points here and only on one point I will
disagree. What a Hi-Z amplifier needs to do is dependent on your aspirations
of the size and quantity of elements you decide to use. The combiner losses
will dictate what you must do at the element end of an array for an
amplifier. Let me clear one thing up. The YCCC amplifier is not a unity gain
amplifier. It has a 6 dB loss due to its output impedance of around 75 ohms.
Thus the evolution of what I called the +6 amps 6 or 7 years ago that indeed
have unity gain and still have a 75 ohm output impedance. A significant
reduction in the noise figure of an array with a lossy combiner.
   If ones aspirations are only to use a simple array like the YCCC then the
operational amplifier versions seem to fill the bill, but don't expect then
to apply the same amplifiers as you build arrays for higher and higher RDF.
And, there are much better amplifiers available to replace the 8055 if I
remember the YCCC part number correctly. The 8055 has like 4nV/root Hz noise
while some of the new ones get down to 1 nV/root Hz noise a very significant
improvement.
   I could bore you all to distraction with other fine points that Hi-Z amps
need as specifications. It may not meet the eye but that is why performance
comes at a price.

Lee   K7TJR
Hi-Z Antennas

Chris,
Assuming a trans-impedance amplifier, "unity gain" is enough (with
reasonable size elements). Noise and IP3 are far more important. Lightning
and surge immunity are also important. Also, isolate the amp from common
mode noise travelling on the feed-line. Filter the power supply well. Use an
F connector (a high quality one that can be torqued.) GL and 73, George,
AA7JV/C6AGU

On Wed, 11 Mar 2020 11:33:34 +
  Chris Moulding  wrote:
> As well as being a radio amateur (G4HYG) I also run a small business
designing and making radio equipment (Cross Country Wireless).
>
> Recently I've been asked by a radio contest group to see if I can redesign
the YCCC Hi Z amplifier using modern components and using similar mounting
arrangements to our Loop Antenna Amplifier.
>
> The first prototype using surface mount components is working well.
>
> So far I've not build an array of antennas but that will come later when
the production boards arrive.
>
> The prototype uses a unity voltage gain amplifier and a BNC connector.
>
> I've a couple of questions for others on the list with experience of
running vertical receive arrays:
>
> Is a unity voltage gain amplifier OK or do you think it needs more gain
for long coax runs?
>
> At present I'm using a BNC male connector for the output. Would an F type
connector be more compatible with existing antenna arrays.
>
> 73, Chris G4HYG
>
> _
> Searchable Archives: http://www.contesting.com/_topband - Topband 
> Reflector

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Re: Topband: Hi Z amplifiers for 160m

2020-03-11 Thread Chris Moulding

Thanks for all the very helpful replies and suggestions.

I'll change the BNC connector to a 4 hole F connector with 75 ohm output.

The design already has a 20 kA gas discharge tube and DC biased diode 
limiter for lightning and surge protection. It also has an optional (by 
internal link) diode limiter on the output so that it can be used by 
"weak" SDR receivers such as the SDRPlay RSP series that cannot take 
high RF levels.


I agree with the comment on adding a common mode choke on the coax 
output. The amplifier device I'm using has very low noise so it needs 
extra common mode isolation to allow use at very RF quiet locations.


I'm planning to take a trip to the nearest beach this weekend to try the 
prototype in a very low noise location.


73, Chris G4HYG

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Re: Topband: Hi Z amplifiers for 160m

2020-03-11 Thread Lee STRAHAN
  Mouser 601- 25-7630  or  601-25-7660
[Lee  K7TJR] 

 >>>Use an F connector (a high quality one that can be torqued.)

Can you point to a place that sells them. I became a 'fan' of F termination, 
but have recently had second thoughts because of the bulkhead connector's 
quality.

Thanks and 73.

Vince, VA3VF
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Re: Topband: Hi Z amplifiers for 160m

2020-03-11 Thread Jim Brown

On 3/11/2020 6:28 AM, GEORGE WALLNER wrote:
Assuming a trans-impedance amplifier, "unity gain" is enough (with 
reasonable size elements). Noise and IP3 are far more important. 
Lightning and surge immunity are also important. Also, isolate the amp 
from common mode noise travelling on the feed-line. Filter the power 
supply well. Use an F connector (a high quality one that can be torqued.)


Agreed, but I would add power on the coax.

73, Jim K9YC
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Re: Topband: Hi Z amplifiers for 160m

2020-03-11 Thread Lee STRAHAN
Greetings all,
   George has some very pertinent points here and only on one point I will 
disagree. What a Hi-Z amplifier needs to do is dependent on your aspirations of 
the size and quantity of elements you decide to use. The combiner losses will 
dictate what you must do at the element end of an array for an amplifier. Let 
me clear one thing up. The YCCC amplifier is not a unity gain amplifier. It has 
a 6 dB loss due to its output impedance of around 75 ohms. Thus the evolution 
of what I called the +6 amps 6 or 7 years ago that indeed have unity gain and 
still have a 75 ohm output impedance. A significant reduction in the noise 
figure of an array with a lossy combiner.
   If ones aspirations are only to use a simple array like the YCCC then the 
operational amplifier versions seem to fill the bill, but don't expect then to 
apply the same amplifiers as you build arrays for higher and higher RDF. And, 
there are much better amplifiers available to replace the 8055 if I remember 
the YCCC part number correctly. The 8055 has like 4nV/root Hz noise while some 
of the new ones get down to 1 nV/root Hz noise a very significant improvement.
   I could bore you all to distraction with other fine points that Hi-Z amps 
need as specifications. It may not meet the eye but that is why performance 
comes at a price.

Lee   K7TJR
Hi-Z Antennas




Chris,
Assuming a trans-impedance amplifier, "unity gain" is enough (with reasonable 
size elements). Noise and IP3 are far more important. Lightning and surge 
immunity are also important. Also, isolate the amp from common mode noise 
travelling on the feed-line. Filter the power supply well. Use an F connector 
(a high quality one that can be torqued.) GL and 73, George, AA7JV/C6AGU

On Wed, 11 Mar 2020 11:33:34 +
  Chris Moulding  wrote:
> As well as being a radio amateur (G4HYG) I also run a small business 
> designing and making radio equipment (Cross Country Wireless).
>
> Recently I've been asked by a radio contest group to see if I can redesign 
> the YCCC Hi Z amplifier using modern components and using similar mounting 
> arrangements to our Loop Antenna Amplifier.
>
> The first prototype using surface mount components is working well.
>
> So far I've not build an array of antennas but that will come later when the 
> production boards arrive.
>
> The prototype uses a unity voltage gain amplifier and a BNC connector.
>
> I've a couple of questions for others on the list with experience of running 
> vertical receive arrays:
>
> Is a unity voltage gain amplifier OK or do you think it needs more gain for 
> long coax runs?
>
> At present I'm using a BNC male connector for the output. Would an F type 
> connector be more compatible with existing antenna arrays.
>
> 73, Chris G4HYG
>
> _
> Searchable Archives: http://www.contesting.com/_topband - Topband 
> Reflector

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Re: Topband: Hi Z amplifiers for 160m

2020-03-11 Thread RT Clay
Chris,

I just finished making my own set of amplifiers derived from the YCCC design 
but using SMD components. I used an AD8045 (SOIC-8 size) instead of the 8055 
and added a voltage regulator.

They have replaced a set of the original Hi-Z amps (the ones in the black 
mini-boxes with metal covers) in my hexagonal array. I don't have a way to 
directly compare the performance of the new amps with the old ones, but so far 
they seem to work well.

Tor N4OGW





On Wednesday, March 11, 2020, 8:29:33 AM CDT, GEORGE WALLNER 
 wrote: 





Chris,
Assuming a trans-impedance amplifier, "unity gain" is enough (with 
reasonable size elements). Noise and IP3 are far more important. Lightning 
and surge immunity are also important. Also, isolate the amp from common 
mode noise travelling on the feed-line. Filter the power supply well. Use an 
F connector (a high quality one that can be torqued.)
GL and 73,
George,
AA7JV/C6AGU

On Wed, 11 Mar 2020 11:33:34 +
  Chris Moulding  wrote:
> As well as being a radio amateur (G4HYG) I also run a small business 
> designing and making radio equipment (Cross Country Wireless).
>
> Recently I've been asked by a radio contest group to see if I can redesign 
> the YCCC Hi Z amplifier using modern components and using similar mounting 
> arrangements to our Loop Antenna Amplifier.
>
> The first prototype using surface mount components is working well.
>
> So far I've not build an array of antennas but that will come later when the 
> production boards arrive.
>
> The prototype uses a unity voltage gain amplifier and a BNC connector.
>
> I've a couple of questions for others on the list with experience of running 
> vertical receive arrays:
>
> Is a unity voltage gain amplifier OK or do you think it needs more gain for 
> long coax runs?
>
> At present I'm using a BNC male connector for the output. Would an F type 
> connector be more compatible with existing antenna arrays.
>
> 73, Chris G4HYG
>
> _
> Searchable Archives: http://www.contesting.com/_topband - Topband Reflector


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Re: Topband: Hi Z amplifiers for 160m

2020-03-11 Thread GEORGE WALLNER

Chris,
Assuming a trans-impedance amplifier, "unity gain" is enough (with 
reasonable size elements). Noise and IP3 are far more important. Lightning 
and surge immunity are also important. Also, isolate the amp from common 
mode noise travelling on the feed-line. Filter the power supply well. Use an 
F connector (a high quality one that can be torqued.)

GL and 73,
George,
AA7JV/C6AGU

On Wed, 11 Mar 2020 11:33:34 +
 Chris Moulding  wrote:

As well as being a radio amateur (G4HYG) I also run a small business designing 
and making radio equipment (Cross Country Wireless).

Recently I've been asked by a radio contest group to see if I can redesign the 
YCCC Hi Z amplifier using modern components and using similar mounting 
arrangements to our Loop Antenna Amplifier.

The first prototype using surface mount components is working well.

So far I've not build an array of antennas but that will come later when the 
production boards arrive.

The prototype uses a unity voltage gain amplifier and a BNC connector.

I've a couple of questions for others on the list with experience of running 
vertical receive arrays:

Is a unity voltage gain amplifier OK or do you think it needs more gain for 
long coax runs?

At present I'm using a BNC male connector for the output. Would an F type 
connector be more compatible with existing antenna arrays.

73, Chris G4HYG

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Searchable Archives: http://www.contesting.com/_topband - Topband Reflector