Topband: Hi Z amplifiers for 160m (LONG)

Michael Tope W4EF at dellroy.com
Fri Mar 13 07:34:26 EDT 2020


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 of the main lobe 
goes up by 20*log(2) = 6dB. That would imply that the gain of the array 
has gone up by 6dB and that the azimuth beamwidth of the main lobe has 
gone down by a factor of 4. However, if you look at gain of a linear 
broadside array when you double the number of elements (assuming 
constant element spacing), the gain goes up by at most 3dB. If the 
average gain for the isotropic atmospheric noise is a constant 0dB, then 
signal-of-interest in the antenna bore site can only go up by at most 
3dB relative to the atmospheric noise. But the mathematical sum of the 
components of the signal-of-interest have gone up 6dB, so the 
mathematical sum of the components of the isotropic atmospheric noise 
have to go up by at least 3dB.

I think I have this right, John, but feel free to shoot holes in it if I 
don't. I know thinking about it made my head hurt.

73, Mike W4EF........

On 3/12/2020 4:37 PM, John Kaufmann via Topband wrote:
> 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.net at contesting.com] On Behalf
> Of Michael Tope
> Sent: Thursday, March 12, 2020 4:37 PM
> To: topband at 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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