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Re: Steve ugly-build LZ1AQ using MPS2222 sweeps uploaded to Photos
Chavdar,
?
In order to "complicate" this matter more.
The current theory about usage test simulators for receiving antennae postulates:
"these equivalent circuits ( Thevenin and Norton ) may be applicable to transmit system but not suitable for receive antenna system since the receiving antenna is actually a constant power source.
An accurate model for a receiving antenna should be a power source rather than a voltage or a current source".
Thus, the current NEC or EZNEC tools are for birds unless we are modeling transmit anteenae?
?
Raphael |
Re: Steve ugly-build LZ1AQ using MPS2222 sweeps uploaded to Photos
To
Chavdar
: Even Balanis in his treatment of traveling wave antennas makes the comment that the small loop can be treated with similar arguments which address the TW antenna.? I didn't go through the math as I didn't want a headache, but I have to believe him.? Dave - W?LEV On Mon, Oct 7, 2024 at 7:33?PM §é§Ñ§Ó§Õ§Ñ§â §Ý§Ö§Ó§Ü§à§Ó via <lz1aq=[email protected]> wrote:
-- Dave - W?LEV |
Re: Steve ugly-build LZ1AQ using MPS2222 sweeps uploaded to Photos
¿ªÔÆÌåÓýHi Chavdar, ? My acknowledgement about transformation from Thevenin to Norton are as follow, based on equal power transform :
? In your previous work where you depicted ?as an example ?Norton's model for loop antenna with 3 ohm load the diagram does not include any 1 Kohm resistors. That is right representation of equivalent Norton's model but your test simulator does not follow that¡ Again these 1 Kohm resistors destroy Norton's model. For practical reasons building simulator to test active loop antennas with any amplifiers should be used either signal induced technique like Martin proposed and used or signal injected method, using a ?dummy aerial model based on Thevenin's ckt. In other words, in your simulator are Thevenin's voltage source with elements of Northon's LCR and load¡because of those resistors. ? ? Regards, ? Raphael ? ? From: [email protected] <[email protected]> On Behalf Of ?????? ?????? via groups.io
Sent: Monday, October 7, 2024 2:04 PM To: [email protected] Subject: Re: [loopantennas] Steve ugly-build LZ1AQ using MPS2222 sweeps uploaded to Photos ? ? Hi Raphael, I am sorry , ignore previous message #20287 it is wrong. The? Current source resistances must be much higher than the anticipated LOAD resistance ,? so 2 KOm which are used are 20 times higher than the maximal expected input impedance of the amplifier (e.g. 100 ohms with input filter at highest frequency) .? NEC data show that the loop deliver? constant current in very wide frequency range.?? So we will get frequency response of the loop amplifier if we assure constant current at its input . This is very simple? - even we can get almost correct frequency response without inductance at all ¨C just we must feed the input with constant current .? 2 KOm will give current 5% less at 100 Ohm load? compared to 6 Ohms load.? To increase the accuracy we can use e.g. 20 K? and the error will be 0.5% .? The problem is that 20 K will reduce the signal input substantially? with existing signal generators? and also parasitic capacitances of the resistors cannot be ignored e.g.? 1 pF at 30 MHz? = 5.5 kOm.? The parallel? inductance will go into action at low frequencies where its impedance is comparable to R load. ? Again: the internal resistance of the current source must be much higher than the anticipated? R load (not the? impedance of inductance) .?? Chavdar |
Re: Steve ugly-build LZ1AQ using MPS2222 sweeps uploaded to Photos
To Dan, When the loop length is ?close to the wavelength there are standing waves ?- in your last data? from NEC (thanks for that) the ratio Imax/Imin is? 1.4 ¨C the max. ?current ?being at the loop side and min. current at the load. I plotted ?the current vs. segment# and I can ?see a typical ?standing wave pattern. The current variation is not very large so with fixed current source measurement setup we can expect even at these frequencies to get a glimpse of the frequency response of the antenna factor . ?? ? About loop as transmission line Yes, I think that the loop can be considered as a ?transmission line. ?But since the loop is so short compared to the wavelength ?we cannot observe standing wave patterns ?at low frequencies when loop is shorted or opened. ?For me closed and open loop are both standing wave cases. ?By the way if we terminate one side of the small loop with? characteristic impedance of this transmission line ??we will get something? like traveling wave antenna?? - ??Flag antenna ?is a typical example. Flag becomes unidirectional when load R = Zc of this ?tr. line. ?But I will stop here ¨C my knowledge in antenna theory is very very limited, I am just a standard NEC user. ? Chavdar lz1aq |
ADDRESSING SKIN DEPTH
Addressing skin depth: For copper: Conductivity:? ¦Ò = 6.30 E +7 S/m Resistivity:? 1/¦Ò = 1.60 E -8 ¦¸m Skin Depth: 2.47 E-5 m Frequency of following analysis:? 7.000 MHz For the above, refer to:? ? ??????????????????????? and ? ?? From the same reference the resistance due to skin depth can be calculated:? ? ? ? For my 36-inch diameter loop made of 0.5-in copper tubing (and converting everything to the MKS system) the resistance due only to skin depth comes out to be: ? ? ? ? ? ? ? ? ? ? ? ? ? ? ? ?? 0.0952 ohms At 1 MHz, this will be "roughy" 0.1X of that value and at 100 MHz, this will be "roughly" 10X of that value.?? These are only roughly.? But it does indicate some frequency dependance. However, in all cases from 1 MHz through 100 MHz, the added resistance is considerably greater than the DC or radiation resistance.? So, I'd conclude current in the loop should vary with frequency as a result of skin depth.? In addition, the variation between "DC" and 30 MHz should be only a factor of "roughly" 10.? Interestingly this goes against the EZNEC analysis presented earlier.? It showed current pretty much constant even up to resonance.? Guess someone needs to actually measure current as a function of frequency with a constant RF input level.?? I can short my 36-inch tuned loop to do that.? Anyone else want to contribute in this measurement???? Dave - W?LEV |
SOME MEASUREMENTS of a SML - 2.0
Addressing skin depth: For copper: Conductivity:? ¦Ò = 6.30 E +7 S/m Resistivity:? 1/¦Ò = 1.60 E -8 ¦¸m Skin Depth: 2.47 E-5 m Frequency of following analysis:? 7.000 MHz For the above, refer to:? ? ??????????????????????? and ? ?? From the same reference the resistance due to skin depth can be calculated:? ? ? ? For my 36-inch diameter loop made of 0.5-in copper tubing (and converting everything to the MKS system) the resistance due only to skin depth comes out to be: ? ? ? ? ? ? ? ? ? ? ? ? ? ? ? ?? 0.0952 ohms At 1 MHz, this will be "roughy" 0.1X of that value and at 100 MHz, this will be "roughly" 10X of that value.?? These are only roughly.? But it does indicate some frequency dependance. However, in all cases from 1 MHz through 100 MHz, the added resistance is considerably greater than the DC or radiation resistance.? So, I'd conclude current in the loop should vary with frequency as a result of skin depth.? In addition, the variation between "DC" and 30 MHz should be only a factor of "roughly" 10.? Interesting this goes against the EZNEC analysis presented earlier.?? Guess someone needs to actually measure current as a function of frequency with a constant RF input level.?? I can short my 36-inch tuned loop to do that.? Anyone else want to contribute in this measurement???? Dave - W?LEV? ? ? ? ? ? ? ? ? ? ? -- Dave - W?LEV |
Re: Steve ugly-build LZ1AQ using MPS2222 sweeps uploaded to Photos
?Hi Raphael, I am sorry , ignore previous message #20287 it is wrong. ?The ?Current source resistances must be much higher than the anticipated LOAD resistance , ?so 2 KOm which are used are 20 times higher than the maximal expected input impedance of the amplifier (e.g. 100 ohms with input filter at highest frequency) .? NEC data show that the loop deliver ?constant current in very wide frequency range. ??So we will get frequency response of the loop amplifier if we assure constant current at its input . This is very simple? - even we can get almost correct frequency response without inductance at all ¨C just we must feed the input with constant current . ?2 KOm will give current 5% less at 100 Ohm load ?compared to 6 Ohms load.? To increase the accuracy we can use e.g. 20 K? and the error will be 0.5% .? The problem is that 20 K will reduce the signal input substantially? with existing signal generators? and also parasitic capacitances of the resistors cannot be ignored e.g. ?1 pF at 30 MHz? = 5.5 kOm. ?The parallel ?inductance will go into action at low frequencies where its impedance is comparable to R load. ? Again: the internal resistance of the current source must be much higher than the anticipated ?R load (not the? impedance of inductance) . ?? Chavdar |
Re: MLA-30+, the story continues!
#Small_receiving_loops_RX-only
I would agree with Fred.
?
Despite what many articles and videos on the internet may suggest, including many professional ones, it is not easy to make practical and repeatable IMD measurements, especially at the IMD levels we are interested in.
?
I've struggled with this, and have my own built band pass and notch filters and crystal oscillator based test sources. But even things like dirty connectors, especially things like BNC test leads, can cause results to vary considerably.
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The first step is to check that your IMD test rig is capable of producing results that are at least 10dB better than the device you are testing. Even this isn't really good enough, but it's something to aim for. Then try measuring known devices, such as the Mini-Circuits PGA-103+ or GALI-74+.
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I've always found these perform pretty closely to their published specification, and I tend to use one as a sanity check, before I try measuring something else.
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Regards,
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Martin
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On Mon, Oct 7, 2024 at 04:19 PM, Fred M wrote:
the Signal generators Output Stages and even the Splitter with its Ferrite nonlinearity are also a source of Intermodulation which limit your measurement dynamics. Again, IP measurement of high IPs is demanding, dont't fall in your own traps. |
Re: MLA-30+, the story continues!
#Small_receiving_loops_RX-only
Hi Chin-Leong Lim ( the first time that i got right)
?
Besides the TinySA, whose own IP3 is 17 dBm at best (thats your absolute limitation), the Signal generators Output Stages and even the Splitter with its Ferrite nonlinearity are also a source of Intermodulation which limit your measurement dynamics. Again, IP measurement of high IPs is demanding, dont't fall in your own traps.
?
regards, Fred |
Re: Steve ugly-build LZ1AQ using MPS2222 sweeps uploaded to Photos
Dave,
?
As far my acknowledgement of usung VNA for measurement small impedances or resistors of 0.1 ohms value allows to reach about 0.04 % accuracy.?
However, for low resistance values that you mentioned shall be used a different method by connecting between CH0 and CH1 ports of VNA ( so called I- method by measiring S21 or current through your resistor). This technique has 0.01 %.
I guess you can measure ohmic resistors not radiation resistance
?
Raphael
? |
Re: Steve ugly-build LZ1AQ using MPS2222 sweeps uploaded to Photos
Chavdar,
?
I am sorry I forgot to mention another point. I can understand why you have been using Norton equivalent circuit for a prove how great works active small loop antenna in short current mode. The low resistive input of amplifier cancels the reactive influence of loop antenna and regardless what series arms in simulator are used - we will get flat ( frequency independent ) frequency response.
On other hand using Thevenin circuit it does not? prove the above said because you do not have a control mechanism allowing the source voltage to follow the frequency in acordance to Faraday' law of induced current. So, the frequency response is not "frequency flat" ( indepenent from frequency ) more but skewed down with the frequency increase.
My understanding has been usage of dummy aerial circuit with a receiver in our technical business always? ignores that applied test signal shall follow Faraday's law.?
?
?
Raphael? |
Re: Steve ugly-build LZ1AQ using MPS2222 sweeps uploaded to Photos
Hi Chavdar,
?
With all my respect to you spending a lot of time exploring loop antennae with amplifiers I am in disagreement with your "simulator" design.
For all practical means we have been using as a source voltage generators, thus for testing active antennae their equivalent circuit? should be Thevenin's circuit.
Yes, we can transform from Thevenin to Norton circuit but it is pure theoretical move.
We agreed that value of current source in Norton's is related to voltage source in Thevenin's as I sc = V oc / Z ant because of equal power condition requirement for this transform.
Using as series arms in your simulator relatively high in value resistors 1 Kohm, it cannot be? anticipated that really was created Norton's circuit because the current source does not reach the required current level? when 1 Kohm >> Z ant in frequency range of interest from f lc ( low-cut off ) to up to f0 ( resonance point ).
?
Regards,
Raphael
?
? |
Re: MLA-30+, the story continues!
#Small_receiving_loops_RX-only
Hi Martin & Fred,
?
Thanks for the article links. I will dig into them later.
?
At this moment, I don't have notch filters for the 5-30 MHz range that I want to measure. To quickly verify whether the IP is internal to the TinySA, I will try to increase its attenuation to see if the displayed IMD reduces.?
What I find hard to understand is why the measured OIP3 is 30 dBm at 20 MHz (see graph), but progressively drops as the frequency pair is lowered, and finally reaching 16 dBm at 5 MHz. My expectation is internally generated IMD should be quite constant over frequency. On the other hand, if the external & internal IMD are combining constructively and destructively at different frequencies, as Martin has speculated, I would expect the OIP3 trace to be wavy. Or did I miss something?
Anyway, more investigation is required to understand the setup's eccentricities.
At the project onset, I thought it would take 1 month max to build a working active loop, but now it has already taken a year of my life ?. What a deep rabbit hole!
?
73, Chin-Leong Lim, 9W2LC |
Re: MLA-30+, the story continues!
#Small_receiving_loops_RX-only
On Sun, Oct 6, 2024 at 07:32 PM, <biastee@...> wrote:
Hi Chin-Leon Lim Measurements of high IP3 values are challenging. It is very likely that the measured IM products will be created in Tiny SA itself, not in the DUT. Your limitation is the internal IP of the Tiny SA ?
regards, Fred |
Re: MLA-30+, the story continues!
#Small_receiving_loops_RX-only
Hi Leong,
?
OK thanks for that.
?
From experience, I don't think you will be able to achieve the required performance of your test setup without building fundamental frequency notch filters to place on you analyser input.
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Ideally you need to be able to measure signal levels below -100dBm, in the presence of test signals at 0dBm or more. Even with a high end SA, this is asking a lot.
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Steve and Everett wrote this useful practical guide for Siglent.
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https://www.siglenteu.com/application-note/inter-modulation-distortion-imd-testing/
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I think the variation you are seeing is due to the external and internal IP generation aiding and abetting each other as the phase and amplitude relationships vary with frequency.
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In the old days of analogue TV transmitters, we used to deliberately generate IP products at low level, and inject them into the RF transmission chain, to null out IP's that were being produced in the high power amplifier stages. We called this feed-forward correction.
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Regards,
?
Martin
? |
Re: MLA-30+, the story continues!
#Small_receiving_loops_RX-only
On Sun, Oct 6, 2024 at 10:52 AM, Martin - Southwest UK wrote:
Hi Martin,
Sharp eyes! ?
You r correct, the LZ1AQ OIP3 looks too small. I think the problem lies in the large variation with freq - the OIP3 varies from 16 dBm at 5 MHz to 30 dBm at 20 MHz. In contrast, the competition - MLA-30+, M0AYF & PA0FRI have flatter OIP3 variation.
?
The |OIP3 - P1dB| in the table looks deceptively small because it is the worst case value, taken at different frequencies, i.e. P1dB is taken at 20 MHz, while OIP3 is at 5 MHz. If the OIP3-P1dB is taken at the same frequency, say 20 MHz, the delta is a more believable 15 dB (see this graph). When I find the time, I will create another graph showing |OIP3-P1dB| vs. freq - hopefully, it will clarify things.
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FY6900 function gen, Minicircuits ZSC-2-4 hybrid combiner, & TinySA. I admit I haven't validated the setup.
Hi Everett, thanks for sharing your measurement results.
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73, Chin-Leong Lim, 9W2LC.
? |