Loop antennas used for long and medium wave reception are based on the
principle of a large loop whose inductance is tuned out with an air variable
capacitor or varactor in series with loop. It does just what Doug describes:
allows a lot of current to flow at a very sharply tuned resonant frequency.

Ken Javor
Phone: (256) 650-5261




From: Douglas Smith <[email protected]>
Reply-To: Douglas Smith <[email protected]>
Date: Mon, 29 Jan 2018 22:55:06 -0800
To: <[email protected]>
Subject: Re: [PSES] [SI-LIST] Re: Measurement Dilema - THE EXPLANATION!


 Hi Istvan, If I connect the oscillator directly to the scope chassis, I get
similar readings at different frequencies. I generally get less amplitude as
well.

The small capacitance between the scope and oscillator is capable of tuning
the whole system to a low input impedance on the probe end. I have seen this
in many scenarios that ended up loading the oscillator to a near short
circuit! The whole system is resonant. I only get enough current to get
large probe voltages at discrete frequencies. I had to tune around to get
the results you saw. These is a lot more information when I do the demo live
for a class that are not practical to put in a video (would last way too
long).

I think amateur radio operators can identify with the amazing
characteristics of resonant systems.

A loop is not nearly dangerous as a loop terminated in a small capacitance!

Tesla coils resonate using stray capacitance. I built a 600 Watt coherent
300 kHz RF driven Tesla Coil in the 9th grade, but that is another
story......

Doug
K4OAP

Doug Smith
Sent from my iPhone
IPhone:  408-858-4528
Office:    702-570-6108
Email:     [email protected]
Website: http://dsmith.org

On Mon, Jan 29, 2018 at 22:24, Istvan Novak <[email protected]>
wrote:
> Doug,
> 
> I see your point, but I think we would need a little more convincing
> argument for the amount of current you assume in this example.
> 
> I agree with the approximate calculation of the L*dI/dt voltage drop,
> where the ground-lead inductance is assumed to be 100nH and I assume you
> measured the rise/fall times of the HC240 to be around 2ns.  If we
> assume 40mA current delta, we approximately get the voltages you see on
> the screen.   I am just not convinced that the current is really in the
> order of 40mA.  If I am not mistaken, you say (and the video suggests
> the same) that the oscillator's return (its 'ground') is left floating.
> In this case it matters much less what is the inductance of the
> ground-lead loop (you say it is 100nH, not disputed), but for current to
> flow through the oscillator output, it has to find its way back to its
> return by going through the parallel of the two probes' braid impedance
> (we can call it common-mode impedance) and eventually it has to close
> back to the floating return of the oscillator.  This last portion of the
> current loop, closing back from the oscilloscope chassis/ground to the
> oscillator return would need to be in the order of 50 pF or higher in
> capacitive coupling to not limit to current to lower values.  Judging
> crudely from the video, the 'stray' capacitance of the oscillator might
> very well be much lower.  However, here is another possible contributor
> to the waveforms on the oscilloscope screen: the oscillator imposes a
> common-mode voltage onto the scope probes, which creates current in the
> shields and these being passive probes, through the finite surface
> transfer impedance of the cable braid, voltage is induced at the probe
> connections.  To prove/disprove the existence and amount of this
> potential contributor, you could redo the test by eliminating the
> ground-lead loop (for instance by using coax receptacles for the probe
> tips), leaving everything else the same. If the displayed voltage drops
> significantly, I would consider as a proof that in fact the dominant
> source of the waveform is related to the ground-lead inductance.  If the
> displayed waveforms would not change considerably, it still would not
> prove that the finite surface transfer impedance is the man cause, but
> it would prove that there should be another major contributor beyond the
> ground-lead inductance.  In this letter case further tests could be
> devised to nail down the major contributor.
> 
> What do you think?
> 
> Regards,
> 
> Istvan Novak
> 
> Oracle
> 
> 
> 
> On 1/29/2018 3:13 PM, Doug Smith wrote:
>> > OK Everyone,  here is the explanation:
>> >
>> > The box is superfluous, it just hides what is actually going on. The box
>> contains two heavy gauge wires. One shorts the two tips sig and gnd together
>> and the other connects the center point of the first wire  to the center pin
>> of the BNC connector. This is equivalent to removing the box and putting a
>> stiff wire into the BNC center pin  on the generator and connecting both
>> probe tips and both ground leads to this stiff wire.
>> >
>> > Doing so causes the generator to push a current out the prob e ground leads
>> creating a voltage across the inductance of the leads that create a loop at
>> the front of the probe. The current flowing through the ground leads creates
>> magnetic fields that for the most part are captured by the loop formed by the
>> ground leads and probe delivering the induced voltage to the probes.
>> >
>> > The probes only respond to voltage between their tips and ground lead
>> attachment point, and the ground lead induced voltage is delivered to each
>> probe by loop they form.
>> >
>> > Since the probes are lying apart from each other, one on the plastic table
>> with a loop in its cable, and the other over a highly conducting (center
>> layer) ESD mat, their common mode impedance will be different, varying at
>> different frequencies. That results in different common mode currents on the
>> probes and the ground lead induced voltages are therefore different and that
>> is what is displayed on the scope. It is interesting that the current output
>> of an HC240 Octal Inverting Buffer can induce volts across the ground leads
>> when its output is only 5 V P_P, but entirely understandable if you calculate
>> e = Ldi/dt = 100 nH*.040 A/2ns) as an approximation.
>> >
>> > For the generator to push a current onto the probe cables, it must form an
>> image current somewhere and that is displacement current to the nearby scope
>> chassis and some radiation from the oscillator itself into the "ether,"
>> although it is on the small side to radiate itself efficiently at 40 MHz.
>> >
>> > I suspect the total current being pushed onto the probes is about 40 mA,
>> the short circuit current of the HC240 IC being used. At some frequencies,
>> each probe cable will resonate with the capacitance back to the scope from
>> the oscillator. By changing the frequency, I can make either probe register a
>> larger signal than the other probe.
>> >
>> > I love experiments like this. I have been doing this one for over 20 years
>> for my classes and have have tons more demos to challenge engineering minds.
>> Most of my demos have an unexpected result and the discussion that follows
>> elucidates some engineering principle or addresses a myth.
>> >
>> > Doug
>> > University of Oxford, Course Tutor
>> > Department for Continuing Education
>> > Oxford, Oxfordshire, United Kingdom
>> > --------------------------------------------------
>> > Doug Smith
>> > P.O. Box 60941
>> > Boulder City, NV 89006-0941
>> > TEL/FAX: 702-570-6108/570-6013
>> > Mobile: 408-858-4528
>> > Email: [email protected]
>> > Web: http://www.dsmith.org
>> > --------------------------------------------------
>> >
>> >
>> >
>> > On Mon, 29 Jan 2018 14:40:17 -0800, "Tom Dagostino"  wrote:
>> >
>> > Why is everybody looking for tricks or complex answers.  This is really a
>> > very simple, basic issue.  If you look closely you will see the difference.
>> >
>> > Tom Dagostino
>> > 971-279-5325
>> > [email protected]
>> >
>> > Teraspeed Labs
>> > 9999 SW Wilshire Street
>> > Suite 102
>> > Portland, OR 97225
>> >
>> >
>> > -----Original Message-----
>> > From: [email protected] [mailto:[email protected]] On
>> > Behalf Of Austin Mack
>> > Sent: Monday, January 29, 2018 2:28 PM
>> > To: [email protected]; 'si-list'
>> > Subject: [SI-LIST] Re: ***UNCHECKED*** Measurement Dilema
>> >
>> > Hi All,
>> >
>> > It looks to me like the oscillator and its power pack (with very long
>> leads)
>> > are in close proximity to the CH2 probe cable. Since the oscillator output
>> > is tied to GND at the probes, it and the floating power pack will be
>> > radiating like crazy at 40MHz and electromagnetically and capacitively
>> > coupling to the CH2 shield which BTW is close to a quarter wavelength.
>> >
>> > Austin
>> >
>> > -----Original Message-----
>> > From: [email protected] [mailto:[email protected]] On
>> > Behalf Of Doug Smith
>> > Sent: Friday, January 26, 2018 2:53 PM
>> > To: si-list
>> > Subject: [SI-LIST] ***UNCHECKED*** Measurement Dilema
>> >
>> > 
>> >
>> >
>> > Hi All,
>> >
>> > Can you explain the result in this video I just made? Scope plots of the
>> > same two nodes are completely different. Probes and scope are operating
>> > normally, no problem with the equipment itself.
>> >
>> > If you have been to my seminars you know the answer, please do not post the
>> > answer unless you have not seen this experiment until now.
>> >
>> > Hint 1: There are no EM fields radiating from the shielded box affecting >>
the
>> > probes.
>> > Hint 2: There are no active components inside the box.
>> >
>> > https://youtu.be/qj-HBFMEJiY
>> >
>> > I do a lot of experiments in my classes that give surprising results. Each
>> > one addresses a design or troubleshooting problem that engineers do not
>> > realize their troubleshooting efforts. Next
>> > one:http://emcesd.com/bcsem_hfmeas.htm on March 13-16.
>> >
>> > Doug
>> >
>> >
>> >
>> >
>> >
>> >
>> >
>> >
>> >
>> > ------------------------------------------------------------------
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> 
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