The analytical portion of this post is, as the author stated, worst case.  A
cable attached to a susceptible circuit picks up a common-mode potential,
which most likely drives a current on a shield if the the circuit is
sensitive.  Then only the current multiplied by shield transfer impedance
actually gets into the victim, assuming no CMR.  Which just makes my
original point - unintentional emissions from ITE can only upset a radio
receiver tuned to the emission frequency.  That is why, as another
contributor posted, we use EMI receivers and spectrum analyzers with preamps
to make OATS measurements.

 on 1/4/02 12:51 PM, Tom Cokenias at t...@tncokenias.org wrote:

> At 8:34 AM -0500 1/4/2002, Keith Armstrong wrote:
> 
>> Does anyone else think that ordinary semiconductors doesn't respond to RF?
> 
> 
> 
> I agree that commonly used semiconductors have responses well into
> the 100's of MHz.
> 
> How much of a problem this is will depend on the nature and function
> of the circuitry using these components.
> 
> The EUT wires, cables, pcb traces etc. act like antennae,  on which
> the incident field voltages and currents.  An antenna factor can be
> thought of as ratio of the field strength  to the voltage induced on
> the terminated cable connected to the antenna.
> 
> In an impedance matched system,
> 
> 
> AF=9.734/lamda*(G)^0.5,   lamda being wavelength in meters, G being
> antenna gain over isotropic,
> 
> or in dB
> 
> AF dB =  -  G dBi  -29.7 dB + 20logFMHz
> 
> Assuming G is 1 (isotropic antenna), AF is 1  (= 0 dB) at about 30.8
> MHz, and AF get larger  as frequency increases, to  a factor of 32.7
> (= 30.3 dB) at 1 GHz .  Since AF is  field strength divided by
> induced voltage, the voltage induced on the trace goes down as
> frequency goes up for the same incident field strength.
> 
> An effective receive antenna needs to be on the order of 1/2
> wavelength or so; for 30 MHz this is 15m, for 1000 MHz this is 15 cm.
> 
> So if a victim EUT circuit has a pretty effective receive  antenna,
> and does not have any filtering and is equally sensitive across the
> frequency range under consideration (all taken together, a worst case
> scenario for susceptibility),
> 
> (1)  A 10 V/m field will  theoretically induce a voltage  0.33V  to
> 10V, depending on frequency
> 
> (2) A 5000 uV/m field (10x the FCC class B limit above 960 MHz) will
> theoretically induce a voltage from 152 uV to 5 mV, depending on
> frequency.
> 
> (3) A 500 uV/m field will  theoretically induce a voltage from 15 uV
> to 500 uV depending on frequency.
> 
> These are first order approximations, but they are useful in
> determining the level of the potential EMI  threat.   For instance a
> 4-30 mA sensor circuit using high gain operational amps will most
> likely  be interfered with  in scenario (1),  there may be some
> susceptibility detected in scenario (2), and most likely no problem
> encountered with scenario (3).
> 
> A sensitive all - band  AM communications receiver will have problems
> with all three, a broadcast TV operating in a strong signal area will
> probably be OK  with scenario 3 but not with 1 or 2.
> 
> I guess what I'm really trying to say with all this is that EMC is a
> systems thing, taking into account the nature of the culprit EMI
> generator, the nature of the victim EMI receiver,  and the path
> between them.  Then we have the economics of operating different
> devices in the same vicinity, the politics of who gets how much of
> what kind of protection, etc., etc.  All things considered, we should
> have jobs for life!
> 
> best regards and a Happy New Year to all.
> 
> Tom Cokenias
> 
> T.N. Cokenias Consulting
> P.O. Box 1086
> El Granada CA 94018
> 
> tel   650 726 1263
> cell 650 302 0887
> fax  650 726 1252
> 
> 
> 
> 
> 
> 
> 
> 


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