Re: Radiation formula

2002-08-15 Thread Doug McKean

Re: Radiation formulaLooks like Ott formulas. Personally I have trouble with
those equations.  There's obviously some trig functions
that should be included in those equations to denote
directionality or directivity, or there's some assumption(s)
going on not stated.

Those equations in general form are highly directional.
It is true that one can use those equations to show that
the E-field produced by a Hertzian magnetic dipole is
proportional to the square of the frequency and that the
E-field produced by a Herztian electric dipole is
proportional to the frequency, but the magnitudes of
the coefficients could erronously show which is of
greater concern depending upon the situation and
obviously do not give any information about directivity.

Personal opinion only.  This post is NOT to be construed
as a criticism of the great pioneer himself, Mr. Ott.

Regards, Doug McKean



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Re: Radiation formula

2002-08-14 Thread Ken Javor
I'll bet I could work it out, but you need to understand sever limitations
of these models.  The loop model is a low frequency model.  It might work at
30 MHz for a physically small radiator, but it only works when the loop size
is small relative to a wavelength.  If there is a cable connected tot he
EUT, then you have to look at cable radiation, which is more efficient at
low frequencies.  And that brings up a major limitation of the second
equation.  It only works at frequencies where the cable is electrically
short.  Off the top of my head I don't know the exact form of the real
equation, but in this low frequency model someone has used the small angle
approximation that sin x = x for small x to substitute the ratio of cable
length to wavelength instead of the sine of that ratio.

--
From: Dave Wilson davewilson...@yahoo.com
To: emc-p...@ieee.org
Subject: Radiation formula
List-Post: emc-pstc@listserv.ieee.org
Date: Wed, Aug 14, 2002, 1:53 PM



Hi Group,

I found a source which states that radiated emissions can be modeled as a
small loop antenna (i.e. less than 1/4 wavelength), where the maximum
E-field strength at 10m is proportional to the square of the frequency:-

E = 263 x 10^-12 (F^2 x A x Is) V/m

where A = loop area in sq cm, F in MHz, Is = source current in mA

For cable radiation, we can model as a monopole antenna over a ground plane,
whereby the maximum field strength at 10m (allowing for +6dB ground
reflections) is direectional proportional to the frequency:-

E = 1.26 x 10^-4 (F x L x Icm) V/m

where L = cable length in m, Icm is cm current at F MHz in the cable

My question is this - does anyone out there know how the constants in these
formulae are derived?

Thanks in advance,

Dave Wilson





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Radiation formula

2002-08-14 Thread Dave Wilson

Hi Group,

I found a source which states that radiated emissions can be modeled as a small 
loop antenna (i.e. less than 1/4 wavelength), where the maximum E-field 
strength at 10m is proportional to the square of the frequency:-

E = 263 x 10^-12 (F^2 x A x Is) V/m

where A = loop area in sq cm, F in MHz, Is = source current in mA

For cable radiation, we can model as a monopole antenna over a ground plane, 
whereby the maximum field strength at 10m (allowing for +6dB ground 
reflections) is direectional proportional to the frequency:-

E = 1.26 x 10^-4 (F x L x Icm) V/m

where L = cable length in m, Icm is cm current at F MHz in the cable

My question is this - does anyone out there know how the constants in these 
formulae are derived?

Thanks in advance,

Dave Wilson





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