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Message-ID: <51DF33E4.7030101@iup.uni-heidelberg.de>
Date: Fri, 12 Jul 2013 00:38:28 +0200
From: =?ISO-8859-1?Q?Stefan_Sch=E4fer?= <Stefan.Schaefer@iup.uni-heidelberg.de>
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To: rsgb_lf_group@blacksheep.org
Subject: Fwd: Re: LF: VK1OD's analysis of the MiniWhip antenna
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Hello Pieter-Tjerk, LF,

Another point comes to my mind:

When thinking about the sketch you recently attached (here attached=20
again), would you agree that here the shape of the probe is _not_=20
irrelevant? I mean, a round plate which is in a horizontal position to=20
ground should cause less potential difference (signal level) then a=20
vertical thin wire with the same capacity.

BTW, capacity against what is the question. It's not the capacity=20
against ground but to the far field i think. Here it becomes complex to=20
me :-)

I try to compare it to a TX antenna. I see the TX antenna as a capacitor=20
against ground. But the imaginary E field lines that go directly to=20
ground are "useless", except for reduction of the needed L for=20
resonance. This can be described as a fixed capacitor parallel to the=20
loading coil. Ony the field lines that make a faaaaaaaar way will cause=20
something that is described by a radiation resistance.
So back to the mini whip, the often stated 4 pF must be against=20
"something useful", which is not the grounded pole. It must catch some=20
of the field lines of the distant transmitter. And if the E fields of=20
your sketch are from this transmitter it must be useful to cross as many=20
as possible of the =E4quipotential lines, i.e. a long thin vertical wire=20
should result in more signal voltage as a plate near the pole.

Or not?

73, Stefan/DK7FC


-------- Original-Nachricht --------
Betreff: 	Re: LF: VK1OD's analysis of the MiniWhip antenna
Datum: 	Sun, 7 Jul 2013 12:15:12 +0200
Von: 	Pieter-Tjerk de Boer <ptdeboer@cs.utwente.nl>
Antwort an: 	rsgb_lf_group@blacksheep.org
An: 	rsgb_lf_group@blacksheep.org

[...]

See the attached sketch: the equi-potential lines in the area near the
probe are much closer together because the pole is at ground potential.

[...]

73, Pieter-Tjerk, PA3FWM


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Hello Pieter-Tjerk, LF, <br>
<br>
Another point comes to my mind: <br>
<br>
When thinking about the sketch you recently attached (here attached
again), would you agree that here the shape of the probe is <u>not</u>
irrelevant? I mean, a round plate which is in a horizontal position to
ground should cause less potential difference (signal level) then a
vertical thin wire with the same capacity. <br>
<br>
BTW, capacity against what is the question. It's not the capacity
against ground but to the far field i think. Here it becomes complex to
me :-) <br>
<br>
I try to compare it to a TX antenna. I see the TX antenna as a
capacitor against ground. But the imaginary E field lines that go
directly to ground are "useless", except for reduction of the needed L
for resonance. This can be described as a fixed capacitor parallel to
the loading coil. Ony the field lines that make a faaaaaaaar way will
cause something that is described by a radiation resistance. <br>
So back to the mini whip, the often stated 4 pF must be against
"something useful", which is not the grounded pole. It must catch some
of the field lines of the distant transmitter. And if the E fields of
your sketch are from this transmitter it must be useful to cross as
many as possible of the &auml;quipotential lines, i.e. a long thin vertical
wire should result in more signal voltage as a plate near the pole. <br>
<br>
Or not?<br>
<br>
73, Stefan/DK7FC<br>
<br>
<br>
-------- Original-Nachricht --------
<table class="moz-email-headers-table" border="0" cellpadding="0"
 cellspacing="0">
  <tbody>
    <tr>
      <th valign="BASELINE" align="RIGHT" nowrap="nowrap">Betreff: </th>
      <td>Re: LF: VK1OD's analysis of the MiniWhip antenna</td>
    </tr>
    <tr>
      <th valign="BASELINE" align="RIGHT" nowrap="nowrap">Datum: </th>
      <td>Sun, 7 Jul 2013 12:15:12 +0200</td>
    </tr>
    <tr>
      <th valign="BASELINE" align="RIGHT" nowrap="nowrap">Von: </th>
      <td>Pieter-Tjerk de Boer <a class="moz-txt-link-rfc2396E" href="mailto:ptdeboer@cs.utwente.nl">&lt;ptdeboer@cs.utwente.nl&gt;</a></td>
    </tr>
    <tr>
      <th valign="BASELINE" align="RIGHT" nowrap="nowrap">Antwort an: </th>
      <td><a class="moz-txt-link-abbreviated" href="mailto:rsgb_lf_group@blacksheep.org">rsgb_lf_group@blacksheep.org</a></td>
    </tr>
    <tr>
      <th valign="BASELINE" align="RIGHT" nowrap="nowrap">An: </th>
      <td><a class="moz-txt-link-abbreviated" href="mailto:rsgb_lf_group@blacksheep.org">rsgb_lf_group@blacksheep.org</a></td>
    </tr>
  </tbody>
</table>
[...]<br>
<pre>See the attached sketch: the equi-potential lines in the area near the
probe are much closer together because the pole is at ground potential.

[...]

73, Pieter-Tjerk, PA3FWM


</pre>
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