Delivered-To: daveyxm@virginmedia.com Received: by 10.50.1.100 with SMTP id 4csp35468igl; Sun, 14 Jul 2013 14:36:55 -0700 (PDT) X-Received: by 10.180.74.197 with SMTP id w5mr7013910wiv.20.1373837814287; Sun, 14 Jul 2013 14:36:54 -0700 (PDT) Return-Path: Received: from post.thorcom.com (post.thorcom.com. [195.171.43.25]) by mx.google.com with ESMTP id la4si16287398wjb.139.2013.07.14.14.36.53 for ; Sun, 14 Jul 2013 14:36:54 -0700 (PDT) Received-SPF: neutral (google.com: 195.171.43.25 is neither permitted nor denied by best guess record for domain of owner-rsgb_lf_group@blacksheep.org) client-ip=195.171.43.25; Authentication-Results: mx.google.com; spf=neutral (google.com: 195.171.43.25 is neither permitted nor denied by best guess record for domain of owner-rsgb_lf_group@blacksheep.org) smtp.mail=owner-rsgb_lf_group@blacksheep.org Received: from majordom by post.thorcom.com with local (Exim 4.14) id 1UyTKW-0005Hs-K7 for rs_out_1@blacksheep.org; Sun, 14 Jul 2013 21:55:40 +0100 Received: from [195.171.43.32] (helo=relay1.thorcom.net) by post.thorcom.com with esmtp (Exim 4.14) id 1UyTKW-0005Hj-25 for rsgb_lf_group@blacksheep.org; Sun, 14 Jul 2013 21:55:40 +0100 Received: from mx5.utsp.utwente.nl ([130.89.2.33] helo=mxpool.utwente.nl) by relay1.thorcom.net with esmtps (TLSv1:AES256-SHA:256) (Exim 4.77) (envelope-from ) id 1UyTKU-0002FW-N9 for rsgb_lf_group@blacksheep.org; Sun, 14 Jul 2013 21:55:38 +0100 Received: from ewi1614.ewi.utwente.nl (utwks06146.ad.utwente.nl [130.89.13.213]) by mxpool.utwente.nl (8.13.8) with ESMTP id r6EKtbuP022758 for ; Sun, 14 Jul 2013 22:55:37 +0200 Received: by ewi1614.ewi.utwente.nl (Postfix, from userid 17643373) id 52CC03C40903; Sun, 14 Jul 2013 22:55:37 +0200 (CEST) Date: Sun, 14 Jul 2013 22:55:37 +0200 From: Pieter-Tjerk de Boer To: rsgb_lf_group@blacksheep.org Message-ID: <20130714205537.GB6192@cs.utwente.nl> Mail-Followup-To: rsgb_lf_group@blacksheep.org References: <51DF33E4.7030101@iup.uni-heidelberg.de> <20130713103545.GA13777@cs.utwente.nl> <51E1DB68.80007@iup.uni-heidelberg.de> MIME-Version: 1.0 Content-Disposition: inline In-Reply-To: <51E1DB68.80007@iup.uni-heidelberg.de> User-Agent: Mutt/1.5.20 (2009-06-14) Subject: Re: Fwd: Re: LF: VK1OD's analysis of the MiniWhip antenna Content-Type: multipart/mixed; boundary="LQksG6bCIzRHxTLp" X-Spam-Checker-Version: SpamAssassin 2.63 (2004-01-11) on post.thorcom.com X-Spam-Level: X-Spam-Status: No, hits=0.0 required=5.0 tests=none autolearn=no version=2.63 X-SA-Exim-Scanned: Yes Sender: owner-rsgb_lf_group@blacksheep.org Precedence: bulk Reply-To: rsgb_lf_group@blacksheep.org X-Listname: rsgb_lf_group X-SA-Exim-Rcpt-To: rs_out_1@blacksheep.org X-SA-Exim-Scanned: No; SAEximRunCond expanded to false Status: O X-Status: X-Keywords: X-UID: 1849 --LQksG6bCIzRHxTLp Content-Type: text/plain; charset=iso-8859-1 Content-Disposition: inline Content-Transfer-Encoding: quoted-printable X-MIME-Autoconverted: from 8bit to quoted-printable by mxpool.utwente.nl id r6EKtbuP022758 On Sun, Jul 14, 2013 at 12:57:44AM +0200, Stefan Sch=E4fer wrote: > Of course the plate is > at one potential, just as the grounded pole. So the equipotential > lines in the sketch will go a different way when the probe is placed > on the top of the pole. Attached is a plot of the equipotential lines in the case of a pole with some probe (quite a big cylinder in this case) above it. In contrast to my earlier picture, this one is not a hand-drawn sketch, but it is a (numerical) solution to Maxwell's equations (which in this simple case simplify to Laplace's equation). It is still a simplification of course: in reality there must be some circuitry between pole and probe, which will further disturb the field a bit. But a thin wire will do so much less than the pole. > I meant that the optimal position of the > probe must be there, where the density of the equipotential lines > (and so the E field strength) is as high as possible, I don't think so. When there's a pole but no probe, the equipotential lines are densest just above the pole (there they are compressed most). However, those lines just above the pole are the ones which are at the lowest potential (follow them to the left or right and you see they are close to ground). A little bit higher the equipotential lines are less dense, but these lines are at a much higher potential, so putting the probe there gives a much higher output voltage. > so that the > capacity against the far field is as high as possible and the > capacity to the grounded pole is as low as possible, so that the > capacitive divider is optimized. As noted above: the equipotential lines are densest just above the grounded pole, but that's of course also the place where the probe's capacity to the pole would be largest. So again, that's not the best place. 73, Pieter-Tjerk, PA3FWM --LQksG6bCIzRHxTLp Content-Type: image/png Content-Disposition: attachment; filename="pole-and-probe.png" Content-Transfer-Encoding: base64 iVBORw0KGgoAAAANSUhEUgAAAnoAAAGlCAIAAADiSMw8AAAABGdBTUEAALGPC/xhBQAAADh0 RVh0U29mdHdhcmUAWFYgVmVyc2lvbiAzLjEwYSAgUmV2OiAxMi8yOS85NCAoUE5HIHBhdGNo IDEuMindFS5JAAAgAElEQVR4nOy9Z3Rd13mn/9zeG3ovBEAQAIvYKYrqci/xxC22RzNO4jjx xHE8M4mTD7O8Ml7/D0lWZsbxOMtO94zHjos841iusiRKYhGbQBFEL0QvF+323v4fzitcAIKK bV5JpPbz6RK85dxzz9m/vffZ5310hUIBhUKhUCgUpUT/em+AQqFQKBS3PypuFQqFQqEoOcbX ewMUiptBPk8ohMWC3b7l77kc4XDxsdGI1/uSbxIIEAjIY6ORpqaXfGYyycICySSJBEBrK2Vl v/zGP/88uZxsQEUFd9zxK73V6io+H4DB8Cu91fo6k5MANhtWK3V1WK0v+eSZGbJZeezzyQbs SDBINovBIP90u4uPNeJxUik8HvRqMKC4rVBxWxryeVZWyGal9ff7KRSwWGBTO76+TjBINEom w/g4zc2YTASDeDwcOQLQ38/SEkAux/nz7N0rb97WxqFDAI89RiBAKEQsxsgIhw5Jutx7LydO AHzxi6RS8qo//dPi5v3JnwCkUly9yh13SGb83d8Vn/DJTwIEg3znO8U/fvCDsjEXLtDdLX98 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