Return-Path: Received: from portal.udlp.com ([207.109.1.80]) by truman.olsusa.com (Post.Office MTA v3.5.1 release 219 ID# 0-52269U2500L250S0V35) with ESMTP id com for ; Tue, 12 Oct 1999 14:05:41 -0400 Received: from portal.udlp.com (root@localhost) by portal.udlp.com with ESMTP id NAA03987 for ; Tue, 12 Oct 1999 13:09:42 -0500 (CDT) Received: from ccmail.udlp.com ([10.1.6.254]) by portal.udlp.com with ESMTP id NAA03956 for ; Tue, 12 Oct 1999 13:09:40 -0500 (CDT) Received: from ccMail by ccmail.udlp.com (IMA Internet Exchange 3.12) id 0008EFB5; Tue, 12 Oct 1999 13:04:03 -0500 From: CHRISTOPHER_ZAVATSON@udlp.com Date: Tue, 12 Oct 1999 10:58:39 -0500 Message-ID: <0008EFB5.C21254@udlp.com> Subject: Pitot tube (dynamic) pressure To: Lancair.list@olsusa.com X-Mailing-List: lancair.list@olsusa.com Mime-Version: 1.0 <<<<<<<<<<<<<<<<--->>>>>>>>>>>>>>>> << Lancair Builders' Mail List >> <<<<<<<<<<<<<<<<--->>>>>>>>>>>>>>>> >> 1. H = V^2/(2*g) and 2. P = 1/2 * rho * V^2 are equivalent once density is added to equ. 1 to make it fluid specific. One must be very careful with units in this case, especially with density (slug/ft3 vs lb/ft3) P = H[ft] * dens[lb/ft^3] = v[ft/s]^2/(2*g[ft/s^2]) * dens[lb/ft^3] = 0.5 * v[ft/s]^2 * dens[lb/ft^3]/g[ft/s^2] = 0.5 * v[ft/s]^2 * rho[slug/ft^3] If density of the fluid can be considered a constant, as in incompressible pipe flow, it is conventional to express pressures in terms of pressure heads. Then density can be left out of the equation. In aeronautical applications, density of the fluid (air) varies enormously with changes in altitude (among other things)and, therefore, dynamic pressure (1/2 * rho * V^2) is much easier to deal with. It also makes the equation independent of the gravitional 'constant' which technically varies with altitude and latitude. Chris Zavatson L-360 N91CZ >>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>>> LML website: http://www.olsusa.com/Users/Mkaye/maillist.html