Relay-Version: version B 2.10 5/3/83; site utzoo.UUCP Posting-Version: version B 2.10.3 4.3bsd-beta 6/6/85; site ucbvax.BERKELEY.EDU Path: utzoo!watmath!clyde!burl!ulysses!ucbvax!space From: ST401385@BROWNVM.BITNET Newsgroups: net.space Subject: Specific Impulse Message-ID: <8603070058.AA06014@s1-b.arpa> Date: Thu, 6-Mar-86 14:36:07 EST Article-I.D.: s1-b.8603070058.AA06014 Posted: Thu Mar 6 14:36:07 1986 Date-Received: Sat, 8-Mar-86 05:11:26 EST Sender: daemon@ucbvax.BERKELEY.EDU Organization: The ARPA Internet Lines: 25 The metric unit (newton seconds thrust per kilogram propellant) which is measured in meters per second, is properly defined as the exhaust velocity, Ve, *not* the specific impulse. Ve = g Isp Where Isp is specific impulse, and g is the acceleration of gravity. This is true in any system of units. However, you are right that Ve is a much more convenient way to specify propellant characteristics, since you can plug it right into the rocket equation, Delta V = Ve ln(Mi/Mf) Where Mi/Mf is the mass ratio. Specific impulse (and exhaust velocity) are most useful for systems where the energy and the reaction gas are the same. In this case, it is *always* to your advantage to increase the specific impulse (or exhaust velocity). For objects like nuclear engines, where the energy comes from a different source than the reaction gas, it is a less useful concept. --Geoffrey A. Landis, Brown University Reply to: ST401385%BROWNVM.BITNET@WISCVM.ARPA