Relay-Version: version B 2.10 5/3/83; site utzoo.UUCP Posting-Version: version B 2.10.1 6/24/83; site hhb.UUCP Path: utzoo!watmath!clyde!cbosgd!ihnp4!houxm!whuxl!whuxlm!harpo!decvax!mcnc!philabs!hhb!leon From: leon@hhb.UUCP (Leon Gordon) Newsgroups: net.math Subject: Re: Interview Q revisited Message-ID: <104@hhb.UUCP> Date: Tue, 26-Mar-85 00:33:12 EST Article-I.D.: hhb.104 Posted: Tue Mar 26 00:33:12 1985 Date-Received: Fri, 29-Mar-85 00:50:26 EST References: <7700003@hplvle.UUCP> Organization: HHB-Softron, Mahwah, NJ Lines: 26 Actually, the delta "functional" can not be represented as the limit of a sequence of odd functions, but a closely related function (the "derivative" of the delta "function" can). It is easy to convince yourself that this function extracts the value of the derivative of the function it is convoluted with. that is: integral[ delta'(t-T) * f(t)]dt = a*f'(0) where a is a constant factor that I'm too lazy to figure out at the moment (some mix of 2's, pi's, and -1's) By the way, a much clearer and more intuitive way of looking at delta and related quantities is as a linear functional over a prescribed function space. Thus delta is the functional which maps f(x) -> f(0). The properties of delta can be developed formally without the pain of considering distributions. leon {decvax,ihnp4,allegra}!philabs!hhb!leon