Relay-Version: version B 2.10 5/3/83; site utzoo.UUCP Posting-Version: version B 2.10.1 6/24/83; site brl-vgr.ARPA Path: utzoo!watmath!clyde!floyd!harpo!seismo!brl-vgr!gwyn From: gwyn@brl-vgr.ARPA (Doug Gwyn ) Newsgroups: net.math Subject: Re: Calculus problem Message-ID: <3077@brl-vgr.ARPA> Date: Sat, 31-Mar-84 02:17:35 EST Article-I.D.: brl-vgr.3077 Posted: Sat Mar 31 02:17:35 1984 Date-Received: Sat, 31-Mar-84 10:08:51 EST References: <115@iham1.UUCP> Organization: Ballistics Research Lab Lines: 31 Your problem boils down to two assumed initial conditions: s(t=0) = 0 v(t=0) = 0 where v = ds / dt and one force equation: (F = ) m a = m g - k v^2 where a = dv / dt = d^2s / dt^2 (sorry about the superscripts) In terms of s(t) this is a second-order non-linear ordinary differential equation with two equations of constraint (boundary conditions): s(0) = 0 s'(0) = 0 where ' denotes time-derivative m s''(t) = m g - k (s'(t))^2 What you do at this point depends on why you are asking the question. I myself would just look up the solution and save time. Since you have the solution for s(t), all you technically need to do is just demonstrate (by substitution) that it satisfies the three constraints. If this is for a course in ODE, you should use some of the tricks taught in the course to methodically synthesize the answer. Note that IF there is a limiting velocity, its value is trivial to derive, since then a == 0 and the force equation is trivial to solve for v.