Relay-Version: version B 2.10 5/3/83; site utzoo.UUCP Path: utzoo!linus!philabs!cmcl2!harvard!caip!lll-crg!lll-lcc!pyramid!hplabs!hplabsb!bl From: bl@hplabsb.UUCP (Bruce T. Lowerre) Newsgroups: net.sci Subject: Re: How will it fall? Message-ID: <3477@hplabsb.UUCP> Date: Wed, 14-May-86 12:46:52 EDT Article-I.D.: hplabsb.3477 Posted: Wed May 14 12:46:52 1986 Date-Received: Fri, 16-May-86 05:19:22 EDT References: <632@tekigm2.UUCP> <3461@hplabsb.UUCP> <415@ccird1.UUCP> Organization: Hewlett Packard Labs, Palo Alto CA Lines: 36 > In article <3461@hplabsb.UUCP> bl@hplabsb.UUCP (Bruce T. Lowerre) writes: > >> Hello Out There, > >> > >> Here's a little thought problem that might stir things up a bit. > >> > >> Picture yourself on a space station similar to the one used in 2001 > >> (i.e. a spinning ring or toroid). You are standing in the middle of > >> one of the decks near the outside edge of the ring and the spin of > >> the station is providing a "gravity" about equal to that found on > >> the surface of the Earth. > >> > >> If you were to drop a ball (a simple release with no additional > >> forces applied), would it fall straight down (along a line through > >> the center of the ring and the point of release) or would it follow > >> another path (relative to the aforementioned line)? > > > >Due to angular momentum (or lack there of) it will fall in a curved > >path toward the opposite direction of the rotation of the toroid. > > Theoretically, there should be the same curved path for a ball dropped > on Earth. It is not noticable because the earths rotation is so slow, > and gravity so strong, that it would appear to fall straight. > > As to whether you would see an observable curve, depends on the, > diameter of the toroid. Since you have specified pseudogravitation > equal to earths, a small toroid would have to spin very quickly, and > curvature would be quite pronounced. If the toroid were sufficiently > large, the arc might only be a few seconds. > > Does anybody have a formula for the relationship? An interesting observation is that the falling ball inside of the toroid would NOT accelerate as it "fell" while on Earth it would. Actually, the ball would mearly proceed in a straight line (seen from an unaccelarted frame of reference). If the ball were to be released on a point along the axis of rotation, then it would not "fall".