Relay-Version: version B 2.10 5/3/83; site utzoo.UUCP Posting-Version: version B 2.10.2 9/5/84; site umich.UUCP Path: utzoo!lsuc!watmath!clyde!burl!ulysses!gamma!epsilon!mb2c!umich!torek From: torek@umich.UUCP (Paul V. Torek ) Newsgroups: net.politics.theory Subject: Re: Pollution: no libertarian solution! Message-ID: <374@umich.UUCP> Date: Thu, 19-Dec-85 13:38:40 EST Article-I.D.: umich.374 Posted: Thu Dec 19 13:38:40 1985 Date-Received: Fri, 20-Dec-85 21:57:12 EST References: <841@mmintl.UUCP> <353@umich.UUCP> <618@calgary.UUCP> <365@umich.UUCP> <2@calgary.UUCP> Reply-To: torek@zippy.UUCP (Paul V. Torek ) Organization: University of Michigan, EECS Dept., Ann Arbor, MI Lines: 18 Summary: In article <2@calgary.UUCP> radford@calgary.UUCP (Radford Neal) writes: >For an analogy, consider the derivation of classical electrodynamics from >quantum electrodynamics. The classical laws can be derived as statistical >approximations, but not absolutely. > >In practice, this means that I can apply the usual "rules" of libertarianism >to a large number of real cases but don't have to try to defend *every* >application of them to peculiar circumstances. I don't think this is >cheating; everyone does it. Well, it depends. Note that one can predict when the classical laws fail, and when they do fail, one can turn to quantum-mechanical desription for principled answers. Now, what analogous recourse does your libertarianism have in the problem cases? If there is none, I think something very fishy is going on. --Paul V Torek torek@umich (Or is that torek@zippy now? Darn rn headers!)