Relay-Version: version B 2.10 5/3/83; site utzoo.UUCP Path: utzoo!mnetor!uunet!seismo!columbia!rutgers!husc6!bloom-beacon!gatech!emory!platt From: platt@emory.uucp (Dan Platt) Newsgroups: sci.physics,sci.philosophy.tech Subject: Re: a QM paradox (??) Message-ID: <2191@emory.uucp> Date: Tue, 4-Aug-87 01:34:32 EDT Article-I.D.: emory.2191 Posted: Tue Aug 4 01:34:32 1987 Date-Received: Thu, 6-Aug-87 01:34:30 EDT References: <3794@oberon.USC.EDU> Reply-To: platt@emory.UUCP (Dan Platt) Distribution: sci Organization: Math & Computer Science, Emory University, Atlanta Lines: 74 Keywords: Uncertainity Principle Xref: mnetor sci.physics:1963 sci.philosophy.tech:349 In article <3794@oberon.USC.EDU> mathur@pollux.usc.edu (Samir Kumar Mathur) writes: >Here is a thought experiment which seems to violate Uncertainity Principle (UP) >that came up at a casual discussion with a friend. > >Scenario : > There are two particles A and B and I am trying to measure their > momentum and positions accurately. > >Experiment : > (1) At time t: > (a) I measure the momentums p(A,t) & p(B,t) and hence > p(A&B,t) = p(A,t) + p(B,t) as accurately as I wish. > > (2) At time t+dt: > (a) I measure the momentum of A, p(A,t+dt) as accurately > as I wish. > (b) I measure the position of B, q(B,t+dt) as accurately > as I wish. > (c) I calculate p(B,t+dt) = p(A&B,t) - p(A,t+dt) > {conservation of momentum} as accurately as I wish. > >Conclusion: > From steps 2(b),(c) I conclude that I can measure p(B,t+dt),q(B,t+dt) > as accurately as I wish. This obviously violates Heisenberg's UP. > >----------------------------------------------------------------------------- A simple answer to this paradox could center around several points: 1) How repeatable are your results? 2) Exactly how is your system configured? In answer to 1), you may be able to measure q(B,t+dt), but if you run several experiments, you'll find that the value of q is not predictable to within a factor of hbar/2/deltap where deltap is the uncertainty in p(A) and p(B). If you adjust the experiment to improve the measurement of q, then the values of the p's will deteriorate (assuming your experiment is capable of measureing to the accuracies required to observe these). For point 2) it looks like you have two particles A and B which are interacting only with each other, and that they may exchange momentum between t and t+dt. If this is so, how did you measure the momentum at t so that you knew what the momentum was after the measurement? (I won't suggest that the act of measurement produces effects which can't be determined; limitations in measurements are inherent in the system, and should be determinable, but it is important to consider that your measurement techniques should be reflected in the conservation of momentum equation (have you added or changed momentum?)). Lastly, I'd like to point out that the Heisenberg Uncertainty Principle is mathematically equivalent to the restriction of the rate of transmission of information via radio. If you send a signal with amplitude modulation (AM) or frequency modulation (FM -- though this is a little more complicated) a pure tone (the carrier) contains no information. When you modulate the carrier, you induce new frequencies. If you want to localize a signal (information) in a smaller and smaller dt, then you need a wider and wider dfrequency (bandwidth of induced frequencies) to handle the information. This is equivalent to trying to localize the location of a particle to dq; it requires a larger and larger bandwidth of dp's to handle the information required to define dq. The reason for this is that in quantum mechanics, the p,q pair are 'conjugate' to each other in the same way that frequency,t are 'conjugate' to each other in radio transmission. If you accept the DeBrogie hypothesis (which has been experimentally confirmed in any experiment dependant on quantum effects), then the Heisenberg principle follows. It's built into the structure of QM. Hope this is a help. Dan