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Re: [Phys-l] Teaching Special Relativity



Just as the physics of a moving photon clock explains (below) the mechanism which gives it a longer period, it is the assertion of the relativity principle that there will be a corresponding physical mechanism behind the slowing of any well constructed moving clock.

It is further asserted that the same principle applies to all "relativistic effects" in the behavior of moving objects. This is the very essence of the relativity principle. After all, Einstein's 1905 relativity paper was entitled "The electrodynamics of moving bodies".

Even before 1905 - Lorentz, Fitzgerald, et al argued that a real shortening of a moving rigid rod follows from Maxwellian electrodynamics. Their argument centered around the real weakening of the E field of a moving charge in the direction of its motion (its spherically symmetric field becomes "squashed" in its forward direction). This is a real effect of Maxwellian electrodynamics, with real consequences - it is not merely a projection or merely an appearance .

For Lorentz this effect depended on the absolute velocity of the observed object - ie, relative to the aether. Einstein's leap was the bold assertion that the velocity of an observed charge in Maxwell's equations is relative to the observer - ANY inertial observer.

PS:
J.S. Bell (yes, THAT Bell) outlines the Lorentz approach in "How to Teach Relativity", Progress in Scientific Culture, Vol 1, summer 1976. This paper is included in the paperback collection by Bell: "Speakable and Unspeakable in Quantum Mechanics", Cambridge, 1987.

Bob Sciamanda
Physics, Edinboro Univ of PA (Em)
treborsci@verizon.net
http://mysite.verizon.net/res12merh/

--------------------------------------------------
From: "Bob Sciamanda" <treborsci@verizon.net>
Sent: Saturday, July 04, 2009 8:35 AM
To: <phys-l@carnot.physics.buffalo.edu>
Subject: Re: [Phys-l] Teaching Special Relativity


The driving essence of the principle of (special) relativity is that physics is the same in all (inertial) reference frames. This means that measured quantities are related by the same quantitative equations. This is achieved by (Lorentz) transforming the measurables in the invariant equations.

For example in the case of the simple bouncing photon clock, the physics is simply that time of travel = distance traveled, divided by the frame invariant speed "c".

Both the "proper observer"(traveling with the clock) and the "stationary observer" use this same physics to describe the observed reality. But when you compare the calculations of the two observers, it will be apparent that the stationary observer calculates the time of travel as a larger distance divided by the same speed "c".

The measurable quantities appearing in the physics equation are the physicists "reality"; and these realities change numerical values (through Lorentz transformations) when measured in different reference frames, the physics (equation) remaining the same.

This is the same relativity which describes the E and B components of an electromagnetic field when viewed in different frames. There is no universal "proper" frame in which E and B are measured as their "real" values. (Is it that we want to resurrect the "aether frame"?)

Bob Sciamanda
Physics, Edinboro Univ of PA (Em)
treborsci@verizon.net
http://mysite.verizon.net/res12merh/