{"id":394698,"date":"2024-06-29T11:46:49","date_gmt":"2024-06-29T11:46:49","guid":{"rendered":"http:\/\/savepearlharbor.com\/?p=394698"},"modified":"-0001-11-30T00:00:00","modified_gmt":"-0001-11-29T21:00:00","slug":"","status":"publish","type":"post","link":"https:\/\/savepearlharbor.com\/?p=394698","title":{"rendered":"Let\u2019s Discuss the Lorentz Transforms \u2013 Intermission: Rapidity, and What it Means<\/span>"},"content":{"rendered":"
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I thought my previous post<\/a> rather funny, and was surprised seeing it initially receive so few views. I thought the entertainment flopped, but fortunately I was wrong. I therefore feel it my duty before my readers to address the subject of the Landau & Lifschitz proof of the invariance of the interval.<\/p>\n

You can find the summary<\/a> of it in Wikipedia. Making their starting point the light-like interval always being equal to zero, Landau & Lifschitz seem to make a great fuss about it. The Wikipedia article even says: \u2018This is the immediate mathematical consequence of the invariance of the speed of light.\u2019 No, it is not.<\/p>\n

I beg everyone\u2019s pardon, but the light-like interval always being equal to zero is nothing else but the following statement: \u2018The length of a ray of light will always be equal to the length of this ray of light\u2019. Sounds like a cool story, bros and sis, but I cannot see what further inferences can be drawn from it. The \u2018proof\u2019 of this truism cannot fail under any circumstances whatever \u2013 whether you keep the speed of light invariant, or keep or change the metric of space or time or both \u2013 or make both metric and speed of light change \u2013 the light-like interval will remain equal to zero. I am okay with anyone wanting to prove it if they feel like it, but you cannot make it an \u2018immediate mathematical consequence of the invariance of the speed of light\u2019. Neither is it possible to make the constancy of the speed of light a consequence of the invariance of the light-like interval for the reason already mentioned: this is a truism. It does not prove anything, nor can it be a consequence of anything. When Landau & Lifschitz insist that this is a consequence of the constancy of the speed of light, that is either an error or a downright subterfuge, a means employed to create a spectre of logical connection between two unconnected notions, and charge this ghostly connection with pretended significance. And, since the following proof of invariance of an arbitrary interval hangs on the invariance of the light-like interval, we can altogether dismiss it: the necessity of introduction of such a measure as interval cannot be derived from the statement that a length of something will be equal to itself in whatever frame of reference it is measured.<\/p>\n

For today\u2019s topic now. We need this preliminary discussion to get prepared for the final of this longish saga.<\/p>\n

In 1910, Vari\u0107ak discovered that one can introduce an additive measure directly corresponding to the velocity in the place of the Einstein non-additive velocities \u2013 later, this measure c\u00a0artanh(v\/c)<\/em> came to be known as \u2018rapidity\u2019.<\/p>\n

What can this additivity of rapidity mean?<\/p>\n

For the simple case of the parallel motion, Einstein (Einstein, p. 11) is very straightforward when deducing the formula of the velocity addition. His derivation is done for a more general case of coplanar velocities \u2013 we do not need this, and will be discussing an even simpler case of parallel velocities, but reproducing Einstein\u2019s logic. He is considering a point moving relatively to the moving frame of reference at a speed w, <\/em>and its coordinate x’ <\/em>is changing as x’\u00a0=\u00a0wt’<\/em>, whence, if x’\u00a0=\u00a0\u03b3(x \u2013 vt)<\/em> and<\/p>\n

<\/figcaption><\/figure>\n

we get<\/p>\n

<\/figcaption><\/figure>\n

or<\/p>\n

\"(1)\"
(1)<\/figcaption><\/figure>\n

the right-hand part of (1) being the formula for the resulting speed of the point in the unprimed frame of reference k<\/em> (velocity addition) in the Einstein mathematics.<\/p>\n

This straightforwardness, however, is a little puzzling. It looks okay to consider motion of a point, but add a second point located at the infinitesimal distance dx’<\/em> to the first one, and you will get that your parallel translation does not preserve distances (and therefore stops being a parallel translation). But it is not what we are after today.<\/p>\n

To get to the bottom of this velocity composition, let us suppose that what Einstein means by x’\u00a0=\u00a0wt’ <\/em>is nothing else but the function x’\u00a0=\u00a0(w\/c)ct’ <\/em>in the (ct’, x’, y’, z’) <\/em>coordinate system in a 4-space of hyperbolic curvature, or to be even more exact, the graph<\/em> of this function drawn in this coordinate system. In that case, w\/c<\/em> should be the hyperbolic tangent of the angle between the graph line and the ct’<\/em> axis, and that in its turn would mean that the \u2018velocity addition\u2019 problem is about finding the hyperbolic angle between the graph line and the ct<\/em> axis, or the tangent of that angle.<\/p>\n

Indeed, in the Einstein velocity addition formula one can easily recognize the sum of two area hyperbolic tangents:<\/p>\n

\"(2)\"
(2)<\/figcaption><\/figure>\n

whence the new tangent u\/c<\/em> resulting from the \u2018added velocity\u2019 w<\/em> will be<\/p>\n

<\/figcaption><\/figure>\n

We can go further and see that the form of (2) suggests that the motion of k’<\/em> is also being considered as a graph of the function x\u00a0=\u00a0(v\/c)ct <\/em>in the (ct, x) <\/em>plane. Velocities being non-additive become clear in this perspective: if we need to find a sum of two angles, it will be useless to add up their tangents. Velocities are non-additive because they are tangents, and the rapidity c\u00a0artanh(v\/c)<\/em> is additive since it is the angle.<\/p>\n

This passing remark, though rather elementary, will be helpful for the discussion to come.<\/p>\n

To be continued<\/p>\n

Literature<\/p>\n

[1] Einstein, A. On the Electrodynamics of Moving Bodies; available here<\/a><\/p>\n

[2] Landau, L.D.; Lifshitz, E.M. The Classical Theory of Fields. Course of Theoretical Physics. Vol.\u00a02<\/p>\n

[3] Vari\u0107ak, V. Anwendung der Lobatschefskijschen Geometrie in der Relativtheorie, found here<\/a> <\/p>\n

Previous parts<\/p>\n