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Sunday, 30 October 2022

Accelerating `waves'

 Waves travel only at constant speed. We can see this in light of argument of u(x,t)=f(xvt) which is x=vt.

The fact that relativity and wave equation are so harmonious together is related to this: x=vt is first-order both in space and time. 

From u(x,t)=f(xvt) one can easily arrive at the 1D wave equation and from there it suffices to enter the 3D generalization of second derivative, Laplacian. 

Recently motivated by Milgrom's constant a0cH02π I was led to ask what is this acceleration a0?

It is not hard to speculate that it is the acceleration of light. But light is a wave (we are not indulging quantum mechanics yet) and a wave cannot accelerate. 

So how do we make a `wave' accelerate? Quite easy in fact: Pursuing the same method, we begin in 1D u(x,t)=f(x12at2vt) 

This yields 1v+att(1v+atϕt)=2ϕ 



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