Canonical Conjugates and Fourier Transforms in Classical Physics

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In quantum mechanics, the wave function can be transformed between conjugate pairs using Fourier transforms, a concept that raises questions in classical mechanics. When analyzing a particle in a potential well, the periodic trajectory of its coordinate can be represented as a triangle wave, while its momentum reverses at the walls. The Fourier transform of this triangle wave results in a squared sinc curve, suggesting that the momentum distribution consists of two delta functions, indicating momentum values at p and -p. This leads to the inquiry of whether Fourier transforms provide meaningful insights into conjugate pairs in classical physics. The discussion highlights the complexity of relating classical and quantum mechanics through mathematical transformations.
Mark Spearman
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In quantum mechanics one can convert the wave function of one variable into the wave function of its conjugate pair (e.g., momentum and coordinate) using a Fourier transform.

Now consider the classical case. Suppose there is a particle in a potential well with insufficient energy to escape thereby resulting in a cyclic trajectory for the coordinate
q(t). What does the Fourier transform of q(t) over its period tell us about its momentum?

Perhaps it tells us nothing. Consider the simple case of a (classical) particle in a box with initial velocity of v and mass m. The periodic behavior of q(t) is a triangle wave while the momentum will be p = mv, reversing instantaneously at the walls of the well. The Fourier transform of a triangle wave is a squared sinc curve. It would appear that the distribution of p would be two delta functions, one at p and the other at -p.

So, does the Fourier transform tell us anything about conjugate pairs in classical physics?

Thanks,

Mark
 
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Good evening, Mark.

Can I commend to you the book about just this subject:

The Use of Integral Transforms

Ian Sneddon

He treats lots of transforms and applications as well as Fourier eg the Mehler-Fock transform in fracture mechanics.

go well
 
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