Friday, June 23, 2017

quantum mechanics - Why do we obtain classical physics by taking the limit of Planck's constant to zero?


Why if we specifically set Planck's constant equal to zero (the limit of it) do we sometimes get classical physics? I mean, what does it mean physically to set the constant equal to zero? Or to say it in another way, what did the first human to do this think of in order to come up with it?
I have seen in various situations somebody taking h-->0, but what is making anybody who does this to take h-->0 in the first place? Why would somebody take h-->0 to take the classical limit in the first place?



Answer



In classical physics there exists no h, and everything was going happily along until the data/measurements showed that classical electrodynamics + classical mechanics could not explain a number of data.


The datum that introduced the otherwise unknown and undefined h_bar was black body radiation. It was not possible to reconcile the fact that no excess ultraviolet radiation was observed from the experimental study of the radiation from bodies in the lab. Planck had the brilliant idea to assume that the electromagnetic radiation was not continuous but came in quanta of energy h*nu, where nu is the frequency, and could fit the data. Thus the constant took his name. It became obvious that a new framework for physical observations was emerging.


When the photoelectric effect, and then the spectra of atoms appeared in the labs the new framework became consistent by using this h*nu identification for photons that make up light. These data are not classical physics. Quantum mechanics was developed to explain it, and it soon became clear that all classical observations emerged from an underlying quantum mechanical framework, and this can be proven with advanced mathematical methods. For example, the way the classical electromagnetic radiation is built up by photons.


A second foundation stone for quantum mechanics is Heisenberg's Uncertainty Principle. , HUP . This is what sets the stage for deciding whether quantum mechanical methods are needed or whether classical theories are adequate. For example


HUP


this inequality does not hold for classical physics, since h is a very small number. The constraints of the inequality appear at the level of particle physics, for micrometers and lower values. The statement that one gets classical physics when h is zero comes from the observation that classical momenta times classical dimensions multiplied have no lower bounds up to dimensions of micrometers and smaller . The handwaving statement "one gets classical physics if h is zero" is based on this relation.



The HUP is in the foundation of the mathematics of quantum mechanics, it appears in the commutator and anticommutator relations of operators representing measurable observables, like position and momentum. If h is zero, one has to fall back on the classical theories. , the consistency check also needs advanced mathematics to see the correspondence.


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