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FHSST Physics/Waves/Electromagnetic Applications
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Practical Applications of Waves: Electromagnetic Waves
In physics, wave-particle duality holds that light and matter
simultaneously exhibit properties of waves and of particles. This
concept is a consequence of quantum mechanics.
In 1905, Einstein reconciled Huygens' view with that of Newton. He
explained the photoelectric effect (an effect in which light did
not seem to act as a wave) by postulating the existence of
photons, quanta of energy with particulate qualities. Einstein
postulated that the frequency of light, , is related to the energy, , of its photons:
(2.3)
where is Planck's constant ().
In 1924, De Broglie claimed that all matter has a wave-like
nature. He related wavelength and momentum p:
(2.4)
This is a generalization of Einstein's equation above, since the
momentum of a photon is given by
(2.5)
where is the speed of light in vacuum, and .
De Broglie's formula was confirmed three years later by guiding a
beam of electrons (which have rest mass) through a crystalline
grid and observing the predicted interference patterns. Similar
experiments have since been conducted with neutrons and protons.
Authors of similar recent experiments with atoms and molecules
claim that these larger particles also act like waves. This is
still a controversial subject because these experimenters have
assumed arguments of wave-particle duality and have assumed the
validity of de Broglie's equation in their argument.
The Planck constant h is extremely small and that explains why we
don't perceive a wave-like quality of everyday objects: their
wavelengths are exceedingly small. The fact that matter can have
very short wavelengths is exploited in electron microscopy.
In quantum mechanics, the wave-particle duality is explained as
follows: every system and particle is described by state functions
which encode the probability distributions of all measurable
variables. The position of the particle is one such variable.
Before an observation is made the position of the particle is
described in terms of probability waves which can interfere with
each other.