The atom and the Bohr theory of its structure : $b an elementary presentation — John Shaqi
The atom and the Bohr theory of its structure : $b an elementary presentationHolst, Helge
Science
The atom and the Bohr theory of its structure : $b an elementary presentation
Holst, Helge
Atomic theory
In both light and sound the use of such terms as wave and wave motion
is figurative, for crests and troughs are lacking. But this choice of
terms is commendable, because sound and light possess an essential
property similar to one possessed by water waves. What happens when
a tuning-fork emits sound waves into the surrounding air, is that
the air particles are set in oscillation in the direction of the
propagation of sound. All the particles of air have the same period as
the tuning-fork, and the number of oscillations per second determines
the pitch of the note produced; but the air particles at different
distances from the tuning-fork are not all simultaneously in the same
_phase_ or condition of oscillation. If one particle, at a certain
distance from the source of sound and at a given time, is moving most
rapidly away from the source, then at the same time there is another
particle, somewhat farther along the direction of propagation, which is
moving towards the source most rapidly. This alternation of direction
will exist all along the path of the sound. Where the particles
are approaching each other, the air is in a state of condensation,
and where the particles are drawing apart, the air is in a state
of rarefaction. While the individual particles are oscillating in
approximately the same place, the condensations and rarefactions, like
troughs and crests in water, advance with a velocity which is called
the velocity of sound. If we call the distance between two consecutive
points in the same phase a wave-length, and the number of oscillations
in a period of time the frequency, then, as in the case of water waves,
the velocity of propagation will be equal to the product of frequency
and wave-length.
Light, like sound, is a periodic change of the conditions in the
different points of space. These changes which emanate from the
source of light, in the course of one period advance one wave-length,
_i.e._, the distance between two successive points in the same
phase and lying in the direction of propagation. As in the cases of
sound and water waves, the velocity of propagation or the velocity of
light is equal to the product of frequency and wave-length. If this
velocity is indicated by the letter _c_, the frequency by ν and
the wave-length by λ, then
_c_ _c_
_c_ = νλ or ν = ---- or λ = ---- .
λ ν
The velocity of light in free space is a constant, the same for all
wave-lengths. It was first determined by the Danish astronomer Ole
Rømer (1676) by observations of the moons of Jupiter. According to
the measurements of the present day the velocity of light is about
1,000,000,000 feet or 300,000 kilometres per second. In centimetres it is
thus about 3 × 10¹⁰.
Public-domain text, read in full here on John Shaqi.
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