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
The same characteristic phenomenon made evident in the passage of
α-particles through substances by the investigations of Rutherford
appears in a more direct way in Wilson’s researches discussed on
p. 81. His photographs of the paths of α-particles through air
supersaturated with water vapour (see Fig. 22) show pronounced kinks
in the paths of individual particles. Thus in the figure referred
to, there are shown the paths of two α-particles. One of these is
almost a straight line (with a very slight curvature), while the
other shows a very perceptible deflection as it approaches the
immediate neighbourhood of the nucleus of an atom, and finally a very
abrupt kink; at the latter place it is clear that the α-particle has
penetrated very close to the nucleus. If one examines the picture
more closely, there will be seen a very small fork at the place where
the kink is located. Here the path seems to have divided into two
branches, a shorter and a longer. This leads one at once to suspect
that a collision between two bodies has taken place, and that after the
collision each body has travelled its own path, just as if, to return
to the analogy of the bombardment of the butter wall, one had been
able to drive two pellets out of the butter by shooting in only one.
Or, to take perhaps a more familiar example, when a moving billiard
ball collides at random with a stationary one, after the collision
they both move off in different directions. So, when the α-particle
hits at random the atomic nucleus, both particle and nucleus move off
in different directions; though in this case, since the nucleus has
the much greater mass of the two, it moves more slowly, after the
collision, than the α-particle, and has, therefore, a much shorter
range in the air than the lighter, swifter α-particle. Had the gas in
which the collisions took place been hydrogen, for example, the recoil
paths of the hydrogen nuclei would have been longer than those of
the α-particles, because the mass of the hydrogen nucleus is but one
quarter the mass of the α-particle (helium atom).
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