Presentation Speech by Professor C.W. Oseen, member of the Nobel Committee for Physics of the Royal Swedish Academy of Sciences, on December 10, 1926
Your Majesty, Your Royal Highnesses, Ladies
and Gentlemen.
Nature can be physically explained in two ways. When a group of
phenomena is to be understood, we can seek to deduce, on the
basis of observations, general laws from which it will be
possible to infer concrete phenomena. Or we can proceed from a
hypothesis on the structure of matter and seek to explain the
phenomena from that. These two methods have been exployed so long
as physical research has been carried out.
An example will allow me to show the difference between the
phenomenological and the atomistic description of Nature. We all
know that air is less dense at the top of a mountain than at
ground level. This phenomenon is explained completely by the laws
which govern a heavy gas, and there is no reason for not
considering the gas as a continuous medium. The problem is
herewith solved so far as the phenomenological description is
concerned. But for the supporters of the molecular theories the
results obtained in this way constitute only a superficial
description of the phenomena. For him, a gas evokes the image of
a multitude of molecules moving in all directions. Only an
explanation which reduces the phenomenon to the laws of molecular
movements can be satisfactory to him.
The object of the researches of Professor Jean Perrin which have
gained for him the Nobel Prize in Physics for 1926 was to put a
definite end to the long struggle regarding the real existence of
molecules.
The idea which Professor Perrin pursued in the early stages of
his researches was this. If it follows from the laws governing
the movements of molecules that in spite of its weight air is not
compressed against the surface of the earth, but that it extends
- while becoming rarefied, it is true - well above the highest
mountains, in that case, and seeing that the movements of
molecules obey the same laws as every other minute body, there
must be something analogous for every system of small bodies. If
a large quantity of sufficiently small and light particles is
distributed in a liquid, not all of them should yet settle at the
bottom even if they are heavier than the liquid, but they should
distribute themselves at different levels according to a law
similar to that for the air. Perrin, now, had to realize this
experiment.
He had for this purpose to prepare a system of very small
particles, all of which, moreover, should have the same weight
and the same size. He succeeded herein by using gamboge, a
preparation obtained from a vegetable sap and which can be
handled like soap. By rubbing the gamboge between his hands under
water, Perrin obtained an emulsion which under the microscope
proved to consist of a swarm of spherical particles of different
size. He then succeeded in obtaining from it an emulsion of
particles of the desired dimension and all of equal size. This
was by no means an easy operation which is proved by the fact
that after several months of accurate and careful work Perrin was
able to obtain from one kilogram of gamboge only some decigrams
of particles of the desired size. It then became possible to
undertake the experiment. The result was as expected. By means of
his gamboge emulsion Perrin was able to determine one of the most
important physical constants, Avogadro's number, that is to say
the number of molecules of a substance in so many grams as
indicated by the molecular weight, or to take a special case, the
number of molecules in two grams of hydrogen. The value obtained
corresponded, within the limits of error, to that given by the
kinetic theory of gases. Vast work to verify this, has not shaken
the soundness of the method.
It may perhaps be said that in the work which we have just
summarized Perrin has offered indirect evidence for the existence
of molecules. Here, follows a direct evidence. Microscopic
particles in a liquid are never at rest. They are in perpetual
movement, even under conditions of perfect external equilibrium,
constant temperature, etc. The only irrefutable explanation for
this phenomenon ascribes the movements of the particles to shocks
produced on them by the molecules of the liquid themselves. A
mathematical theory of this phenomenon has been given by Einstein. The first experimental proof
of this theory was given by a German physicist, Seddig. After
him, the problem was taken up by two scientists simultaneously.
One of them was Perrin; the other Svedberg. I have to speak of
Perrin only. His measurements on the Brownian movement showed
that Einstein's theory was in perfect agreement with reality.
Through these measurements a new determination of Avogadro's
number was obtained.
The molecular impacts produce not only a forward movement of the
particles distributed in a liquid, but also a rotational
movement. The theory of this rotation was developed by Einstein.
Measurements in relation herewith were carried out by Perrin. In
these measurements he has found another method for determining
Avogadro's number.
What then is the result of these researches ? How many molecules
are there in two grams of hydrogen? The three methods have given
the following answers to this question: 68.2 x 1022;
68.8 x 1022; 65 x 1022.
Professor Perrin. For more than thirty years you have worked with your head and your hands in the service of atomistic ideas. Please, accept our congratulations on the result that you have achieved. Allow me also to express the happiness which we experience in greeting you as a representative of the glorious sciences of France. I ask you to receive from the hands of our King the Nobel Prize in Physics for 1926.
From Nobel Lectures, Physics 1922-1941, Elsevier Publishing Company, Amsterdam, 1965
Copyright © The Nobel Foundation 1926