The Principle of Least Action
Selected references.
Maupertuis
[In 1746 Maupertuis formulated] the Principle of Least Action,
which is all too commonly credited to one of the three great
mathematicians, Euler, Lagrange, and Hamilton, who further
developed it. This Principle is indeed one of the greatest
generalizations in all physical science, although not fully
appreciated until the advent of quantum mechanics in the present
century. Maupertuis arrived at this principle from a feeling
that the very perfection of the universe demands a certain
economy in nature and is opposed to any needless expenditure
of energy. Natural motions must be such as to make some quantity
a minimum. It was only necessary to find that quantity, and this
he proceeded to do. It was the product of the duration (time)
of movement within a system by the "vis viva" or twice what
we now call the kinetic energy of the system. Having found the
quantity that tends to a minimum, Maupertuis regarded the
principle as all-inclusive: "The laws of movement and of rest
deduced from this principle being precisely the same as those
observed in nature, we can admire the application of it to
all phenomena. The movement of animals, the vegetative growth
of plants ... are only its consequences; and the spectacle of
the universe becomes so much the grander, so much more
beautiful, the worthier of its Author, when one knows that
a small number of laws, most wisely established, suffice for
all movements." This sort of talk aroused vigorous opposition.
Translated into recent biological terminology, however,
what is it other than Claude Bernard's principle of the
maintenance of the internal environment, W.B. Cannon's
principle of homeostasis, or the principle of Le Chatelier:
"In a system in equilibrium, when one of the factors which
determine the equlibrium is made to vary, the system reacts
in such a way as to oppose the variation of the factor, and
partially to annul it.1
"Le Grand principe que la nature, dans la production de ses
effets, agit toujours par les voies les plus simples."
2
Leibniz
Leibniz in Tentamen Anagogicum, "On ne regarde pas au plus
grand ou au plus petit, mais generalement au plus determine
ou au plus simple."3
Euler
In his 1748 paper, Euler in "Reflexions sur quelques loix
generales de la nature.." starts by declaring his commitment
to the least-action principle. His expression corresponds to
what we would now call potential energy, so that his statement
of least action in statics is equivalent to the principle that
a system of bodies at rest will adopt a configuration that
minimizes total potential energy. Euler called this quantity
"effort".3
Fermat, Hamilton, Thomson, Feynman
Geodesy, as the term is used in physics, is the tendency of
physical changes and processes to take the easiest or minimum
path. Almost the whole of physics can be represented in
geodetic form. Water running downhill seeks the steepest
descent, the quickest way down, and water running into a basin,
even one with irregular shape and bottom, distributes itself
so that its surface is as low as possible, the water then
has the minimum potential energy in the earth's gravitational
field. Light finds the quickest trajectory through an optical
system (Fermat's principle of Least Time). The path of a body
in a gravitational field (i.e. free fall in space time) is a
geodesic. Feynman's formulation of quantum mechanics is based
on a least-action principle, using path integrals. Maxwell's
equations can be derived as conditions of least action.
Newton's mechanics is contained in Hamilton's principle of
least action, and also Gauss's principle of least constraint.
Thomson's theorem states that electrically charged particles
arrange themselves so as to have the least energy. The Second
Law of Thermodynamics requires that thermal systems change
along a sequence of configurations, each having a higher
probability of occurrence than the preceding configuation.
4
When light goes through optical systems, it finds the path
of least time, taking short cuts in glass and water, where
light travels slower, and longer paths through air... The
problem for the physicist is like that of figuring out the
quickest way of reaching a person drowning down the beach from
you... You run down the beach to almost the point where you
are nearest the drowning person, then plunge in and swim.
4
Pierre Louis Moreau de Maupertuis, b. 1698, member of the
Royal Society, seems to have been an interesting character.
He became a disciple of Newton and
converted Voltaire and others to the Newtonian view. In 1736 he
went on an expedition to Lapland to test the flattening of the earth
at the poles. He attempted a calculus of pain and pleasure, studied
hexadactylism in family trees, developing a theory of heredity.
And he anticipated the survival of the fittest:
"May we not say that, in the fortuitous combination of the
productions of Nature, since only those creatures could
survive in whose organization a certain degree of adaptation
was present, there is nothing extraordinary in the fact that
such adaptation is actually found in all those species which
now exist? Chance, one might say, turned out a vast number of
individuals; a small proportion of these were organized in
such a manner that the animal's organs could satisfy their
needs. A much greater number showed neither adaptation nor
order; these last have perished... Thus the species which
we see today are but a small part of all those that a blind
destiny has produced. (Maupertuis. Essaie de cosmologie, 1750)
1
References.
- Forerunners of Darwin. Glass, Temkin, Strauss. Johns Hopkins. 1959
- Maupertuis. Oeuvres.
- Maupertuis: an intellectual biography. David Beeson. The Voltaire
Foundation. 1992.
- Six Roads from Newton. Edward Speyer. Wiley. 1994.