[Editor's Note: The following extended extracts have been reprinted with the
kind permission of the author and the original publisher, Cambridge
University Press. The original and complete essay appeared in the book "Three
hundred years of gravitation", ed. S. W. Hawking and W. Israel, Cambridge
University Press, pp 5-16 (1987), copyright Cambridge University Press 1987.
Any reproduction of this material must first receive the written consent of
Cambridge University Press, 40 West 20th Street, N.Y., N.Y. 10011]
Newtonianism and today's physics
________________________________
Steven Weinberg
University of Texas
Austin, Texas
(first printed - Vol. 2, No. 7 - March, 1996)
Newton was a complicated man, who lived in complicated times. It would
take the talents of a historian to say anything new and useful about Newton
himself. I am not a historian, and know better than to try. I am a physicist,
and will talk here not about Newton, but Newtonianism; that is, about Newton's
work, his achievement, as an example which over the last three hundred years
has guided the evolution of the science in which I now work; Newton, in other
words, to use a much over-used word, as paradigm.
The central part of the Newtonian achievement I suppose is his theory
of the solar system, which had three parts, each one of which would by itself
guarantee his immortality. First, there is Newton's theory of gravity, which
explains how the distribution of all the matter in the universe determines the
gravitational force on any one particle, whether that particle is a particle
here on earth or a particle on the sun or the moon or the stars. Second, there
is a law of motion that describes how, given the forces acting on a particle,
one can calculate its motion. Third, there is a method of calculation, the
mathematical tool now known as calculus. ...
The first question that I as a physicist should address is: how well
does it work? How does Newtonianism stand up after three hundred years of
experimental testing? It stands up very well. We do now understand that there
are small corrections to the Newtonian picture of gravity and dynamics. The
most interesting and important corrections are those provided by Einstein's
general theory of relativity, but they're awfully small. ...
However, whether the corrections are large or small doesn't seem to me
to be the point. In 1919, when Einstein's theory began to be popular, The
Times of London proclaimed that Einstein had disproved Newton. That's very far
from the truth. Einstein's theory reduces to Newton's theory in the limit of
slowly moving bodies at large distances from each other, which is certainly
true of the outer part of the solar system ,and indeed of most of the
universe.
In fact, it is fair to say that, not only does Einstein's theory not
supplant Newton's theory, it explains Newton's theory. ...
Newton's theory then works very well, and it now has a rationale that
it lacked in Newton's time, provided by general relativity. We use it to
follow the motion of objects in the solar system, some of them objects that we
put there ourselves. I think nothing was more dramatic as an example of our
faith in the Newtonian theory than the Apollo project. In its early stages,
remember that astronauts were sent out in spacecraft which circled the moon,
orbited several times, were given a little boost from a rocket motor, and then
came back to the earth with essentially all the fuel gone; just relying on the
validity of Newton's laws. It was somehow very appropriate that Major William
Anders on the return from the first circumlunar voyage in December 1968, made
the remark,'I think Isaac Newton is doing most of the driving right now.'
So Newton's theory is not challenged as a theory of the solar system.
What about Newton's theory as a model for physical theory in general?
. . .
I would not say that either the broad picture of a deterministic
mechanical universe, or the particular details of Newton's law of gravity, or
Newton's equation of motion, or even the invention of the calculus constitute
the heart of the Newtonian achievement. In preparing this, I did some soul
searching about why Newtonianism seems to me to be such an incredible
watershed in the history of our species. I think it is because with Newton's
work mankind for the first time saw the glimpse of a possibility of a
comprehensive quantitative understanding of all of nature.
Now of course Newton was not the first person to think about nature in
quantitative terms. The Hellenistic Greeks, such as Eratosthenes, Ptolemy, and
Archimedes, and then in the century before Newton physicists like Huygens and
Galileo, were masters at bringing quantitative methods to bear on physical
reality. Also Newton was not the first person who tried to think about nature
in comprehensive terms, who tried to make a unified theory of everything. That
goes back even further than the Hellenistic Greeks, to Thales and Anaximenes,
and then, closer to Newton's time, Descartes. But the two styles had never
come together before. Those who thought comprehensively about nature from
Thales to Descartes had never confronted the necessity of carrying their
comprehensive world picture through to a quantitative understanding of nature
in all its aspects. And those who thought quantitatively about nature had
never seen the beginning of a hope of formulating laws that would describe
everything.
With Newton, for the first time one saw the possibility of a
quantitative understanding of everything, not just the motion of the planets
around the sun, but of all physical phenomena. Newton showed us what could be
done. In this sense, the most important part of Newton's opus was not his
theory of planetary motion, but his theory of the motion of the moon, in book
three of the Principia. There Newton observes that on earth the force of
gravity makes objects fall with a certain acceleration, which can be described
by saying that a body allowed to drop from rest in the first second will fall
sixteen feet. The surface of the earth where we do our experiments is a
certain distance from the center of the earth, and Newton knew that you could
think of the earth as if all its mass was concentrated at the center. The moon
is sixty times farther from the center of the earth than we are here on the
earth's surface, so from the inverse square law the moon, if allowed to drop
from rest, in the first second should fall not sixteen feet, but an amount
less than that by a factor of sixty squared, or 3600. You can easily work out
that sixteen feet divided by 3600 is about a twentieth of an inch. So if you
let the moon drop from rest, it should fall toward the earth a twentieth of an
inch in the first second. Now of course the moon isn't at rest, it's going
around in a circular orbit, but it's really the same thing. If the moon were
not attracted to the earth it would go off in a straight line, a tangent to
wherever it was in its orbit at that moment. Instead of going in a straight
line it curves toward the earth; that's what a circle does. And any one second
it curves toward the earth an amount which brings it closer to the earth than
if it had gone in a straight line in that second by an amount which is in fact
just a twentieth of an inch. The beautiful thing about this argument is that
Newton was not just relating celestial phenomena to each other. He was
relating a celestial phenomenon, the moon's orbit, to something here on earth,
an apple falling on his head in Cambridgeshire. (No, I don't know if the apple
ever fell on his head.) Newton broke down the barrier between the celestial
and terrestrial styles in physics, and in so doing he not only demystified the
heavens, he opened up the possibility of an understanding which would embrace
the heavens and the earth, all in one synthesis.
. . .
But Newton of course only provided us with a glimpse of a really
comprehensive system of nature. Newton knew there were other forces in nature
besides gravitation, and he knew that he didn't know what they were, but he
hoped that the same kind of mathematical reasoning, the same clarity of vision
that had revealed the nature of the force of gravitation through its role in
the solar system, would reveal the nature of the other forces, and their role
governing all the phenomena of nature. In the preface to the first edition of
the Principia, which Newton wrote at Trinity College on 8 May 1686, he said,
'I wish we could derive the rest of the phenomena of nature by the same kind
of reasoning for mechanical principles, for I am induced by many reasons to
suspect that they may all depend on certain forces.' But he didn't know what
those forces were, and it took a long time to understand what they were. There
was the understanding in the nineteenth century by organic chemists that the
chemicals of living things were not subject to separate chemical laws, but
were subject to the same chemical laws as ordinary inorganic chemicals. There
was the understanding by Darwin and Wallace that the growth of various species
of living things on earth did not have to be accounted for by some extra
biological laws separate from the ordinary laws of physics and chemistry, but
could be accounted for by the operations of chance on inheritable variations
among organisms. There was the realization by Maxwell that light was not
something separate from the rest of nature, but was a manifestation of
oscillating electric and magnetic fields.
And so on. These were all great steps in the development of a unified
view of nature, but by the beginning of the twentieth century we were still a
long way from understanding even the possibility of a really unified view.
. . .
So it goes. Newton's hope,'I wish we could derive the rest of the
phenomena of nature . . .', has not been fulfilled, but we are working on it,
very much in the Newtonian tradition: the formulation of increasingly
comprehensive quantitative laws. From this high viewpoint, all that has
happened since 1687 is a gloss on the *Principia*.