[net.physics] Why believe physics?

stern@bnl.UUCP (Eric Stern) (04/04/85)

        With the reappearence of the old debate  on  whether
all those who question scientific theory should be heard out
or not, I thought I  would  clarify  the  situation  of  how
theories  get to become accepted, and why the current system
acts to prevent the acceptance of false opinion  and  dogma.
Along  the way, I will discuss the related issues of experi-
mentation and theories, and peer review of scientific work.

        In general, theories do not  develop  in  a  vacuum.
There  is usually a body of knowledge that requires explana-
tion.  This body of knowledge is acquired through experimen-
tation.   What  experimenters do is to measure parameters of
phenomena.  Sometimes, they are verifying existing theories,
or  searching  for  deviations  from theories, but sometimes
they also perform searches for new phenomena independent  of
any  theories.   This provides the grist for the mill of new
theories.

     When they perform experiments  and  make  measurements,
the  answer  they  come  up  with  is subject to independent
verification.  An experiment that nobody  can  reproduce  is
not considered to be valid.  This is happening all the time.
For instance, an experiment has been done at  Stanford  that
seems to observe fractional charge, by a method based on the
Millikan oil drop experiment, only  this  one  uses  charged
niobium  spheres.   The  result  would  seem to indicate the
existence of free quarks, which have  not  been  seen  else-
where.   In  fact, the Stanford experiment has been repeated
at other institutions, with  a  null  result.   Because  the
Stanford  result  is  not reproducible, free quarks are con-
sidered to be unobservable.

     The result of an experiment is expected to  include  an
experimental  error.   The experimenter estimates the magni-
tude of deviation from the quoted value that he or she  con-
siders possible, given the nature of the measuring apparatus
and procedure.  The experimenter cannot cheat  and  quote  a
error  that  is  too  small, lest a future experiment make a
measurement which does not agree within  the  error  limits.
If  the  error  quoted  is  too large, to insure that future
experiments will agree, the experiment is considered  to  be
worthless  in  the  eyes of the scientific community.  After
all, if there is such a large error on the measurement, they
think,  it  is  no  better than no measurement at all.  Once
several experiments agree on a  phenomenon,  those  measure-
ments  enter the general body of knowledge and become candi-
dates for theoretical explanation.

     So, Joe Experimentalist discovers a new phenomenon  and
gets  a Nobel Prize.  There is still this matter of an unex-
plained observation to deal with.  How  does  one  go  about
cooking  up  a  theory?   One  cannot  make  up an arbitrary
theory, there are guidelines that should be observed.  A new
theory  can't  directly  invalidate  an old theory.  The old
theory  did  perfectly  well  at  explaining  its   set   of
phenomena.   The new theory must include the old theory as a
special case; it must reduce to the old theory in the  limit
of  a  regime where the old theory held.  This point must be
stressed.  Old theories don't die, they just  become  incor-
porated  into  new ones.  The two great new theories of this
century, special relativity and quantum  mechanics,  conform
to  this  principle.   Classical  Newtonian Mechanics is the
limit of special relativity considered at  velocities  small
compared  to  the speed of light.  Quantum mechanics reduces
to  classical  mechanics  in  the  limit  of  large  quantum
numbers.

     The two examples above illustrate something in physics,
that,  while  is  not a fixed law, is a general principle of
operation.  That is, new phenomena occur  when  new  regimes
are  looked  at  for the first time.  Quantum effects become
noticable on the microscopic scale, and  special  relativity
becomes apparent at high velocities.

     Another good thing to have in a new theory is  general-
ity  or  universality.   Physicists  hate special cases, and
find the idea of a theory that just applies to one thing, to
be  morally  repugnant.   Good  theories should explain many
different kinds of effects without  making  special  assump-
tions  about  each  one.   Proliferation  of theories and of
assumptions is something to avoid.  The best clue  a  physi-
cist  has,  that  a  theory  is not fundamental, or just not
working, is when new assumptions, new  principles,  and  new
laws have to be continually added to a theory to make it fit
the data.

     Let us look at this in practice.  The geocentric  views
of  planetary  motion  were  very  complicated  indeed.  The
planets moved around the sky, but periodically,  they  would
reverse  their  motion.  Furthermore, each planet had a dif-
ferent manner of behavior that varied with the time of year.
Then Kepler came along.  Kepler showed that from a heliocen-
tric point of view, the sky is very  simple.   The  apparent
oddities  of  planetary  motion arise from the motion of our
own viewpoint.  All objects orbiting the sun share a  common
pattern,  a  relationship  between the orbit period, and the
orbit distance that holds for all planets.

     Another example of universality relates  to  chemistry.
In  the  1700's  and 1800's, many new chemical elements were
discovered.  They all seemed to have different chemical pro-
perties.   Mendeleev  arranged  the  elements  in  a  table,
ordered by atomic weight, and  found  a  repeating  pattern.
Elements  separated  by  a  certain  amount in the table had
similar chemical properties.  Later on,  it  was  determined
that atoms consist of smaller particles, and it was the con-
figuration of these constituent  particles  that  determined
the  chemical  behavior  of  the  atom.   But, the clue that
something funny was going on was the  proliferation  of  the
number  of  elements, and the discovery of a pattern made it
obvious that there was an underlying principle.

     The story is not  over  when  a  successful  theory  is
found.   The new theory continues to undergo tests to deter-
mine its applicability in new situations.  Even  well  esta-
blished  theories  are  tested  anew,  when  improvements in
experimental technology allow more sensitive measurements of
a  theory's  validity.   The  Coloumb inverse square law for
electric and magnetic fields,  which  was  discovered  about
1770  are  tested as better techniques become available.  A.
S. Goldhaber wrote a Scientific  American  article  in  1979
describing  experiments  which verify the inverse square law
by observing the Earth's magnetic field.  An observed devia-
tion  from  the  inverse  law  would imply a non-zero photon
mass, which would have many consequences.

     An established theory is used as  the  basis  to  build
more  theories.  Physics advances by building new structures
on top of old ones.  Conversely, new theories depend on  the
validity  of  previous  theories.  Every new theory verified
acts to confirm the theories upon which it is built.

     With that preface out of the way, we can ask  the  real
question  that prompted this article: what are the odds that
someone working independently of the "scientific  establish-
ment"  discovers  something wrong in a basic theory, such as
classical electrodynamics?  Well, it has to be pretty  small
odds.   The  "scientific establishment" has been working for
over 100 years testing its own basic premises.  If something
was  wrong  with  a  basic theory, we would be seeing incon-
sistencies in later work based on those same basic theories.
In  fact,  something  wrong  *was* discovered in about 1890.
Classical mechanics seemed to be inconsistent with  electro-
dynamics.   That  was  just one problem.  Radiation calcula-
tions based on electrodynamics indicated that all the  elec-
trons  orbiting  nuclei  would  radiate all their energy and
crash into the nucleus.  This  was  the  great  "Ultraviolet
Catastrophe", so named because the radiation given off would
be high frequency, low wavelength, hence  ultraviolet.   The
resolution  of  these  two  problems  eventually  led to the
development of special relativity,  quantum  mechanics,  and
finally  quantum  electrodynamics.   As it happens, the most
precisely verified quantity known is the gyromagnetic  ratio
of  the  electron.   This  property of the electron has been
measured to over eight  significant  figures  and  found  to
agree  with  the value predicted by quantum electrodynamics.
The correctness of quantum electrodynamics implies the vali-
dity  of  almost  every  previous theory including classical
mechanics, classical electrodynamics, quantum mechanics  and
special  relativity.  So it seems, if past experience is any
guide, physics is quite capable of recognizing its own prob-
lems and dealing with them.

     Current physical theory is the result of  several  hun-
dreds of years of work by people who didn't necessarily like
each other, and includes results of thousands of experiments
verifying  the theories.  Because of all this work, a physi-
cist feels confident in rejecting the assertions of  someone
who gets the idea that physics is wrong.  The views of those
who feel that rejecting such notions is  equivalent  to  the
treatment  given  Gallileo and Capernicus may be answered by
noting that prior to these visionaries, there was  no  esta-
blished  science.  At that time, ideas of the physical world
were dictated by preconceived notions  having  no  basis  in
observation.

     Physics, in the final analysis is  totally  based  upon
experimental  observations.   There  is no accepted physical
theory which can't be demonstrated  to  be  correct  in  the
laboratory.  Given the large body of knowledge that has been
collected about the laws of the universe, and the demonstra-
tion by several independent experimenters of the validity of
the procedures used to accumulate this knowledge, the  ines-
capable  conclusion  is  that  the  theories which have been
developed to explain the observations must reflect the  true
behavior of the universe.


				Eric G. Stern
				Dept. of Physics
				SUNY StonyBrook
				StonyBrook, NY 11794
				stern@bnl.arpa
				stern@bnl.bitnet
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