TEXT A Any physical theory is
always provisional, in the sense that it is only a hypothesis: you can never
prove it. No matter how many times the results of experiments agree with some
theory, you can never be sure that the next time the result will not contradict
the theory. On the other hand, you can disprove a theory by finding even a
single observation that disagrees with the predictions of the theory. As
philosopher of science, Karl Popper has emphasized a good theory is
characterized by the fact that it makes a number of predictions that could in
principle be disproved or falsified by observation. Each time new experiments
are observed to agree with the predictions the theory survives, and our
confidence in it is increased; but if ever a new observation is found to
disagree, we have to abandon or modify the theory. At least that is what is
supposed to happen, but you can always question the competence of the person who
carried out the observation. In practice, what often happens is
that a new theory is devised that is really an extension of the previous theory.
For example, very accurate observations of the planet Mercury revealed a small
difference between its motion and the predictions of Newton’s theory of gravity.
Einstein’s general theory of relativity predicted a slightly different motion
from Newton’s theory. The fact that Einstein’s predictions matched what was
seen, while Newton’s did not, was one of the crucial confirmations of the new
theory. However, we still use Newton’s theory for all practical purposes because
the difference between its predictions and those of general relativity is very
small in the situations that we normally deal with. (Newton’s theory also. has
the great advantage that it is much simpler to work with than Einstein’s !
) It turns out to be very difficult to devise a theory to
describe the universe all in one go. Instead, we break the problem up into bits
and invent a number of partial theories. Each of these partial theories
describes and predicts a certain limited class of observations, neglecting
the effects of other quantities, or representing them by simple sets of numbers.
It may be that this approach is completely wrong. If everything in the universe
depends on everything else in a fundamental way, it might be impossible to get
close to a full solution by investigating parts of the problem in isolation.
Nevertheless, it is certainly the way that we have made progress in the past.
The classic example again is the Newtonian theory of gravity, which tells us
that the gravitational force between two bodies depends only on one number
associated with each body, its mass, but is otherwise independent of what the
bodies are made of. Thus one does not need to have a theory of the
structure and constitution of the sun and the planets in order to calculate
their orbits: Today scientists describe the universe in terms of
two basic partial theories-the general theory of relativity and quantum
mechanics. They are the great intellectual achievements of the first half of
this century. Unfortunately, however, these two theories are known to be
inconsistent with each other-they cannot both be correct. One of the major
endeavours in physics today, is the search for a new theory that will
incorporate them both-a quantum theory of gravity. We do not yet have such a
theory, and we may still be long way from having one, but we do already know
many of the properties that it must have. According to the last paragraph, the author may suggest that______.
A.either of the two partial theories may be correct B.the new theory has been established to replace the two partial theories C.the new theory may develop from either of the two partial theories D.the new theory may combine many of the properties of the two partial theories