Contents List:RecapitulationScientific Method Inference or Speculation? Observation Cosmology |
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One should expect a cosmological model based on Symmetrical Impermanence to contain some extensive clouds of very tenuous gas. In an expanding Universe, these would begin to form as soon as the distance between adjacent galaxies exceeded a certain critical value. At first, these clouds would grow rapidly in extent, while they still remained so tenuous that the gas between stars within our galaxy would have to be called dense in comparison. But when these extragalactic clouds had acquired a substantial gravitational field of their own, they would capture hydrogen from their surroundings and would also shrink under the influence of their own gravitational fields. Hence they would become more dense. But in spite of their smaller volume they would also become more massive, for loss from matter falling out of the cloud would cease and be replaced by gain from the matter that fell into it.
These clouds would bear but little resemblance to the spiral nebulae, and the closer study of their formation that is to follow shortly will not improve the resemblance. On the contrary, it will be found that the incipient clouds must differ quite significantly from spiral nebulae in shape, in size, in the way matter within them is distributed, and in their own intrinsic motion.
Can it then be inferred that the cloud will eventually develop into a spiral nebula — into a galaxy similar to those with which astronomers are familiar? If one cannot infer this, the cosmological model that is based on Symmetrical Impermanence does not resemble actuality — in which case this basic hypothesis must be abandoned and, with it, the even more basic Principle of Minimum Assumption. Much depends on whether one can infer from established knowledge and this principle that the extragalactic cloud can develop into a familiar spiral nebula.
For this reason it now becomes necessary to consider in detail what one should expect to happen to an extragalactic cloud after it has begun to form on an astronomical summit. But such consideration can with advantage be preceded by an appreciation of the task that it involves, and this will most easily be obtained, even though at the cost of some repetition, if I recall what has been said in Chapter 2 about scientific method.
To draw such inferences considerably taxes the engineer's powers of logical reasoning. It calls for great care lest some decisive factor be overlooked; it may require the use of some new mathematical tool; the design may have to be preceded by much experimental research of which the purpose is to extend the range of established knowledge. But in engineering, the new machine does not have to be manufactured and tried out before anything is known of its performance. The designer knows, of course, that some mistake or unforeseen circumstance may falsify his predictions, so his performance figures include margins, technically known as tolerances. When there is some doubt, a prototype may precede mass production. But these precautions do not imply that the engineer lacks all faith in his own powers of calculation and logical inference; and in the great majority of cases, experience shows a close agreement between inference and eventual performance.
There are sundry reasons for this; one is man's natural intellectual indolence. The detection of faulty reasoning requires a substantial mental effort, while other criteria can be applied with little or none. One of these false criteria is applied when the result of inference from established knowledge is dismissed as 'mere speculation'. If this happens more often than one should expect, it is because the difference between inference and speculation tends to be obscured.
A machine that has never been made is certainly unobservable at the time when the designer makes statements about its performance, and so the philosophers of this school would have to say that such statements could not be justified scientifically. These philosophers advocate a kind of empiricism that would make the engineer's task impossible. It is fortunate that most physicists, and all engineers, know better than to practise what is sometimes preached to them.
All this applies to the present theme. We are here trying to draw inferences about the behaviour of masses of gas so enormous that their movement is largely governed by their own gravitational fields. Such masses are not at the disposal of the laboratory technologist. The telescope tells us a little about them, but by no means all that we need to know. If we are to extend our knowledge in the field of cosmology, we must adopt the engineer's technique of inference. There is no alternative, and those who deprecate inference do not suggest one. One must either use this technique with the thoroughness and care of the machine designer, or abandon all hope of gaining a better insight into cosmological processes.