Classics of modern science : $b (Copernicus to Pasteur)
History
Classics of modern science : $b (Copernicus to Pasteur)
Science; Science -- History
The last point is proven even more conclusively by the famous
experiment of Torricelli. [Fill a long closed glass tube with mercury,
then invert it.] The top of the glass tube not filled by the mercury
contains a high vacuum, but transmits light as well as when filled
with air. This demonstrates that there is within the tube some form
of matter different from air, and which penetrates either glass or
mercury, or both, though both are impenetrable to air. And if a like
experiment is tried with a little water on top of the mercury, it
becomes equally clear that the substance in question traverses either
glass or water or both.
In regard to the different methods of transmission of sound and light,
in the case of sound it is easy to see what happens when one remembers
that air can be compressed and reduced to a much smaller volume than
usual, and that it tends with the same force to expand to its original
volume. This quality, considered along with its penetrability retained
in spite of such condensation seems to show that it consists of small
particles that float about in rapid vibration in an ether consisting
of still more minute particles. Sound, then, is caused by the struggle
of these particles to escape when at any point in the course of a wave
they are more crowded together than at some other point.
Now the wonderful speed of light considered with its other qualities,
does not permit us to believe it to be transmitted in the same manner.
Therefore I shall try to explain the way in which I think it must
take place. I must first, however, describe that quality of hard
substances through which they transmit motion one to another. If one
take a number of balls of the same size of any hard substance, and
place them touching one another in one line, he will find that on
letting a ball of the same size strike against one end of the line,
the motion is transmitted in an instant to the other end of the line.
The last ball is driven from the line while the others are apparently
undisturbed, the ball that struck the line coming to a dead stop.
This is an illustration of a transmission of motion at great speed,
varying directly as the hardness of the balls. Yet it is certain that
this transmission is not instantaneous, but requires time. For if the
movement, or if you wish, the tendency to move, did not pass from one
ball to another in succession, they would all be set in motion at the
same instant and would all move forward at the same time. Now this is
so far from the case that only the last one leaves the row, and it has
the speed of the ball that first struck the line.
Public-domain text, read in full here on John Shaqi.
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