Every-day Science: Volume 7. The Conquest of Time and SpaceWilliams, Henry Smith
History
Every-day Science: Volume 7. The Conquest of Time and Space
Williams, Henry Smith
Transportation
If you have taken the trouble to follow carefully the description just
given, you will be prepared to understand the anomalies of action of
the gyrocar; for example, why its side rises when a weight is placed
on it; why it leans toward the wind, and why it leans to the inner and
not to the outer side of the track in rounding a curve. The substance
of the explanation is that the greater the force brought to bear on
the roller R1 by the segment of the car that strikes against it, the
stronger its precession, and hence the more powerful its lift. The
oscillations and counter-oscillations thus brought about continue to
operate powerfully on the roller R1 so long as the weight of the car is
out of balance; and balance is restored only when the heavier side of
the car rises, bringing the centre of gravity over the track, just as a
man carrying a weight on the right shoulder leans toward the left, and
vice-versa. Thus, when the gyrocar has a heavy weight on one side, or
encounters a strong wind, it may lean far over, but still be perfectly
and securely balanced, the gyroscopes finally remaining quiescent in
their new position until some new disturbance is applied.
It remains to be said, however, that there is another element
introduced when the car rounds a curve. To understand this, we must
revert to the action of the Foucault gyrostat, as illustrated in
diagram 1. If you held such a gyrostat in your hand in the upright
position in which it is shown in the diagram, and whirled it about, the
axis _O A_ would of course maintain a fixed direction so long as the
gyrostat was free to revolve on the axis _D E_. But if you prevented
such revolution, as by clutching the spindle _E_ firmly, and then
whirled the gyrostat about at arm's length, the axis _O A_ would at
once be forced to take an upright position. If your hand whirled to
the right, the point _A_ would rise; if your hand whirled to the left,
the point _A_ would go down; the principle determining this motion in
either case being that the direction of whirl of the gyroscope must
correspond to the direction of curve given to the apparatus as a whole
by the motion of your arm.
Public-domain text, read in full here on John Shaqi.
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