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
Our diagram 2, then, will represent one of Mr. Brennan's gyroscopes
in action. It is pivoted into the framework of the car on the axis _D
E_. If you examine it you will see that it is essentially the Foucault
gyrostat of our other diagram, with the axis _O A_ projected beyond the
frame to the point _F_.
In practice, the frame _B A C_ is made to carry the field-magnet of
an electric motor for spinning the wheel. But this in no wise affects
the principles of action. Mr. Brennan's invention consists of the
exceedingly ingenious way in which he applies these principles; and
to understand this we must follow our diagram closely. Looking at it,
you will see that the spindle _O F_ carries two rollers _R1_ and _R2_
which may come in contact under certain circumstances with the curved
segment marked _G1_, _G2_, _G3_, _G4_, which are strong segments of
the car-frame itself--the segments, indeed, upon which the force
of the gyroscope is expended in holding the car in equilibrium. It
must be understood further that the roller _R1_ is loosely fitted to
the spindle _O F_ and hence can whirl with it when pressed against
the segment _G1_ or _G3_; whereas the roller _R2_ is fitted about a
non-revolving extension of the frame _B A C_, and not to the spindle
itself. Bearing in mind that the gyroscope itself is perfectly balanced
and hence tends to maintain its axis _O F_ in a fixed direction, we
shall be able to understand what must happen when the car is tipped
from any cause whatever--as the shifting of its load, the pressure of
the wind, or the centrifugal action due to rounding a curve.
[Illustration: FIG. 2.]
Suppose, for example, that the car tips to the right. This will bring
the segment _G1_ in contact with the roller _R1_, and the roller will
instantly tend to run along it, as a car-wheel runs along the track,
because friction with the spindle causes it to revolve. But this, it
will be evident, is equivalent to pushing the spindle _F_ (or the frame
_A_) toward _B_--"accelerating the precession"--and we know that the
effect of such a push will be to cause the spindle (thanks to that
round-the-corner action) to rise, thus pushing up the segment _G1_, and
with it the car itself.
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