Spinning Tops: The "Operatives' Lecture" of the British Association Meeting at Leeds, 6th September, 1890 — John Shaqi
Spinning Tops: The "Operatives' Lecture" of the British Association Meeting at Leeds, 6th September, 1890Perry, John
Science
Spinning Tops: The "Operatives' Lecture" of the British Association Meeting at Leeds, 6th September, 1890
Perry, John
Gyro compass; Gyroscopes; Tops
As an illustration of this, consider the spinning projectile of Fig. 10.
The spin tends to keep its axis always in the same direction. But there is
a defect in the arrangement, which you are now in a {37} position to
understand. You see that at A the air must be pressing upon the
undersurface A A, and I have to explain that this pressure tends to make
the projectile turn itself broadside on to the air. A boat in a current not
allowed to move as a whole, but tied at its middle, sets itself broadside
on to the current. Observe this disc of cardboard which I drop through the
air edgewise, and note how quickly it sets itself broadside on and falls
more slowly; and some of you may have thrown over into the water at Aden
small pieces of silver for the diving boys, and you are aware that if it
were not for this slow falling of the coins with a wobbling motion
broadside on, it would be nearly impossible for any diving boy to get
possession of them. Now all this is a parenthesis. The {38} pressure of the
air tends to make the projectile turn broadside on, but as the projectile
is spinning it does not tilt up, no more than this gyrostat does when I try
to tilt it up, it really tilts out of the plane of the diagram, out of the
plane of its flight; and only that artillerymen know exactly what it will
do, this kind of _windage_ of the projectile would give them great trouble.
You will notice that an experienced child when it wants to change the
direction of a hoop, just exerts a tilting pressure with its hoop-stick. A
man on a bicycle changes his direction by leaning over so as to be out of
balance. It is well to remind you, however, that the motion of a bicycle
and its rider is not all rotational, so that it is not altogether the
analogue of a top or gyrostat. The explanation of the swerving from a
straight path when the rider tilts his body, ultimately comes to the same
simple principle, Newton's second law of motion, but it is arrived at more
readily. It is for the same reason--put briefly, the exercise of a
centripetal force--that when one is riding he can materially assist his
horse to turn a corner quickly, if he does not mind appearances, by
inclining his body towards the side to which he wants to turn; and the more
slowly the horse is going the greater is the tendency to turn for a given
amount of tilting of one's body. Circus-riders, when galloping in a circle,
assist their horses greatly by the position of their bodies; it is {39} not
to save themselves from falling by centrifugal force that they take a
position on a horse's back which no riding-master would allow his pupil to
imitate; and the respectable riders of this country would not scorn to help
their horses in this way to quick turning movements, if they had to chase
and collect cattle like American cowboys.
Public-domain text, read in full here on John Shaqi.
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