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
If you now clamp the frame, and allow the spinning axis to have no motion
except in a horizontal plane, the motion which the earth tends to give it
about a vertical axis cannot now affect the gyrostat, but the earth
constrains it to move about an axis due north and south, and consequently
the spinning axis tries to put itself parallel {108} to the north and south
direction (Fig. 47). Hence with such an instrument it is easy to find the
true north. If there were absolutely no friction the instrument would
vibrate about the true north position like the compass needle (Fig. 50),
although with an exceedingly slow swing.
[Illustration: FIG. 47.]
It is with a curious mixture of feelings that one first recognizes the fact
that all rotating bodies, fly-wheels of steam-engines and the like, are
always tending to turn themselves towards the pole star; gently and vainly
tugging at their foundations {109} to get round towards the object of their
adoration all the time they are in motion.
[Illustration: FIG. 48.]
Now we have found the meridian as in Fig. 47, we can begin a third
experiment. Prevent motion horizontally, that is, about a vertical axis,
but give the instrument freedom to move vertically in the meridian, like a
transit instrument in an observatory {110} about its horizontal axis. Its
revolution with the earth will tend to make it change its angular position,
and therefore it places itself parallel to the earth's axis; when in this
position the daily rotation no longer causes any change in its direction in
space, so it continues to point to the pole star (Fig. 48). It would be an
interesting experiment to measure with a delicate chemical balance the
force with which the axis raises itself, and in this way _weigh_ the
rotational motion of the earth.[9]
Now let us turn the frame of the instrument G B round a right angle, so
that the spinning axis can only move in a plane at right angles to the
meridian; obviously it is constrained by the vertical component of the
earth's rotation, and points vertically downwards.
[Illustration: FIG. 49.]
[Illustration: FIG. 50.]
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