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
I will now consider the attraction on the protuberant equatorial belt
indicated by A and B. The sun attracts a pound of matter at B more than it
attracts a pound of matter at A, because B is nearer than A, and hence the
total resultant force is in the direction M N rather than O O, through the
centre of the earth's mass. But we know that a force in the direction M N
is equivalent to a force O O parallel to M N, together with a tilting
couple of forces tending to turn the equator edge on to the sun. You will
get the true result as to the tilting tendency by imagining the earth to be
motionless, and the sun's mass to be distributed as a circular ring of
matter 184 millions of miles in diameter, inclined to the equator at 23½°.
Under the influence of the attraction of this ring the earth would heave
like a great ship on a calm sea, rolling very slowly; in fact, making one
complete swing in about three years. But the earth is spinning, and the
tilting couple or torque acts upon it just like the forces which are always
tending to cause this ship-model to stand upright, and hence it has a
precessional motion whose complete period is 26,000 years. When there is no
spin in the ship, its complete oscillation takes place in three seconds,
and {85} when I spin the gyrostat on board the ship, the complete period of
its precession is two minutes. In both cases the effect of the spin is to
convert what would be an oscillation into a very much slower precession.
There is, however, a great difference between the earth and the gyrostat.
The forces acting on the top are always the same, but the forces acting on
the earth are continually altering. At midwinter and midsummer the tilting
forces are greatest, and at the equinoxes in spring and autumn there are no
such forces. So that the precessional motion changes its rate every quarter
year from a maximum to nothing, or from nothing to a maximum. It is,
however, always in the same direction--the direction opposed to the earth's
spin. When we speak then of the precessional motion of the earth, we
usually think of the mean or average motion, since the motion gets quicker
and slower every quarter year.
Further, the moon is like the sun in its action. It tries to tilt the
equatorial part of the earth into the plane of the moon's orbit. The plane
of the moon's orbit is nearly the same as that of the ecliptic, and hence
the average precession of the earth is of much the same kind as if only one
of the two, the moon or the sun, alone acted. That is, the general
phenomenon of precession of the {86} earth's axis in a conical path in
26,000 years is the effect of the combined tilting actions of the sun and
moon.
Public-domain text, read in full here on John Shaqi.
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