Golfers are in the way of saying that this ball “flies well” or that the
other ball “does not fly well.” Sometimes it is imagination born of lack
of form; but when great players concur it is not imagination. Some balls
are obviously better than others--made of better material, better
elastic thread, and more carefully constructed. There is an evident
reason why such balls should fly better than others; that is to say,
why they should go off the club more quickly, keep their place in the
air longer, and travel farther. But then there are many balls of
absolutely first-rate quality--and maximum price--that vary considerably
in their flying properties, and it very commonly happens that even balls
out of the same box, made at the same time and in the same way and of
the same stuff, vary also. One frequently finds one or two “bad” balls
in a box, and one or two very good ones. The excellent player very soon
knows when he has come by the good ones and the bad ones. Now why, under
such circumstances, should these balls vary so? What is it that makes
them vary? Golfers in general do not know. Often enough they put it down
to “pure cussedness”; others, to an idea that it is due to some
accidental flaw in the manufacture. It is neither the one nor the other.
The scientific explanation is really a very simple one, and it was set
forth very lucidly by Professor Tait. The perfect ball--using the
adjective in its most absolute sense--is that which has its centre of
gravity, that is to say its centre of weight, dead in the centre of the
ball, the centre of measurement. It is by no means to be assumed that
these two centres must necessarily coincide. For them to do so exactly
is an ideal state, and while matter and man are what they are, and
subject to their constant, even though slight, deviations, it is
unattainable. But when a ball is properly cored and properly covered,
most carefully and by the most exact machinery, the two centres come
very near together, and generally, to all intents and purposes, do
coincide. That they do not always do so exactly is merely because the
greatest human effort is incapable of achieving the scientific ideal,
and it must constantly happen that, despite all that effort, the
distances between the two centres vary a little. Practically no effort
can prevent it, particularly when the exigencies of circumstances demand
that balls should be turned out weekly in tens of thousands, and at a
price of not more than two shillings each. Now and again the separation
of the centres will be greater than normal--accidental again--and then
you get a really bad ball, with much bias upon it. When the centre of
weight is not at centre of measurement, it means that the ball in effect
is heavier on one side than the other, biassed, and that is practically
equal to its being not round. Suppose you inserted a small piece of lead
just inside the cover of a ball and closed it up again, shaping it as
perfectly as it was before. The effect of this would be to remove the
centre of weight very far towards that side, and you would have a great
exaggeration of the difference between the two centres that commonly
exists. If you laid that ball on a table it would promptly roll round
until the weighted or biassed side were underneath. If you floated it in
water it would wobble about until eventually it did the same thing; and
if you floated it in air it would wobble again, and such wobbling would
obviously be detrimental to its straight and even flight. There you have
it. The farther the two centres are from each other--from the ideal
state of absolute coincidence--the greater must be the tendency towards
a wobbly or uneven flight, and diminished rotation, and consequently
towards a short flight. In the case of many balls other than golf
balls, these variations are very considerable. You have an extreme
example when a football is out of shape, and it can be seen to make
zigzags in the air. But the flight of footballs, or even cricket balls,
is not such a delicate and susceptible thing as the flight of a golf
ball at its far greater pace.
Professor Tait pointed out two very simple ways of finding out whether a
golf ball had its two centres approximately coincident, and whether in
consequence it ought to and would fly well. The first was by floating it
in a bath of brine or mercury and noticing whether it wobbled or turned
over. Many golfers are acquainted with this test, and employ it in a
cruder and less decisive form by floating the ball in water. While a
ball that had a fairly considerable separation between its two centres
might not show any wobbling movement when floated in water, and
consequently might not completely establish its claim to be properly
centered and of good flying capacity so far as this part of its
properties was concerned, the presumption would be greatly in its
favour. On the other hand, that which did show any perceptible wobble in
water would be self-condemned at once, and would undoubtedly be a bad
flyer and a danger to the game of the good golfer.
The second test is one of comparison, and is exceedingly simple. You
cannot compare the flying capacities of two or more balls by driving
them with golf clubs, for however near to exact similarity you may think
the strokes to have been, there is certain to have been an appreciable
scientific and mathematical difference, such as would make a proper
comparison impossible. But you may give practically exactly the same
initial impetus in exactly the same circumstances to two or more balls
by shooting them in the same direction from a crossbow, when the string
is always pulled out to exactly the same point. Here you will have the
balls flying under the simplest possible conditions, with no spin to
complicate the flight and interfere with the comparison, and anyone who
takes the trouble to make this experiment will find that some balls will
regularly fly farther than others when shot forward in this manner. If
the size and the weights are the same, these balls are better centered
and better flyers, and it is an easy matter for any player to establish
a standard by this test, and to judge of the perfection of any
particular ball at a moment’s notice. Of course such a test takes no
account of the resiliency of the ball; but then, as every player knows,
there is a clear difference between good resiliency and good flying
properties. In the old days of the gutta, when so much depended upon the
even quality of the material all through the ball--and these were, of
course, the days when Professor Tait made his investigations and
experiments, and drew his conclusions--the variations between centres
were greater than they are now, though not so great as in the early
period of the rubber-core, when the winding and covering machinery were
imperfect. Rubber-cored balls have lately begun to be covered by winding
very thin strips of the covering material round the core in just the
same way that the core itself is wound, and this should greatly conduce
towards more accurate centering. An understanding of the foregoing will
help the player towards an appreciation of some of the chief points of a
good ball, and he will see how extreme is the necessity for perfect
winding machinery and for the most careful supervision of the process.
Nobody calls for a hand-made ball in these days: he wouldn’t get it if
he did; and it wouldn’t be any good if he got it, for the chances would
be enormously against its being so well centered as one made by
machinery.
V
Now, however good the ball might be, the chances would be against a
perfect stillness upon any axis during flight; that is, of course, when
no initial spin was imparted to it by the way in which the stroke was
played. It would very likely turn just a little upon an axis, and that
little would unsteady and injure its flight, inasmuch as the wobble
would be from side to side alternately. This difficulty can be got over
by imparting an initial spin to the ball which will always be the same
all through its flight, and which will thus stop the wobbling. In a
word, rotation will steady the flight. This idea was originally at the
bottom of the rifling of the barrel through which a bullet is projected;
certainly it was the fundamental principle of the rifling of the old
32-pounders. Better to make the ball rotate on an axis that you know
about than that it should wobble on one you do not know about, they
said; and so the tubes were rifled inside, the balls were made to
rotate, and their flight was made steadier and therefore longer.
In the very earliest days of his investigations upon the flight of the
golf ball, Professor Tait thought of the application of this idea to the
game. A rotation should be given to the ball to steady its flight and
make it longer. A moment’s thought on the part of those whose
rudimentary scientific knowledge is a little rusty, will indicate that
there are three definite and clearly distinguished axes of rotation. One
is a vertical one, and it is chiefly upon that axis that the golf ball
rotates when it is pulled or sliced, or upon an axis that has something
of the vertical element in it. Then there is the horizontal axis, which
is at right angles to the line of flight; and this is the axis upon
which it rotates when either under-spin or top has been applied to it.
And, thirdly, there is the horizontal axis, which is parallel with the
line of flight. This is the axis upon which the rifle bullet spins. At
first Professor Tait was inclined to the idea that the last-named would
be the ideal axis for the rotation of the golf ball, but it happens to
be the one upon which it is impossible to make it rotate when struck by
a golf club. However, in this detail of his preliminary theorising he
was wrong, due entirely to his not having then investigated the virtues
of under-spin as always given to a ball when well driven, and not having
come by the great discovery that this under-spin helped the ball to
resist gravity and prolong its flight as nothing else could. How exactly
under-spin does this, we have just seen, and readers will now have a
very definite perception of the qualities of a ball and the importance
of rotation, and though the chief advantage of rotation is in resisting
gravity, it is an incidental advantage of it, as will now be understood,
that the flight of the ball is thereby steadied, and a very slight
inaccuracy in centering made of less consequence than it would otherwise
be. But remember that a considerable inaccuracy in centering will
interfere with the rotation, and therefore the bad flying ball can
still be distinguished, because it will fly badly.