St. Nicholas, Vol. 13, No. 12, October 1886Various
General
St. Nicholas, Vol. 13, No. 12, October 1886
Various
Children's literature -- Periodicals; Children's periodicals, American
[Illustration: FIG. 3.]
Now, since action is always equal to reaction, the cushion of
air must push back against the ball just as hard as the ball
pushes against it. And since the cushion is thickest where
the combined forces of the ball are greatest, the cushion must
push back hardest in the direction of a line drawn through the
thickest part of the cushion and the center of the ball; _i.
e._, in the line a, b, Fig. 3, a direction against that of the
onward motion of the ball, and to the right of it.
[Illustration: FIG. 4.]
Finally, if at any instant we represent the force of the ball
and its direction by the line A, B (Fig. 4), and the backward
push of the cushion and its direction by the line A, C, then,
according to the law of physics, that, “if two forces act on
a point, and if lines be drawn from that point, representing
the forces in magnitude and direction, and on these lines, as
sides, a parallelogram be constructed, their _resultant_ will
be represented in magnitude and direction by the diagonal which
passes through that point,” the line A, D will represent the
actual force and direction of the ball at the given instant.
But both the forces, A, B and A, C, are constantly decreasing
from the moment the ball leaves the pitcher’s hand, and,
moreover, the force A, B decreases more rapidly than the force
A, C, inasmuch as A, B is acting against the resistance of
the air plus the attraction of gravity, while A, C is acting
against the resistance of the air alone. Consequently, the
direction of A, D is being constantly changed and away from A,
B, and becomes a curve, instead of a straight or broken line.
This curve will obviously have the direction, A, D (Fig. 5), or
to the right, which is the direction in which a ball rotating
to the right will curve.
[Illustration: FIG. 5.]
This reasoning will hold for a ball rotating in any direction,
so long as the axis of rotation is, or tends to be, at right
angles to the line of progression. The problem of the “drift”
of a projectile from a rifle or rifled cannon is entirely
different, and one I should like to see discussed after this
one of “curving” is settled to your readers’ satisfaction.
I think the above explanation solves the problem as well as
explains all the fallacies of your former correspondents.
Very respectfully,
S. P. E.
* * * * *
ANNAPOLIS.
Public-domain text, read in full here on John Shaqi.
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