Science for the School and Family, Part I. Natural PhilosophyHooker, Worthington
Science
Science for the School and Family, Part I. Natural Philosophy
Hooker, Worthington
Physics; Science
219. =Projectiles.=--I have already spoken of projectiles in § 211.
You saw there that any body, as a cannon-ball, which is projected
horizontally, falls to the earth in a curved line. Two forces act
on the ball; viz., the projectile force given by the powder and
the force of gravitation. The force of gravity being always the
same, the shape of the curve which the projected body describes
must depend on the force with which it is projected. This is very
strikingly exemplified in the curves described by the different
streams of water in Fig. 141. But whether the projectile force be
great or small, the moving body thrown horizontally will in every
case reach the ground in the same time. Thus if two cannons stand
side by side on a height, one of which will send a ball a mile and
the other half a mile, the two balls, if fired together, will reach
the ground at the same instant, though at first thought it would
seem that the ball which travels twice as far as the other would
take a longer time to do it in. This is because the _horizontal_
force of the ball does not oppose in the least the _downward_ force
of gravity. If it were thrown upward instead of horizontally, the
projectile force would be opposed to gravity, and in proportion
as the direction came near to being vertical. As horizontal force
does not interfere with the action of the force of gravity, it
follows that a ball dropped at the instant at which another is
fired will reach the ground at the same instant that the fired ball
does. This can be made clear by Fig. 155. Suppose it takes three
seconds for a ball to fall from the top of a tower to its foot. In
the first second it falls to _a_. The ball projected horizontally
from the cannon, being operated upon by the same force of gravity,
will fall just as far, and will be on a level with it at _b_. Both
balls fall farther and farther each second, both being accelerated
in the same degree because it is done by the same force. The
projected ball will reach _d_ when the falling ball is at _c_, and
the plain at _f_ when the falling ball is at _e_, the foot of the
tower. The same holds true in all cases. A bullet dropped from a
level with the barrel of a gun, paradoxical as it may seem, will
fall to the ground no sooner than one which is shot from the gun.
[Illustration: Fig. 156.]
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