How It Flies; or, The Conquest of the Air: The Story of Man's Endeavors to Fly and of the Inventions by Which He Has SucceededFerris, Richard
Science
How It Flies; or, The Conquest of the Air: The Story of Man's Endeavors to Fly and of the Inventions by Which He Has Succeeded
Ferris, Richard
Aeronautics
Taking up again the illustration of the kite flying in a calm, let us
construct a few diagrams to show graphically the forces at work upon
the kite. Let the heavy line AB represent the centre line of the kite
from top to bottom, and C the point where the string is attached, at
which point we may suppose all the forces concentrate their action
upon the plane of the kite. Obviously, as the flyer of the kite is
running in a horizontal direction, the line indicating the pull of
the string is to be drawn horizontal. Let it be expressed by CD. The
action of the air pressure being at right angles to the plane of the
kite, we draw the line CE representing that force. But as this is a
_pressing_ force at the point C, we may express it as a _pulling_ force
on the other side of the kite by the line CF, equal to CE and in the
opposite direction. Another force acting on the kite is its weight--the
attraction of gravity acting directly downward, shown by CG. We have
given, therefore, the three forces, CD, CF, and CG. We now wish to find
the value of the pull on the kite-string, CD, in two other forces, one
of which shall be a lifting force, acting directly upward, and the
other a propelling force, acting in the direction in which we desire
the kite to travel--supposing it to represent an aeroplane for the
moment.
We first construct a parallelogram on CF and CG, and draw the diagonal
CH, which represents the resultant of those two forces. We have then
the two forces CD and CH acting on the point C. To avoid obscuring the
diagram with too many lines, we draw a second figure, showing just
these two forces acting on the point C. Upon these we construct a new
parallelogram, and draw the diagonal CI, expressing their resultant.
Again drawing a new diagram, showing this single force CI acting upon
the point C, we resolve that force into two components--one, CJ,
vertically upward, representing the lift; the other, CK, horizontal,
representing the travelling power. If the lines expressing these forces
in the diagrams had been accurately drawn to scale, the measurement of
the two components last found would give definite results in pounds;
but the weight of a kite is too small to be thus diagrammed, and only
the principle was to be illustrated, to be used later in the discussion
of the aeroplane.
[Illustration]
Public-domain text, read in full here on John Shaqi.
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