When a baseball is
thrown
or
hit,
the resulting motion of the ball is determined by
Newton's laws of motion
and the relative strength of the forces acting on the ball.
A force may be thought of as a push or
pull in a specific direction.
A force is a
vector quantity
so a force has both a magnitude and a direction. When
describing forces,
we have to specify both the magnitude and the direction.
This slide shows the forces that act on
a baseball in flight.
Weight
Weight is a force that is always directed
toward the center of the earth. In general, the
magnitude
of the weight depends on the mass of an object as first determined
by Newton's law of gravitation.
By rule, the weight of a major league baseball is 5 ounces.
The weight is
distributed throughout the ball. But we can often think of it as
collected and acting through a single point called the
center of gravity.
In flight, the ball
rotates
about the
center of gravity.
A baseball is made with a solid core, a string wrapping around the core,
and a stitched covering. To first order, the center of gravity for a baseball is
located at the exact center of the ball.
Strictly speaking, the ounce (oz.) is a measure of mass and not of weight.
Weight is a force, mass times acceleration, and is not equal to the mass of an
object. Unfortunately, humans often use the units for weight and mass interchangeably;
the assumption being that we talking about the weight at the surface of the Earth
where the acceleration is a constant (32.2 ft/sec^2 or 9.8 m/sec^2).
So when the rule states that the ball weighs 5 oz,
it should more correctly specify that the weight is 5/16 lb.
The pound is a measure of force.
On Mars, the mass of a baseball is the same as on Earth. But since the
gravitational acceleration on Mars is 1/3 that of the Earth,
the weight of a baseball on Mars is 5/48 lb.
As the baseball moves through the air, there is a large aerodynamic
force acting on the ball. Aerodynamicists normally resolve the single aerodynamic
force into two components; drag acts in a direction opposite to the
motion, and lift acts perpendicular to the motion and to the drag.
Let's consider each of these forces separately.
Drag
As the ball moves through the air,
the air resists the motion of the ball and the
resistance force is called drag.
Drag is directed along and opposed to the flight direction.
In general, there are many
factors
that affect the magnitude
of the drag force including the
shape
and
size
of the object,
the square of the
velocity of the object,
and conditions of the air; particularly, the
density and
viscosity of the air.
Determining the magnitude of the drag force is difficult
because it depends on the details of how the flow interacts with the surface
of the object. For a baseball, this is particularly difficult
because the stitches used to hold the ball together are not
uniformly or symmetrically distributed around the ball.
Depending on the orientation of the ball in flight, the drag
changes as the flow is disturbed by the stitches.
To determine the magnitude of the drag, aerodynamicists use
wind tunnel
tests to measure the drag.
The aerodynamic force acts through the
center of pressure
of any object. For an ideal, smooth ball, symmetry considerations
place the the center of pressure at the
center of the ball along with the center of gravity.
But a baseball in flight is neither smooth nor symmetric because of the stitches.
So the center of pressure for a baseball moves slightly about the center of the
ball with time, depending on the orientation of the stitches.
This motion is the source of the "dancing" knuckleball that confuses both
batters and catchers alike.
Lift
Lift is the component of the
aerodynamic force that is perpendicular to the flight direction.
Airplane wings generate
lift
to overcome the weight of the airplane and allow the airplane to fly. A
rotating cylinder
and a
spinning ball
also generate aerodynamic lift.
For a spinning ball the lift force
is generated perpendicular to the axis of rotation.
The magnitude of the lift depends on several
factors
related to the conditions of the air and the object,
and the velocity between the object and the air.
For a spinning ball, the
speed of rotation
also affects the magnitude of the lift.
And the stitches on a baseball introduce some additional complexity in the
generation of lift, just as the stitches introduced complexity in the
generation of drag. To account for the complexities when making predictions
of the lift on a baseball, or of the lift of an airplane wing, aerodynamicists
make an
ideal prediction
using theory, and then
correct
the prediction using experimental data.
The motion of the ball through the air depends on the relative
strength and direction of the forces shown above.
We have built two major simulation packages that look at the
physical problem of pitching a
curve ball,
and of the flight of a baseball that is
hit
from home plate.
The curve ball problem involves all three forces with the lift force
producing the
side force
that causes the ball to curve. The simulation calculates the magnitude of
the lift force and it can be shown that even big league pitchers can not generate
enough lift force to overcome the weight of the ball. There are no rising fast balls.
The hit baseball problem considers only the forces of drag and weight. the
simulator demonstrates the important role that atmospheric conditions
play on the flight of a baseball. The
flight trajectory
is very different from the idealized
ballistic flight
that occurs when drag is neglected.
The figure on this web page was created by Elizabeth Morton, of Magnificat
High School, during a "shadowing" experience at NASA Glenn during May of 2007.
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