All that is necessary to create lift is to
turn
a flow of air. The airfoil of a
wing turns a flow, but so does a spinning ball. The exact
details are fairly complex and are given on a
separate slide.
Summarizing the results, the amount of force generated by a spinning
ball depends on the amount of spin, the velocity of the ball, the size of the ball,
and the density of the fluid.

The figure shows a view of the flow as if we were moving with the
ball. The ball appears stationary, and the
flow moves from left to right. As the ball spins,
the air near the surface of the ball moves with the surface of the ball.
If there was no free stream flow and the ball was stopped and spinning,
there would be circular flow around the ball which would match the speed
of rotation at the surface and die away to nothing far from the ball.
When the free stream flow is added to this circular flow, the resulting
flow has a net turning and produces a force. On the figure the ball
spins counterclockwise, so the free stream flow over the top of the
ball is opposed by the circular flow; the free stream flow below the
ball is assisted by the circular flow. In the figure we can see that
the streamlines around the ball are
distorted because of the spinning. The net turning of the flow has
produced a downward force.

Let's investigate the flow around a spinning ball by using a Java
simulator.

Due to IT
security concerns, many users are currently experiencing problems running NASA Glenn
educational applets. The applets are slowly being updated, but it is a lengthy process.
If you are familiar with Java Runtime Environments (JRE), you may want to try downloading
the applet and running it on an Integrated Development Environment (IDE) such as Netbeans or Eclipse.
The following are tutorials for running Java applets on either IDE:
Netbeans Eclipse

The left window shows a view of a ball placed in a flow of air.
The ball is a foot in diameter and it is moving 100 miles an hour.
You can spin the ball by using the slider below the view
window or by backspacing over the input box, typing in your new value and
hitting the Enter key on the keyboard. On the right is a graph of the lift
versus spin.
The red dot shows your conditions. Below the graph is the
numerical value of the lift. You can display either the lift value (in
English or Metric units) or the lift coefficient by using the choice
buttons surrounding the output box. Click on the choice button and select
from the drop-menu.

Notice that spinning the ball clockwise generates a positive value for lift, while
spinning the ball counter-clockwise generates a negative value of lift. For a clockwise
spin, with flow from left to right, the ball would rise. For a counter-clockwise spin, the ball
would move downward.

You can download a copy of this program by clicking on this button:

You should save the file "FoilB.zip" to your computer, then "Extract" the files.
Click on "Foil.html" to launch the program. Have fun!

As the force acts on the ball, it is deflected along it's
flight path. If the ball is always spinning, the
force is continuous and the ball is deflected along a circular arc.
The mathematical details of the ball's trajectory are
given on a separate slide.

Be particularly aware of the simplifying assumptions that have
gone into this analysis. The type of flow field shown in the figure
is called an ideal flow field. We have produced the ideal flow field
by superimposing the flow field from an ideal vortex centered on the
ball with a uniform free stream flow.
There is no viscosity
in this model, no
boundary layer
on the ball, even though viscosity is the
real origin of the circulating flow! In reality, the flow around a
spinning ball is
very complex
because of the boundary layer growth and
transition. In addition, the flow off the rear of the ball is normally
separated and can even be unsteady. BUT, the simplified model
helps us to determine the important parameters and the dependence of
the lift force on the value of the parameters. To obtain an accurate
value for the force, engineers typically use a
lift coefficient
that is determined experimentally and accounts for the details
that are too complex to model in the analysis.

You can further investigate the lift of a spinning ball, and a variety of
other shapes by using the
FoilSim III Java Applet.
You can also
download
your own copy of FoilSim to play with
for free.
There is also a Java Applet called CurveBall
to help you explore the aerodynamics of big league pitching.
It computes the path of a thrown curveball.
And there is a new (Aug, 2010) Java applet called
SoccerNASA
that models the aerodynamics of a soccer ball. A kicked soccer ball
curves
in flight because of aerodynamic forces.