As an object moves through a gas, the gas molecules are deflected
around the object. If the speed of the object is much less than the
speed of sound
of the gas, the density of the gas remains constant and the flow of
gas can be described by conserving
momentum and
energy. As the
speed of the object increases towards the speed of sound, we
must consider
compressibility effects
on the gas. The density of the gas varies locally as the gas is
compressed by the object.
When an object moves faster than the
speed of sound,
and there is an abrupt decrease in the flow area,
shock waves
are generated.
If the flow area increases, however, a different flow phenomenon is
observed. If the increase is abrupt, we encounter a centered expansion
fan. The word "expansion" denotes that the area is increasing.

There are some marked differences between shock waves and expansion fans.
Across a shock wave, the Mach number decreases, the static pressure increases,
and there is a loss of total pressure because the process is irreversible.
Through an expansion fan, the Mach number increases, the static pressure decreases
and the total pressure remains constant. Expansion fans are
isentropic.

The calculation of the expansion fan involves the use of the
Prandtl-Meyer function.
This function is derived from conservation of
mass,
momentum,
and
energy
for very small (differential) deflections.
The Prandtl-Meyer function is denoted by the Greek letter nu on the
slide and is a function of the
Mach numberM
and the
ratio of specific heatsgam
of the gas. The physical interpretation of the Prandtl-Meyer function is that
it is the angle through which you must expand a sonic (M=1) flow to obtain
a given Mach number.
To compute an expansion from some other Mach number, we denote the upstream
conditions as zone "0" and we calculate the Prandtl-Meyer angle for that
Mach number.

where atan is the
trigonometric inverse
tangent function.
It is also written as shown
on the slide tan^-1. The meaning of atan can be explained
by these two equations:

atan(a) = b

tan(b) = a

We then add the expansion angle a to get the value of the
Prandtl-Meyer function in zone "1".

nu1 = nu0 + a

Then we must iterate (or look up in a table)
to obtain the Mach number in zone "1" which gives that value of the Prandtl-Meyer
function.

Knowing the Mach number in zone "1" and knowing that the flow is
isentropic, we can relate the value of all the flow variables in zone "1" to the
variables in zone "0" through the ratio to the total conditions given on the
isentropic flow
page.

The centered expansion shown on this slide is a special case of the
distributed expansion. Flow expansions can be generated over a long distance
not the sharp edge noted on the slide. Since the flow is isentropic, it is
reversible. Under very careful conditions, we can create isentropic compressions
which take a high Mach number flow down to low Mach numbers, and increase the
static pressure without the loss of total pressure associated with shock waves.
Isentropic compression inlets have been designed for high speed flows, but
typically remain isentropic only over a narrow operating range. If the free
stream Mach number is changed, the isentropic compression waves often coalesce
into a shock wave with the accompanying loss in total pressure.

Here's a Java program which solves the expansion fan problem.

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

To study the expansion fan, you can choose from two types of problems:
the default problem assumes that you know the angle of expansion and wish to
solve for the flow downstream of the expansion; the alternate problem assumes
that you have a specified pressure ratio and you wish to determine the angle
of the expansion and the other flow variables.
Input to the program is made
using the sliders, or input boxes at the lower left. To
change the value of an input variable, simply move the slider. Or
click on the input box, select and replace the old value, and
hit Enter to send the new value to the program.
Output from the program is displayed
in output boxes at the lower right.
The flow variables are presented as ratios
to the free stream value (0).
The graphic at the top shows the expansion surface in red
and the initial and terminal waves generated by the surface as lines.
The user can move the display by clicking on the graphic, holding down,
and dragging the graphic. You can zoom in or out of the graphic by
using the slider at the left. If you loose the graphic, click on "Find"
to restore the initial display.

This simulation was derived from the
ShockModeler
simulation program.
ShockModeler can also be used to study
the intersection and reflection of multiple shock waves.
If you are an experienced user of this simulator, you can use a
sleek version
of the program which loads faster on your computer and does not include these instructions.
You can also download your own copy of the program to run off-line by clicking on this button: