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Remember from your undergraduate fluids that if we have a relationship
of the form

then the nondimensional ratio
will be a function of
the nondimensional combinations (or
-groups) that we can make
from the four function arguments. Now
is already a
nondimensional number. From the other three, we can only get rid of
the mass dimension by taking the ratio
, which we already
know is proportional to the speed of sound a1. We can then get rid
of the velocity dimension by taking a ratio with the speed u1. So
our only other nondimensional combination is the Mach number M1=u1/a1,
and dimensional analysis then tells us that

Of course, the same holds for any other nondimensional ratio we solve
for. So the form of our solution will be:

For the important case of normal air, i.e.
, the book
provides all these functions in tabular form in Table A.2.
The first column in the table is the Mach number M1, the second column the
corresponding p2/p1, the third
, etcetera.
For other values of
than 1.4, you will have to use the
actual formulae, which we will derive now.
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