Now we look at  this 
animation as a periodic sound wave.  The red bar on the left acts  as 
the driving piston.  If it moves in a sinusoidal manner from left  to 
right,  then the wave that is produced will be a sinusoidal wave.   Since 
the wave is sinusoidal, the wavelength, amplitude and frequency  are constant. 
This is seen in nature as a tuning fork, which produces a periodic sound
wave.  In a one dimensional tube as shown  above, each particle undergoes
simple harmonic motion.  The volume that  is contained in one wavelength
also undergoes this same motion.  We can represent the displacement
of this volume as: 
                      
    s(x,t) = smax cos(kx - wt), 
     
       
       where smax is the maximum displacement or displacement 
amplitude,  k is the angular wave number, and w is the angular frequency of
the piston.   
       We can also represent the change in pressure at any 
point  in the same manner as we did for the volume displacement.  That 
is shown  by:  
                 
    dP(x,t) = dPmax sin(kx -
wt),      
       
       where dPmax is the maximum change in pressure, k is 
angular wave  number, and w is angular frequency.
       
   By combining the two equations we can receive the result:
                 
    dPmax = pvwsmax 
     
                 
    where the maximum change in pressure (dPmax), 
 is equal to the density (p), times the velocity of the wave (v), times the 
 angular frequency of the piston (w), times the maximum volume displacement 
 (smax).