# Summary

Refer again to the road map for Chapter 1 given in Figure 1.6. Read again each block in this diagram as a reminder of the material we have covered. If you feel uncomfortable about some of the concepts, or if your memory is slightly “foggy” on certain points, go back and reread the pertinent sections until you have mastered the material.

 This chapter has been primarily qualitative, emphasizing definitions and basic concepts. However, some of the more important quantitative relations are summarized below:

 The center of pressure is obtained from

 Mle ~T~

 Mle N

 r’cp

 [1.80] and [1.91]

 The criteria for two or more flows to be dynamically similar are: 1. The bodies and any other solid boundaries must be geometrically similar. 2. The similarity parameters must be the same. Two important similarity parameters are Mach number M = V/a and Reynolds number Re = p V с/ц.. If two or more flows are dynamically similar, then the force coefficients Cl, Cd, etc., are the same.

 In fluid statics, the governing equation is the hydrostatic equation: dp = ~gp dy [1.52] For a constant density medium, this integrates to p + pgh = constant [1.54] or p і + pgh = P2 + pgh2 Such equations govern, among other things, the operation of a manometer, and also lead to Archimedes’ principle that the buoyancy force on a body immersed in a fluid is equal to the weight of the fluid displaced by the body.