By Bruce R. Munson, Donald F. Young, Theodore H. Okiishi, Wade W. Huebsch
The #1 textual content in its box, basics of Fluid Mechanics is revered through professors and scholars alike for its accomplished topical assurance, its diversified examples and homework difficulties, its program of the visible section of fluid mechanics, and its robust concentrate on studying. The authors have designed their presentation to permit for the sluggish improvement of scholar self assurance in challenge fixing. every one very important thought is brought in basic and easy-to-understand phrases prior to extra advanced examples are mentioned.
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Extra resources for Fundamentals of Fluid Mechanics (6th Edition)
If the container is closed with a small air space left above the surface, and this space evacuated to form a vacuum, a pressure will develop in the space as a result of the vapor that is formed by the escaping molecules. When an equilibrium condition is reached so that the number of molecules leaving the surface is equal to the number entering, the vapor is said to be saturated and the pressure that the vapor exerts on the liquid surface is termed the vapor pressure, pv. Similarly, if the end of a completely liquid-filled container is moved as shown in the figure in the margin without letting any air into the container, the space between the liquid and the end becomes filled with vapor at a pressure equal to the vapor pressure.
Note that doubling the gage pressure does not double the amount of air in the tank, but doubling the absolute pressure does. Thus, a scuba diving tank at a gage pressure of 100 psi does not contain twice the amount of air as when the gage reads 50 psi. 14 Chapter 1 ■ Introduction TA B L E 1 . 7 TA B L E 1 . 6 The gas constant, R, which appears in Eq. 8, depends on the particular gas and is related to the molecular weight of the gas. 8. Also in these tables the gas density and specific weight are given for standard atmospheric pressure and gravity and for the temperature listed.
40 and R ϭ 1716 ft # lbրslug # °R, it follows that c ϭ 1117 ft րs. 42. 19 is also valid for liquids, and values of Ev can be used to determine the speed of sound in liquids. 2 kgրm3 so that c ϭ 1481 mրs or 4860 ftրs. As shown by the figure in the margin, the speed of sound in water is much higher than in air. 8 Vapor Pressure 23 the speed of sound would be infinite. 22. 4. of the speed of sound, c, at the specified altitude. SOLUTION From Eq. 829 c 973 ft/s (Ans) COMMENT This ratio is called the Mach number, Ma.