Fundamentals of Fluid Mechanics (6th Edition) by Bruce R. Munson, Donald F. Young, Theodore H. Okiishi, Wade PDF

By Bruce R. Munson, Donald F. Young, Theodore H. Okiishi, Wade W. Huebsch

ISBN-10: 0470262842

ISBN-13: 9780470262849

The #1 textual content in its box, basics of Fluid Mechanics is revered via professors and scholars alike for its accomplished topical insurance, its different examples and homework difficulties, its software of the visible section of fluid mechanics, and its robust specialise in studying. The authors have designed their presentation to permit for the slow improvement of scholar self assurance in challenge fixing. each one very important notion is brought in uncomplicated and easy-to-understand phrases sooner than extra complex examples are mentioned.
Note: CD-ROM/DVD and different supplementary fabrics are usually not integrated as a part of booklet dossier.

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Extra info for Fundamentals of Fluid Mechanics (6th Edition)

Sample text

1 is a restricted homogeneous equation, whereas the original equation is a general homogeneous equation that would be valid for any consistent system of units. COMMENT A quick check of the dimensions of the various terms in an equation is a useful practice and will often be helpful in eliminating errors—that is, as noted previously, all physically meaningful equations must be dimensionally homogeneous. We have briefly alluded to units in this example, and this important topic will be considered in more detail in the next section.

0 mm? SOLUTION From Eq. 22 hϭ 2s cos u gR Rϭ 2s cos u gh Note that as the allowable capillary rise is decreased, the diameter of the tube must be significantly increased. There is always some capillarity effect, but it can be minimized by using a large enough diameter tube. 789 kNրm3. 5 COMMENT By repeating the calculations for various values of the capillary rise, h, the results shown in Fig. 8 are obtained. 8 Surface tension effects play a role in many fluid mechanics problems, including the movement of liquids through soil and other porous media, flow of thin films, formation of drops and bubbles, and the breakup of liquid jets.

In accordance with Eq. 9, plots of t versus du րdy should be linear with the slope equal to the viscosity as illustrated in Fig. 6. The actual value of the viscosity depends on the particular fluid, and for a particular fluid the viscosity is also highly dependent on temperature as illustrated in Fig. 6 with the two curves for water. Fluids for which the shearing stress is linearly related to the rate of shearing strain 1also referred to as rate of angular deformation2 are designated as Newtonian fluids after I.

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Fundamentals of Fluid Mechanics (6th Edition) by Bruce R. Munson, Donald F. Young, Theodore H. Okiishi, Wade W. Huebsch

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