By Philip J. Pritchard, John W. Mitchell
Fox & McDonald’s Introduction to Fluid Mechanics 9th variation has been the most largely followed textbooks within the box. This highly-regarded textual content keeps to supply readers with a balanced and accomplished method of gaining knowledge of serious suggestions, incorporating a confirmed problem-solving technique that is helping readers advance an orderly plan to discovering the best resolution and concerning effects to anticipated actual habit. The 9th version incorporates a wealth of instance difficulties built-in in the course of the textual content in addition to various new finish of bankruptcy problems.
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Extra resources for Fox and McDonald’s Introduction to Fluid Mechanics
Finally, if the Reynolds number is neither large nor small, no general conclusions can be drawn. To illustrate this very powerful idea, consider two simple examples. First, the drag on your ball: Suppose you kick a soccer ball ðdiameter = 8:75 in:Þ so it moves at 60 mph. 10) for this case is about 400,000—by any measure a large number; hence the drag on the soccer ball is almost entirely due to the pressure build-up in front of it.
On the other hand, when a body moves through a fluid, stresses are developed within the fluid. The difference between a fluid and a solid is, as we’ve seen, that stresses in a fluid are mostly generated by motion rather than by deflection. Imagine the surface of a fluid particle in contact with other fluid particles, and consider the contact ! , of the surface at some point C. The force being generated between the particles. Consider a portion, δA ! orientation of δA is given by the unit vector, n^, shown in Fig.
We define a liquid as “wetting” a surface when the contact angle θ < 90 . By this definition, the car’s surface was wetted before waxing, and not wetted after. This is an example of effects due to surface tension. Whenever a liquid is in contact with other liquids or gases, or in this case a gas/solid surface, an interface develops 31 32 Chapter 2 Fundamental Concepts θ < 90° (a) A “wetted” surface Water droplet θ > 90° (b) A nonwetted surface Fig. 11 Surface tension effects on water droplets.