Download Mechanics of Fluids (8th Edition) by John Ward-Smith, Bernard Massey PDF
By John Ward-Smith, Bernard Massey
Massey has lengthy been a best-selling textbook. This broadly revised and up to date 8th version, like its predecessors, offers the fundamental ideas of the mechanics of fluids in an intensive and transparent demeanour. It presents the fundamental fabric for an honours measure direction in civil or mechanical engineering, as well as supplying a lot suitable fabric for undergraduate classes in aeronautical and chemical engineering.
Emphasis is given to a valid actual realizing of fluid circulate and its engineering purposes, instead of to mathematical innovations. scholars are brought systematically to the topic, with the textual content relocating from the easy to the advanced, and from the frequent to the strange. SI devices are used all through and there are numerous labored examples. The publication is largely self-contained.
The starting bankruptcy has been extended to supply a broader creation to fluid mechanics. New subject matters for this variation comprise uncomplicated functions of complicated variable concept, the physics of tsunamis, strategies for the choice of pumps and lovers, and the losses for circulation via nozzles, orifice meters, perforated plates and gauzes. For teachers, an accompanying options handbook is on the market.
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Extra resources for Mechanics of Fluids (8th Edition)
Sample text
They can be full-scale or can involve scale models. They can involve the measurement of various quantities, such as velocity or pressure, either at a specified point in a flow or to determine profiles in the form of velocity or pressure distributions. Alternatively, using flow visualization techniques, experiments may be designed to show up the patterns of flow. Various kinds of special facilities are used. The wind tunnel is an important tool in the investigation of the flow of air around aircraft, vehicles and buildings.
Water, however, will not wet wax or a greasy surface. Surface tension The interplay of these various forces explains the capillary rise or depression that occurs when a free liquid surface meets a solid boundary. Unless the attraction between molecules of the liquid exactly equals that between molecules of the liquid and molecules of the solid, the surface near the boundary becomes curved. Now if the surface of a liquid is curved the surface tension forces have a resultant towards the concave side.
As Appendix 2 shows, the dynamic viscosity of air at ordinary temperatures is only about one-sixtieth that of water. Yet because of its much smaller density its kinematic viscosity is 13 times greater than that of water. Measurement of dynamic and kinematic viscosities is discussed in Chapter 6. 5 Non-Newtonian liquids For most fluids the dynamic viscosity is independent of the velocity gradient in straight and parallel flow, so Newton’s hypothesis is fulfilled. 9 indicates that a graph of stress against rate of shear is a straight line through Viscosity Fig.