By Faith A. Morrison

ISBN-10: 1107003539

ISBN-13: 9781107003538

This can be a sleek and chic creation to engineering fluid mechanics enriched with a variety of examples, workouts, and functions. it's in response to religion Morrison's imaginative and prescient that flows are either appealing and complicated. A swollen creek tumbles over rocks and during crevasses, swirling and foaming. Taffy might be stretched, reshaped, and twisted in a number of methods. either the water and the taffy are fluids and their motions are ruled through the legislation of nature. The target of this textbook is to introduce the reader to the research of flows utilizing the legislation of physics and the language of arithmetic. this article delves deeply into the mathematical research of flows, simply because wisdom of the styles fluids shape and why they're shaped and the stresses fluids generate and why they're generated is vital to designing and optimizing glossy platforms and units. innovations corresponding to helicopters and lab-on-a-chip reactors may by no means were designed with out the perception introduced by way of mathematical versions.

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Extra resources for An Introduction to Fluid Mechanics

Example text

86 to calculate frictional losses in the pipe. The needed data correlations for p(Q) are discussed next. As discussed previously, to determine F for flows in pipes, we need data on pressure drop as a function of velocity or volumetric flow rate, p(Q). The problem of pressure drop as a function of flow rate in pipe flow has been studied in depth and, with the help of momentum balance, it largely has been solved (discussed in subsequent chapters). To keep moving forward with this quick-start section, we summarize the practical results of the analyses.

24) In an example in the previous section, we related v 1 and v 2 through the mass balance over a converging section of pipe. 25) where D1 is the pipe diameter at Point 1 and D2 is the pipe diameter at Point 2. 26 accurately describes the pressure-drop/flow-rate relationship for many Venturi meters. For slower flows, friction is more important to the total energy, and experiments should be conducted to determine the neglected friction. 27) C V must be determined experimentally by either the user or the manufacturer of the Venturi meter.

The system of water in the flow loop is a single-input, single-output, steady flow of an incompressible fluid. There is no heat transfer and no chemical reaction or phase change; therefore, all requirements of the mechanical energy balance are met. We choose Points 2 and 1 to be where we know the most about the problem. We choose Location 2 to be where the fluid exits the pipe; Location 1 is the liquid free-surface in the tank. 0 in 40 ft A common problem in engineering involves pumping a fluid from a tank at atmospheric pressure through a piping system.

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An Introduction to Fluid Mechanics by Faith A. Morrison


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