By Reiner Decher
Direct power Conversion is written for college kids and working towards engineers with an curiosity within the functionality of strength conversion tactics that contain direct equipment of manufacturing electrical strength from warmth and different basic assets. It offers an in-depth improvement of key concerns from the 1st rules of the underlying sciences, and examines the potential on hand for changing warmth to electrical energy with no the intermediate new release of rotating shaft energy. A actual and quantitative knowing of the constraints of a few commercially fascinating tools is built so one can permit readers review of the applied sciences for particular functions. The checklist of tactics thought of is restricted by way of functionality measured when it comes to expense, conversion potency, and gear density. perfect for senior undergraduate and graduate point classes in strength creation, strength conversion, and tool platforms, Direct strength Conversion can also be a traditional adjunct to the author's prior textual content, Energy Conversion (OUP, 1994), which specializes in the thermodynamics and mechanics of warmth.
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Additional resources for Direct Energy Conversion: Fundamentals of Electric Power Production
Show that the B field distribution is linearly increasing in the column and then decreases as 1/r outside the column. By considering the j x B body force, find the pressure distribution in this static column. 3. Show that the momentum thickness is the proper length scale to measure a viscous force interaction in a developing boundary layer flow in a pipe of diameter D. What is the corresponding scale in a fully developed flow? BIBLIOGRAPHY Sutton, G. , Engineering Magnetohydrodynamics, McGraw-Hill, New York, 1965.
16 DIRECT ENERGY CONVERSION 40 11th 20 0 0 20 40 60 80 100 % Maximum oower 1-10. Part power characteristics of a number of engine types. These variations are qualitative and depend strongly on the specifics of the cycle. FIGURE acteristic size parameter. The (angle-averaged) pressure on the piston and the size of the machinery determines the force on the piston and thus the torque on the shaft. The speeds involved are limited by the linear piston speed, which, in tum, determines the angular speed for a machine of a given size.
The derivative following a fluid element (total derivative) is given by v Dt a = -+U·V dt (2-52) so that the continuity equation (eq. 2-51) can be written as Dp + pV·U=O Dt (2-53) This form is particularly useful to interpret because it shows that div U = 0 when the fluid is incompressible. 3. Momentum Equation For the accounting of forces, the term due to viscous effects is neglected. J(pU)dV v s v (2-54) FLOW WITH ELECTROMAGNETIC INTERACTION 41 Surface outward normal FIGURE 2-11. Flux of a quantity through a surfaceS.