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Titlebook: Engineering Thermodynamics; Theory, Worked Examp G. Boxer Textbook 1976Latest edition Macmillan Publishers Limited 1976 dynamics.engine.eng

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樓主: HARDY
21#
發(fā)表于 2025-3-25 04:54:47 | 只看該作者
Introduction and Instructions for Use,Entropy (a property of the fluid) follows from the second law in much the same way as internal energy follows from the first.
22#
發(fā)表于 2025-3-25 09:31:18 | 只看該作者
23#
發(fā)表于 2025-3-25 11:48:57 | 只看該作者
24#
發(fā)表于 2025-3-25 19:36:19 | 只看該作者
Design of the Automatic Voltage Regulator,Engineers have a prime concern with the production of mechanical work. Since all processes are irreversible in practice, the capacity to perform work is continually being degraded by virtue of the unwanted heat transfers which occur because of viscous friction and large temperature differences between the working fluid and its environment.
25#
發(fā)表于 2025-3-25 23:56:34 | 只看該作者
Work and Heat Transfer,State the direction of the heat transfer . and work . for each of the following processes. (The systems to be considered are underlined.)
26#
發(fā)表于 2025-3-26 00:33:34 | 只看該作者
First Law of Thermodynamics-Systems,The first law of thermodynamics may be expressed in the symbolic equation. Define the symbols and sign convention which give rise to the equation.
27#
發(fā)表于 2025-3-26 04:17:57 | 只看該作者
Fluid Properties (Excluding Entropy),Throughout this volume all tabulated fluid properties are taken from ‘Thermodynamic and Transport Properties of Fluids’ by Y.R. Mayhew and G.F.C. Rogers published by Basil Blackwell, hereafter referred to as ‘tables’.
28#
發(fā)表于 2025-3-26 11:03:46 | 只看該作者
29#
發(fā)表于 2025-3-26 13:42:36 | 只看該作者
Steady Flow Processes-Vapours,The nozzles of a steam turbine receive steam at 3 bar and 150 °C with negligible velocity. The steam expands adiabatically through the nozzles and leaves at 1 bar with a dryness fraction of 0.96. Calculate
30#
發(fā)表于 2025-3-26 19:11:31 | 只看該作者
Steady Flow Processes-Energy and Momentum,In this chapter a new fundamental concept appears — namely momentum — and in addition to the principles of conservation of mass and energy previously encountered we have to use the third principle — conservation of momentum which is embodied in Newton’s laws of motion.
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