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Lactie 4 .1 Shin-sawiralt alion fov Newt. coig cocffoueur Vontiei auculelion h23-2959-989-91 40-s2, Batch -71-99. A> Suiens-Swow neli mclalin Fov auny slius liuwr coondwolio, a sct g aapu canlo such aat
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《流体动力学》(英文版)lecture 1
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Let's first review a bit... from Unified, saw that there are basic considerations in elasticity: 1. Equilibrium 2. Strain-Displacement 3. Stress- Strain Relations (Constitutive Relations)
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We do not characterize materials by their E mnpq The Emnpa are useful in doing transformations, manipulations, etc. We characterize materials by their \ENGINEERING CONSTANTS\ (or, Elastic Constants)
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There are many structural configurations where we do not have to deal with the full 3-D case. First let's consider the models Let's then see under what conditions we can apply them A. Plane Stress
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Thus far we have discussed mechanical loading and the stresses and strains caused by that We noted, however, that the environment can have an effect on the behavior of materials and structures. Let's first consider:
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Have considered the vibrational behavior of a discrete system. How does one use this for a continuous structure? First need the concept of..... Influence Coefficients
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Previously saw (in Unit 19)that a multi degree-of-freedom system has the same basic form of the governing equation as a single degree-of-freedom system The difference is that it is a matrix equation
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Return to the simplest system the single spring-mass This is a one degree-of-freedom system with the governing equation
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When is a flow compressible? compressible flow differs from an incompressible one in that significant change happens in the density
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