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Titlebook: An Introduction to the Properties of Engineering Materials; K. J. Pascoe Book 1978 K. J. Pascoe 1978 X-ray.ceramics.crystal.deformation.fa

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發(fā)表于 2025-3-21 16:06:17 | 只看該作者 |倒序?yàn)g覽 |閱讀模式
期刊全稱(chēng)An Introduction to the Properties of Engineering Materials
影響因子2023K. J. Pascoe
視頻videohttp://file.papertrans.cn/156/155588/155588.mp4
圖書(shū)封面Titlebook: An Introduction to the Properties of Engineering Materials;  K. J. Pascoe Book 1978 K. J. Pascoe 1978 X-ray.ceramics.crystal.deformation.fa
影響因子The engineering designer is always limited by the properties of available materials. Some properties are critically affected by variations in com- position, in state or in testing conditions, while others are much less so. The engineer must know this if he is to make intelligent use of the data on properties of materials that he finds in handbooks and tables, and if he is to exploit successfully new materials as they become available. He can only be aware of these limitations if he understands how pro- perties depend on structure at the atomic, molecular, microscopic and macroscopic levels. Inculcating this awareness is one of the chief aims of the book, which is based on a successful course designed to give university engineering students the necessary basic knowledge of these various levels. The material is equivalent to a course of about eighty to a hundred lectures. In the first part of the book the topics covered are mainly fundamental physics. The structure of the atom, considered in non-wave-mechanical terms, leads to the nature of interatomic forces and aggregations of atoms in the three forms-gases, liquids and solids. Sufficient crystallography is discussed to facilitate
Pindex Book 1978
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The Strengthening of Metals,a. It is possible to grow dislocation-free crystals—known as .—which have strengths which approach the theoretical value. However, these are very small, very expensive to produce, and no plant has yet been made for large scale production.
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Wie eine Arztpraxis werben kann,A description of the internal structure of each of the alloys possible between two or more metals, giving the compositions and temperatures over which the various phases exist, is most conveniently presented as an equilibrium or constitution diagram.
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Wie Sie patientenorientiert kommunizierenOn cooling molten pure iron, it solidifies at 1539 °C into a body-centred cubic structure. On further cooling, this structure changes at 1400 °C to a face-centred cubic structure and again at 910 °C back to body-centred cubic. These structures have been designated ., ., and . from room temperature upwards.
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https://doi.org/10.1007/978-3-642-00734-7The kinetic energy of translation of the molecules of an ideal gas was discussed in Chapter 3 and shown to be equal to . Also it was shown that . for one mole, so that the kinetic energy was . per mole or . per molecule on the average.
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https://doi.org/10.1007/978-3-642-00734-7An examination of the behaviour of single crystals during deformation is necessary to an understanding of the deformation of polycrystalline aggregates. Single crystals of metals in suitable form for carrying out mechanical tests may be prepared by several methods, some of which are outlined in Section 5.9.
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