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In this chapter we turn to chemical products whose value is strongly connected to their microstructure. By “microstructure,” we mean chemical organization on the scale of micrometers. Some microstructured products are listed in Table 9.0–1. To understand how large such structures are, we remember that hair and beards grow about one millimeter in three days, or 300 μm per day. Thus, beard growth in eight hours – a “five o'clock shadow” – is about 100 μm. We can just feel this size. On the other hand, blood cells are discs 8 μm across and 3 μm thick, and we cannot feel individual blood cells. In many cases, the microstructures which we make will be between these sizes. Because they will be smaller than 100 μm, they will feel like continua, but because they are often the size of blood cells, they are not in reality homogeneous.
Another way to judge these products is their size on a logarithmic scale, shown earlier in Figure 1.5–1. On such a scale, the relative size of microstructures lies midway between the sizes of us and of individual molecules. Our little fingers are about 1 cm, or 10,000 μm, across. A microstructure of 1 μm, or 10,000 Å, is much larger than a molecule 3 Å in diameter. Microstructures are around the wavelength of visible light.
Products with microstructure supply added value because of the physical and chemical properties of the microstructure.
We consider the following question: given a set of matrices with no rank-one connections, does it support a nontrivial Young measure limit of gradients? Our main results are these: (a) a Young measure can be supported on four incompatible matrices; (b) in two space dimensions, a Young measure cannot be supported on finitely many incompatible elastic wells; (c) in three or more space dimensions, a Young measure can be supported on three incompatible elastic wells; and (d) if supports a nontrivial Young measure with mean value 0, then the linear span of must contain a matrix of rank one.
The distribution of copolymerized units in the polymer chain
General principles
If a mixture is made of two or more types of monomer which polymerize by similar mechanisms, e.g. the free radical process, they may be polymerized to form chains in which the structural units of the respective homopolymers are present to varying extents and in sequences whose lengths depend on the polymerization conditions. Such copolymers are important commercially and they are also the source of a considerable amount of information on polymerization processes. Their commercial importance is that they provide the means for modifying to advantage the physical properties of the parent homopolymers. They may provide a higher tensile strength, a greater impact strength, a superior stress crack resistance, an improved resistance to thermal and photochemical degradation or a modified crystallization behaviour. At the fundamental level, the molecular structure of the copolymer can often provide information on the polymerization mechanism, such as the factors which determine the reactivity of a particular radical. It is also possible to prepare polymers with known structural defects in order to study their effects. For example, the copolymerization of small amounts of ally1 chloride, CH2=CH—CH2CI, or acetylene, CH≡CH, with viny1 ch1oride may be used to introduce ch1oromethy1 branches, —CH2C1, or double bonds, respectively, into the viny1 chain in order to assess whether these types of defect are the sites of the initiation process for thermal degradation.
This paper deals with the mathematical characterization of microstructure in elastic solids. We formulate our ideas in terms of rank-one convexity and identify the set of probability measures for which Jensen's inequality for this type of functions holds. This is the set of laminates. We also introduce generalized convex hulls of sets of matrices and investigate their structure.
I argue that experiences can have microphenomenal structures, where the macrophenomenal properties we introspect are realized by non-introspectible microphenomenal properties. After explaining what it means to ascribe a microstructure to experience, I defend the thesis against its principal philosophical challenge, discuss how the thesis interacts with other philosophical issues about experience, and consider our prospects for investigating the microphenomenal realm.
This book presents a theory of the firm based on its economic role as an intermediary between customers and suppliers. Professor Spulber demonstrates how the intermediation theory of the firm explains firm formation by showing how they arise in a market equilibrium. In addition, the theory helps explain how markets work by showing how firms select market-clearing prices. Models of intermediation and market microstructure from microeconomics and finance shed considerable light on the formation and market-making activities of firms. The intermediation theory of the firm is compared to existing economic theories of the firm including the neoclassical, industrial organization, transaction cost, and principal-agent models.
Pulsar radio intensities contain a rich range of timescale variations ranging from months down to nanoseconds. The shortest of these fluctuations have been called microstructure. The observational properties of microstructure and the astrophysical value of microstructure are discussed.
Ductile sheared rocks of the Higher Himalayan Crystalline unit (HHC) in micro-scale reveal flanking microstructures defined by nucleated minerals (the cross-cutting elements, CEs), and deflected cleavages and grain margins (the host fabric elements, HEs) of other minerals. Depending on different or the same senses of drag across the cross-cutting elements, the flanking microstructures are grouped into Type 1 or Type 2 varieties, respectively. Cross-cutting elements of Type 2 flanking microstructures connote post-tectonic directional growth. The cross-cutting elements of the Type 1 flanking microstructures consistently demonstrate top-to-SW non-coaxial shearing in the Higher Himalayan Crystalline unit. Here the external host fabric elements bounding the cross-cutting elements act as the C-planes. These cross-cutting element minerals are usually parallelogram-shaped, underwent crystal-plastic deformation and their nucleations are pre- or syntectonic. The facts that the host fabric elements are dragged even in absence of rheological softening at the boundaries of the cross-cutting elements, and that the cross-cutting elements are non-rigid, indicate strong bonds between the host fabric elements and the cross-cutting elements. Salient morphological variations in the flanking microstructures are: (1) variable intensity and senses of drag along the single and the opposite cross-cutting element margins; (2) host fabric elements defined only at one side of the cross-cutting elements; and (3) presence of a thin hazy zone at the HE–CE contacts. The observed cross-cutting element minerals are either of nearly the same or of greater competency than the mineral grains which host them.
We have thus far dealt with the resistance to crack propagation at opposite extremes of material representation, continuum solid and atomic lattice. It is now appropriate to investigate the problem at an intermediate level, that of the microstructure. By ‘microstructure’ we mean the compositional configuration of discrete structural ‘defects’: voids, inclusions, secondphase particles (volume defects); secondary crack surfaces, grain boundaries, stacking faults, twin or phase boundaries (surface defects); dislocations (line defects). It is principally at this intermediate level that significant improvements in the mechanical properties of traditional brittle polycrystalline ceramics (cf. table 3.1) may be realised. By tailoring the microstructure it is possible to introduce an interactive defect structure that acts as an effective restraint on crack propagation and thus enhances the material toughness.
In this chapter we examine some of these ‘toughening’ interactions. We identify two classes of restraint. The first involves purely geometrical processes, deflections along or across weak interfaces, etc. The responsible microstructural elements may be regarded as ‘transitory obstacles’, in the sense that their impeding influence lasts only for the duration of crackfront intersection. Because of their ephemeral nature such interactions are relatively ineffective as sources of toughening, accounting at very most for increases of a factor of four in crack-resistance energy R or, equivalently, a factor of two in toughness T.
The second class of restraint comprises shielding processes. The critical interactions occur away from the tip, within a ‘frontal zone’ ahead or at a ‘bridged interface’ behind.
The Synroc concept was introduced by Ringwood in 19781 and, as is well known, the material now proposed for the disposal of hiah-level civilian nuclear waste consists primarily of hollandite (BaAl2 Ti6016), perovskite (CaTiO3) and zirconolite (CaZrTi207).
Musical coherence is essential for the achievement of meaning in any particular work. While it is possible to speculate on a variety of reasons which may facilitate this coherence, many would agree that an important determinant may be found in the successful articulation of the work’s structure. Furthermore, structure is realised through discourse, which is dependent on the articulation of actual sounds: inflections, accents, local changes in tempo, etc., may alter the meaning of a passage significantly. Although this is true of any music, it acquires additional significance for the composer in the electroacoustic domain since she becomes responsible for the inner attributes of timbre.
Some typical microstructural studies of polycrystalline silicon using transmission electron microscopy (TEM) are described, including the application of this material for assisting TEM investigations themselves. Examples include oxidation and realignment of polysilicon thin films, the structure of polysilicon in EEPROM devices, polysilicon in trench capacitors and measurement of SiO2 layer thicknesses with polysilicon overlayers. It is also shown tha grain growth in heavily phosphorus doped polysilicon films can be followed by in situ heating in the TEM.
The study of microstructure–property relationships and processing history leading to those relationships is at the core of materials engineering. The historical evolution of the understanding of processing–microstructure–property relationships has largely relied on empirical evidence that, in turn, has helped catalyze theories iteratively linking modeling to experiments, which has then helped the maturation process of materials design. While the power of modeling methods has increased, we have, as of yet, no unified mathematical formalism to seamlessly connect materials chemistry with kinetics and micro- and mesoscale information despite decades of work. In this article, we provide an overview of how “microstructural informatics” permits one to capture the interaction between processing variables and their influence on microstructure–chemistry–property correlations. This includes a particular focus on the use of manifold representations and data compression methods for defining microstructure–chemistry–property relationships that can explain known materials behavior and aid in designing new processing pathways of materials with enhanced properties. The concept of identifying an irreducible representation of microstructure is introduced.
The previous chapter outlined an approach to asset price determination that focuses on stocks. In summary: the realized market price is such that the existing stock of each asset is willingly held by investors in the aggregate – the demand to hold the stock is equal to its supply. A second approach to price determination focuses on flows: the asset price is such that the flow of purchases over a short interval of time equals the flow of sales. That is, the total demand from all those investors who seek to add to their holdings of the asset equals the total supply of all those investors who seek to reduce their holdings. The two paradigms are not necessarily incompatible. Neither is necessarily right or wrong. They are just different ways of analysing the same thing – namely, what determines asset prices.
This chapter, unlike most that follow, adopts the second paradigm. Viewing prices as determined by flows of assets is particularly useful in exploring the details of how prices are set in practice and the behaviour of those who set them. Following a brief review of some basic features of market activity in section 2.1, section 2.2 studies the commonest trading mechanisms found in asset markets. Section 2.3 considers asset markets from the perspective of industrial organization and reviews the nature of competition within and between the markets.
Initially, suitable matrix alloy compositions and heat treatments were proposed solely on the basis of experience gained with unreinforced alloys. However, as this chapter demonstrates, the incorporation of a reinforcing phase can have a pronounced effect on the development of matrix microstructure. Because of their sensitivity to matrix microstructure, this is an especially important consideration for discontinuously reinforced systems.
Dislocation structure and behaviour
Plastic deformation in the matrix of a composite is never completely homogeneous. The reinforcement interrupts flow, giving rise to distinctive dislocation structures. As well as having immediate implications for the flow properties of the matrix, these structures also indirectly influence flow behaviour via changes in the precipitation and aging response.
The influence of thermal stress on dislocation structure
In many MMCs, thermal stresses can give rise to dislocation densities which are 10–100 times greater than those for comparable unreinforced alloys. The conditions under which the creation of thermally stimulated dislocations is energetically favourable were first studied by Ashby and Johnson, who found that, for incoherent particles, the critical misfit decreases with increasing particle size. For short fibres and particles, the simplest mechanism of stress relief is to punch out a dislocation loop (a disc of vacancies or interstitials) into the matrix (Fig. 10.1(a,b)). This mechanism, illustrated schematically in Fig. 4.16, is well understood in terms of a relaxation in the local stress field.
Firms create and manage markets by acting as intermediaries between buyers and sellers. An intermediary is an economic agent who purchases from suppliers for resale to buyers or who helps buyers and sellers meet and transact. Intermediaries seek out suppliers, find and encourage buyers, select buy and sell prices, define the terms of transactions, manage the payments and record keeping for transactions, and hold inventories to provide liquidity or availability of goods and services.
This book is concerned with the economic role of firms and the functioning of markets in general. In finance, the study of intermediation and the institutions of exchange is called market microstructure. I apply the term market microstructure generically to refer to the operation of markets for all types of goods and services. I show that there are basic similarities between a broad range of intermediation models in economics and finance. Throughout the book, the main results are derived within a common framework, with similar notation and related economic reasoning.
Just as producing goods and services consumes resources, so does the establishment and operation of markets to allocate those goods and services. Companies incur costs in adjusting prices and communicating price information to buyers and sellers. The types of information imperfections that are present determine the intermediation activities of firms. When there is demand and supply randomness, intermediaries provide liquidity or immediacy by standing ready to buy and sell. Given uncertainty about the willingness to pay or opportunity costs of trading partners, intermediaries coordinate transactions by matchmaking and brokering activities.
Microstructure is a feature of crystals with multiple symmetry-related energy-minimizing states. Continuum models have been developed explaining microstructure as the mixture of these symmetry-related states on a fine scale to minimize energy. This article is a review of numerical methods and the numerical analysis for the computation of crystalline microstructure.
Recently, the late R. Shiromizu carried out studies to establish the limits of metastability in the Cu-Be system. Con-currently, we engaged in parallel research, but with a broader emphasis on the microstructures concomitant with quenching, aging and reversion. A complete report covering 0.16 to 2.1 wt.% Be will be published elsewhere; certain unique structures are presented below.
Alloys of >0.8 wt.% Be quenched from the α (f.c.c.) region exhibit weak {110} tweed strain contrast. Direct lattice imaging did not detect discrete particles in this condition, whereas rather high densities of {100} G.P. Zone plates in regular stairstep array were revealed after aging at temperatures well below the G.P.Z. solvus.