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Material properties defined

The emissive power of a body E is defined as the energy emitted by the body per unit area and per unit time. One may perform a thought experiment to establish a relation between the emissive power of a body and the material properties defined above. Assume that a perfectly black enclosure is available, i.e., one which absorbs all the incident radiation falling upon it, as shown schematically in Fig. 8-4. This enclosure will also emit radiation according to the T law. Let the radiant flux arriving at some area in the enclosure be q, W/m2. Now suppose that a body is placed inside the enclosure and allowed to come into temperature equilibrium with it. At equilibrium the energy absorbed by the body must be equal to the energy emitted otherwise there would... [Pg.376]

The viscoelastic nature of polymers generally determines rate and temperature dependence of their mechanical properties. At low strain levels, i.e. in a linear regime, this dependence is well described by intrinsic material properties defined within constitutive viscoelastic laws [1]. At high strains, in presence of failure processes, such as yielding or fracture, it is more difficult to establish a constitutive behaviour as well as to define material properties able to intrinsically characterise the failure process and its possible viscoelastic features. [Pg.90]

Once the mesh has been created, the scope of the problem to be solved has to be specified. This step includes specifying the material properties, defining the physical models, setting the boundary conditions, and specifying the initial conditions. [Pg.508]

The exchange current density f is a static materials property defined in the section Catalyst Activity. The reaction penetration depth 8cl is a steady-state property determined by the interplay of transport properties of the layer and local electro-catalytic activity, embodied in f. Together, both parameters f and Scl determine the overall effectiveness of catalyst utilization. For illustration purposes, a simple scenario of this interplay for the case of severely limited oxygen diffusion will be considered below. [Pg.175]

Conductivity, thermal (symbol, k) - a material property defining the relative capability to carry heat by conduction in a static temperature gradient. Conductivity varies slightly with temperature in solids and liquids and with temperature and pressure in gases. It is high for metals (copper has a k of380 W/m-°C) and low for porous materials (concrete has a k of 1.0) and gases. [Pg.157]

In order to describe the second-order nonlinear response from the interface of two centrosynnnetric media, the material system may be divided into tlnee regions the interface and the two bulk media. The interface is defined to be the transitional zone where the material properties—such as the electronic structure or molecular orientation of adsorbates—or the electromagnetic fields differ appreciably from the two bulk media. For most systems, this region occurs over a length scale of only a few Angstroms. With respect to the optical radiation, we can thus treat the nonlinearity of the interface as localized to a sheet of polarization. Fonnally, we can describe this sheet by a nonlinear dipole moment per unit area, -P ", which is related to a second-order bulk polarization by hy P - lx, y,r) = y. Flere z is the surface nonnal direction, and the... [Pg.1275]

The performance characteristics of ceramic sensors are defined by one or more of the foUowing material properties bulk, grain boundary, interface, or surface. Sensor response arises from the nonelectrical input because the environmental variable effects charge generation and transport in the sensor material. [Pg.345]

Designers have always had to deal with the fact that parts cannot be made perfectly or if they could, they would not remain perfect for long during use. So defining the ideal component is only one aspect of the designer s job (Hopp, 1993). The designer must also decide by how much a still acceptable component can be from the ideal. A component can vary from the ideal in many ways in its geometry, its material properties, surface finish - a virtually unlimited list (Alexander, 1964). [Pg.38]

Design allowable Statistically defined material property allowable strengths, usually referring to stress and/or strain. [Pg.634]

In our case, we define a formula as consisting of raw materials and/or other formulas. We develop a modelling procedure we call to determine formula characteristics from raw material properties, and give it the recursive property of being able to call itself when it encounters a formula used as a raw material. The procedures terminate when all formulas are resolved into basic raw materials. This terminating condition cannot be met if any formula contains a reference to itself, either directly or indirectly, through another formula. [Pg.55]

Figure 1.4. Catalysts are nanomaterials and catalysis is nanotechnology. If we define nanotechnology as the branch of materials science aiming to control material properties on the nanometer scale, then catalysis represents a field where nanomaterials have been applied commercially for about a century. Many synthetic techniques are available to... Figure 1.4. Catalysts are nanomaterials and catalysis is nanotechnology. If we define nanotechnology as the branch of materials science aiming to control material properties on the nanometer scale, then catalysis represents a field where nanomaterials have been applied commercially for about a century. Many synthetic techniques are available to...

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Material defined

Properties defined

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