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Geometry and Materials

MCFCs typically have a planar cell geometry, with areas ranging from bench scale 0.01 m to full scale up to 1 m [10]. The cell form is normally square or rectangular [11], but recently circular cells have also been proposed [12]. The flow pattern is cross-flow in most cases, but according to Kim et al. [13] the counter-flow pattern is associated with lower irreversible losses due to ohmic resistance and anode and cathode activation. Other workers [14] have found by numerical simulation that the co-flow configuration has a higher net output power in some cases. [Pg.70]

Bipolar plate Metal-coated alloy Incoloy 825, 310S, or316 steel 0.2-0.5 [Pg.70]

The electrolyte management, that is, the optimum distribution of molten carbonate electrolyte in the different cell components, is critical for achieving high MCFC performance various processes, and also corrosion reactions, creepage of the matrix, and salt vaporization, can occur and contribute to the redistribution of the molten carbonate in MCFCs. [Pg.71]

Finally, the stainless-steel bipolar plate consists of a separator and current collectors. The plate is exposed to the anodic environment on one side and the cathodic environment on the other. The low oxygen partial pressure on the anodic side of the bipolar plate prevents the formation of a protective oxide coating and, on the cathode side, the contact electrical resistance increases as an oxide scale builds up. Active research is focused on finding alloys for bipolar current-collector materials that function well in both anodic and cathodic environments, have a low cost and ohmic resistance, and have good corrosion resistance [15]. [Pg.71]

rather than with hydrogen or syngas, the MCFC system is fed with hydrocarbons or oxygenated compounds such as glycerol [16] or other alcohols [17-20], the fuel must typically undergo water steam reforming to be converted to mainly H2 prior to being introduced into the FC and electrochemically oxidized. [Pg.71]


Large computers calculated theoretical models of the secondary processes to produce tables of build-up factors. These tables are for neutrons and gammas of various energies in many geometries and material combinations. [Pg.327]

For laminates that are symmetric in both geometry and material properties about the middle surface, the general stiffness equations. Equation (4.24), simplify considerably. That symmetry has the form such that for each pair of equal-thickness laminae (1) both laminae are of the same material properties and principal material direction orientations, i.e., both laminae have the same (Qjjlk and (2) if one lamina is a certain distance above the middle surface, then the other lamina is the same distance below the middle surface. A single layer that straddles the middle surface can be considered a pair of half-thickness laminae that satisfies the symmetry requirement (note that such a lamina is inherently symmetric about the middle surface). ... [Pg.206]

Figure 7.5. Feedback diagram for skeletal mechanical regulation. When forces are applied to a whole bone, the stimulus that results is sensed by the bone cells in the tissue. The sensor cells then signal bone-forming and -removing cells to change the geometry and material properties of the bone. Figure 7.5. Feedback diagram for skeletal mechanical regulation. When forces are applied to a whole bone, the stimulus that results is sensed by the bone cells in the tissue. The sensor cells then signal bone-forming and -removing cells to change the geometry and material properties of the bone.
These effects, specialized for the geometries and materials properties of the collagen-rich stroma and sclera, have been calculated in a paper by Edwards and Prausnitz [197], They also modeled diffusion across the corneal endothelium assuming that the major path was... [Pg.439]

Since L (9, 0) and L2(9, 0) depend only on the geometry and material of the lens, it is convenient to combine them in a single pupil function, which may be defined as... [Pg.106]

A closed-form expression for the characteristic impedance of a lossless stripline illustrates its dependence on the geometry and material properties of the interconnection (51)... [Pg.466]

Usually, microfabrication techniques are used to prepare cantilevers with integrated tips of various shapes, mass and spring constants [197,198]. Depending on the cantilever geometry and material used to construct the cantilever [52], the frequency of commercial cantilevers typically varies from 15 kHz to more than 500 kHz, and the spring constants range from 0.01 to 100 N/m. Micromachining techniques can be used to prepare special probes such as meander-type cantilevers for bidirectional force microscopy [199]. [Pg.95]

A number of configurations of microplasma reactors will be described here. Classification will be based on the power sources, the electric field switching frequency ranging from DC to GHz, and electrode geometries and materials, extending from DBDs to micro hollow cathodes and microcavity discharges. [Pg.42]

An important part of designing a friction measurement apparatus is choosing the probe size, shape, and material. Because friction is an interaction between two surfaces, the probe geometry and material will affect the values calculated for the friction coefficient of the other surface. Also, results will be more accurate when the probe s normal force is maintained at a constant value or continuously monitored previous methods used to maintain the normal force include spring mechanisms or static weights to weigh down the probe. These parameters are revisited critically later in this article. [Pg.432]

Probe geometry and material influence the measured value of the friction coefficient because friction is a probe-skin interaction phenomenon. Few studies have examined probe effects El-Shimi2 studied probe roughness and Comaish and Bottoms3 probe roughness and material. [Pg.433]

Regeneration curves for different diesel particulate trap geometries and materials are shown in Fig. 15.6. [Pg.445]

Related Calculations. Low-fin tubes are tubes with extended surfaces that have the same outside diameter as bare tubes. They can therefore be used interchangeably with bare tubes in tubular exchangers. Various geometries and materials of construction are available from several manufacturers. [Pg.318]

For the study of the process, a set of partial differential model equations for a flat sheet pervaporation membrane with an integrated heat exchanger (see fig.2) has been developed. The temperature dependence of the permeability coefficient is defined like an Arrhenius function [S. Sommer, 2003] and our new developed model of the pervaporation process is based on the model proposed by [Wijmans and Baker, 1993] (see equation 1). With this model the effect of the heat integration can be studied under different operating conditions and module geometry and material using a turbulent flow in the feed. The model has been developed in gPROMS and coupled with the model of the distillation column described by [J.-U Repke, 2006], for the study of the whole hybrid system pervaporation distillation. [Pg.74]

Fig. 4.1.9 Schematic chart of the dependencies relevant to robust design. The only allowed input model parameters are geometry and material parameters, which are correlated with processing effects... Fig. 4.1.9 Schematic chart of the dependencies relevant to robust design. The only allowed input model parameters are geometry and material parameters, which are correlated with processing effects...
The sensor is installed in the air intake manifold of the car, measuring the aspirated air mass. The measuring principle requires the membrane to be exposed to the airflow and thereby also to dust and other particles, which are either not removed by the air filter or are inherent in the intake pipe. The impact of such particles on the membrane imposes a shock-type mechanical load, which can cause field failures as well as O-km failures due to membrane fracture. The task was to identify the relevant geometry and material parameters limiting the lifetime of the sensor element and to deduce a model for their effects on membrane stability [11]. [Pg.219]


See other pages where Geometry and Materials is mentioned: [Pg.208]    [Pg.2324]    [Pg.207]    [Pg.419]    [Pg.903]    [Pg.489]    [Pg.92]    [Pg.49]    [Pg.400]    [Pg.59]    [Pg.352]    [Pg.229]    [Pg.464]    [Pg.185]    [Pg.694]    [Pg.340]    [Pg.340]    [Pg.410]    [Pg.2079]    [Pg.128]    [Pg.3322]    [Pg.205]    [Pg.206]    [Pg.294]    [Pg.280]    [Pg.370]    [Pg.372]    [Pg.130]    [Pg.325]    [Pg.63]    [Pg.68]    [Pg.209]    [Pg.460]    [Pg.448]    [Pg.84]    [Pg.359]   


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