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Geometry finite element

Calculations for the stub blades or welded attachment points of impeller blades can be done like calculations for the extension blade thickness. The details of welding, casting, or other methods of attachment become critical in the design. Conventional calculations for structural strength may be adequate, but for com-phcated geometry, finite element models can provide better design information. [Pg.1310]

TRIFOU is a combined Finite Elements/Boundary Integral formulation code. The BIM formulation in vacuum is suitable for NDT simulation where the probe moves in the air around the test block. The FEM formulation needs more calculation time, but tetrahedral elements enable a large variety of specimens and defect geometries to be modelled. TRIFOU uses a formulation of Maxwell Equations using magnetic field vector h, where h is decomposed as h = hs + hr (hj source field, and hr reaction field). [Pg.141]

In order to describe inherited stress state of weldment the finite element modelling results are used. A series of finite element calculations were conducted to model step-by-step residual stresses as well as its redistribution due to heat treatment and operation [3]. The solutions for the reference weldment geometries are collected in the data base. If necessary (some variants of repair) the modelling is executed for this specific case. [Pg.196]

The AUGUR information on defect configuration is used to develop the three-dimensional solid model of damaged pipeline weldment by the use of geometry editor. The editor options provide by easy way creation and changing of the solid model. This model is used for fracture analysis by finite element method with appropriate cross-section stress distribution and external loads. [Pg.196]

There are of course products whose shapes do not approximate a simple standard form or where more detailed analysis is required, such as a hole, boss, or attachment point in a section of a product. With such shapes the component s geometry complicates the design analysis for plastics, glass, metal, or other material and may make it necessary to carry out a direct analysis, possibly using finite element analysis (FEA) followed with prototype testing. Examples of design concepts are presented. [Pg.138]

The finite-element method (FEM) is based on shape functions which are defined in each grid cell. The imknown fimction O is locally expanded in a basis of shape fimctions, which are usually polynomials. The expansion coefficients are determined by a Ritz-Galerkin variational principle [80], which means that the solution corresponds to the minimization of a functional form depending on the degrees of freedom of the system. Hence the FEM has certain optimality properties, but is not necessarily a conservative method. The FEM is ideally suited for complex grid geometries, and the approximation order can easily be increased, for example by extending the set of shape fimctions. [Pg.148]

Walter et al. studied the flow distribution in simple multichannel geometries by means of the finite-element method [112]. In order to reduce the computational effort, a 2-D model was set up to mimic the 3-D multichannel geometry. Even at a comparatively small Reynolds number of 30 they found recirculation zones in the flow distribution chamber and corresponding deviations from the mean flow rate inside the channels of about 20%. They also investigated the influence of contact time variation on a simple two-step reaction. [Pg.177]

Avalosse, Th., and Crochet, M. J., Finite element simulation of mixing 1. Two-dimensional flow in periodic geometry. AlChE J. 43, 577-587 (1997a). [Pg.199]

In these last researches, a continuous feedback between the process study and the prototype design and development was established. In this way FEM (Finite element method) simulation has provided useful information about geometry, ultrasound intensity distribution and structural material coupling [37, 48, 49] for the design of an optimized sonoelectrochemical reactor. [Pg.113]

Commercially available CFD codes use one of the three basic spatial discretization methods finite differences (FD), finite volumes (FV), or finite elements (FE). Earlier CFD codes used FD or FV methods and have been used in stress and flow problems. The major disadvantage of the FD method is that it is limited to structured grids, which are hard to apply to complex geometries and... [Pg.315]

The inclusion of chemical reaction into CFD packed-tube simulations is a relatively new development. Thus far, it has been reported only by groups using LBM approaches however, there is no reason not to expect similar advances from groups using finite volume or finite element CFD methods. The study by Zeiser et al. (2001) also included a simplified geometry for reaction. They simulated the reaction A + B - C on the outer surface of a single square particle on the axis of a 2D channel (Fig. 16). [Pg.355]

Different techniques are commonly used to solve the diffusion equation (Carslaw and Jaeger, 1959). Analytic solutions can be found by variable separation, Fourier transforms or more conveniently Laplace transforms and other special techniques such as point sources or Green functions. Numerical solutions are calculated for the cases which have no simple analytic solution by finite differences (Mitchell, 1969 Fletcher, 1991), which is the simplest technique to implement, but also finite elements, particularly useful for complicated geometry (Zienkiewicz, 1977), and collocation methods (Finlayson, 1972). [Pg.428]

Membrane-like microstructures are generally several micrometers thick, while the lateral dimensions of the structures and the surrounding package are on the order of a few hundred micrometers. If the layered thin-film structure would be directly transferred to a 3-d geometry model, an enormous number of finite elements would be created, as the smallest structure size determines the mesh density. Averaging the structural information and properties over the different layers in the cross section of the membrane is a good method to avoid such problems. The membrane is, therefore, initially treated as a quasi-two-dimensional object. [Pg.20]

Klein, 1., The Melting Factor in Extruder Performance, SPEL, 28, 47 (1972) Altinkaynak, A., Three-Dimensional Finite Element Simulation of Polymer Melting and Flow in a Single-Screw Extruder Optimization of Screw Channel Geometry, Ph. D. Thesis, Michigan Technological University, Houghton, MI (2010)... [Pg.244]

Figure 54. Measured (a) and simulated (b) effect of electrode misalignment, (a) Total-cell and balf-cell impedances of a symmetric LSC/rare-earth-doped ceria/LSC cell with nominally identical porous LSC x= 0.4) electrodes, measured at 750 °C in air based on tbe cell geometry shown. (b) Finite-element calculation of tbe total-cell and half-cell impedances of a symmetric cell with identical R—C electrodes, assuming a misalignment of the two working electrodes (d) equal to the thickness of the electrolyte (L). ... Figure 54. Measured (a) and simulated (b) effect of electrode misalignment, (a) Total-cell and balf-cell impedances of a symmetric LSC/rare-earth-doped ceria/LSC cell with nominally identical porous LSC x= 0.4) electrodes, measured at 750 °C in air based on tbe cell geometry shown. (b) Finite-element calculation of tbe total-cell and half-cell impedances of a symmetric cell with identical R—C electrodes, assuming a misalignment of the two working electrodes (d) equal to the thickness of the electrolyte (L). ...
Fig. 8.9. Stress fields at the end of a trench etched in a 15f Fig. 8.9. Stress fields at the end of a trench etched in a 15f<m thick layer of sputtered alumina on a glass substrate. The trench was 15frm deep, 0.4 mm wide, and 10 mm long. The long-range residual stress in the alumina layer measured from the curvature of the glass substrate was —40 MPa (compressive). The top two collages are photographs of one end of the trench with measurements by acoustic microscopy of (a) the sum of the stresses axx + ayy and (b) the difference of the stresses ayy — axx f = 670 MHz. The bottom two pictures are finite-element calculations of the same geometries, with the points AB corresponding to those in the upper pictures and the colour scales corresponding in each case to the picture above, of (c) the sum of the stresses axx + ayy and (d) the difference of the stresses ayy — axx (Meeks et al. 1989).

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See also in sourсe #XX -- [ Pg.183 , Pg.184 , Pg.185 ]




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