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Two-Dimensional Theory

We formulate boundary conditions in the two-dimensional theory of plates and shells. Denote by u = U,w), U = ui,U2), horizontal and vertical displacements at the boundary T of the mid-surface fl c R. Then the horizontal displacements U may satisfy the Dirichlet-type conditions... [Pg.17]

In the two-dimensional theory of solids, the potential energy functional for the shallow shell with the mid-surface is as follows ... [Pg.21]

The use of a line scan facility on an imaging microscope enables the applicability of the two-dimensional theory to be tested directly. In Fig. 12.5, images of glass at three different values of defocus are presented. Superimposed on each picture are line scans measured along the line indicated in the middle. [Pg.271]

Fig. 12.5. A crack from an indent in glass (a) z = 0 (b) z = — 3.8 pm (c) z = —5.2 pm ELSAM, 1.5 GHz. The experimental line-scans superimposed on the images can be compared with the plots calculated using two-dimensional theory (eqns (12.2), (12.13), and (12.14)) with elastic constants from Table 6.3 and values of defocus (a) z = 0 (b) z = —4.2 pm (c) z = —6.8 pm. The values of z in the calculations were chosen for best fit the reason for the discrepancy is not known, though no doubt there are the usual uncertainties associated with thermal drift, the measurement of z, and the frequency and pupil function used (Briggs etal. 1990). Fig. 12.5. A crack from an indent in glass (a) z = 0 (b) z = — 3.8 pm (c) z = —5.2 pm ELSAM, 1.5 GHz. The experimental line-scans superimposed on the images can be compared with the plots calculated using two-dimensional theory (eqns (12.2), (12.13), and (12.14)) with elastic constants from Table 6.3 and values of defocus (a) z = 0 (b) z = —4.2 pm (c) z = —6.8 pm. The values of z in the calculations were chosen for best fit the reason for the discrepancy is not known, though no doubt there are the usual uncertainties associated with thermal drift, the measurement of z, and the frequency and pupil function used (Briggs etal. 1990).
Beside each picture is a line scan corresponding to that value of defocus calculated using the two-dimensional theory. The agreement is not too bad, and suggests that the two-dimensional theory does indeed give a useful account of what is going on. [Pg.273]

Fig. 10.16 Scaled microwave ionization field, nAE, for H plotted against the scaled microwave frequency n3co experimental ( ) one dimensional theory (x) two dimensional theory (O). n3co = 0.05 corresponds to n = 32 and n3aj = 0.6 corresponds to n = 73. Note the decline from n4E = 1/9 at n = 30 to progressively lower values as n approaches 60 (from... Fig. 10.16 Scaled microwave ionization field, nAE, for H plotted against the scaled microwave frequency n3co experimental ( ) one dimensional theory (x) two dimensional theory (O). n3co = 0.05 corresponds to n = 32 and n3aj = 0.6 corresponds to n = 73. Note the decline from n4E = 1/9 at n = 30 to progressively lower values as n approaches 60 (from...
P. Le Guennec, Two-dimensional theory of chirality. I. Absolute chirality. J. Math. Phys. 41, 5954-5985 (2000)... [Pg.81]

To provide this basic appreciation, a brief review of two-dimensional theory of elasticity is given below, followed by a summary of the basic formulation of the crack problem. More complete treatments of the theory of elasticity may be found in standard textbooks and other treatises (e.g., Mushkilishevili [5] Sokolnikoff [6] Timoshenko [7]). [Pg.26]

Equations (] 1.2-19). (11.2-20). and (11.2-21) can be simplified considerably by recognizing that in many syslema tha quantity s is much less than 1. In that care. In (1 + r) is approximately s. Making this substitution, the growth rate from the mononuclear two-dimensional theory becomes... [Pg.596]

In the two-dimensional theory of the threshold for an electrohydrodynamic instability, developed by Pikin [49] and Penz and Ford [50], the velocity of the liquid and the director are regarded as being dependent on both the X- and -coordinates. Solutions are sought which satisfy the conditions of strong molecular anchoring at the electrodes under the following conditions for a planar orientation 6 = 0, = 0, Vz = 0, dvzidz = 0, when... [Pg.249]

FIGURE 5.7. Experimental dependences of the threshold voltage for Ka-pustin-Williams domains with a planar initial orientation (a) on the anisotropy of the electrical conductivity and (b) on the dielectric anisotropy for doped MBBA (circles) and for mixture A of azoxy compoimds (crosses). Calculation is according to a two-dimensional theory (curve 1) and a one-dimensional theory (curve 2). The threshold of the Prederiks effect for doped MBBA is shown in curve 3, which represents the theory, while the squares represent the experimental measurements [31]. [Pg.250]

Additional results have been obtained from the two dimensional theory [8] for which it is found that the non-affine character of x varies in the order uniaxial tension > tension with constrained transverse strain > equal biaxial tension. For the last case, no reorientation of elements occurs (x - 0) a.nd the t extremal for Hookean elements is identically affine. (It is emphasized that biaxial tension in a three-dimensional network does result in element reorientation.)... [Pg.79]


See other pages where Two-Dimensional Theory is mentioned: [Pg.134]    [Pg.344]    [Pg.110]    [Pg.663]    [Pg.21]    [Pg.21]    [Pg.28]    [Pg.271]    [Pg.281]    [Pg.26]    [Pg.27]    [Pg.29]    [Pg.795]    [Pg.288]    [Pg.596]    [Pg.624]    [Pg.416]    [Pg.596]    [Pg.4]    [Pg.33]    [Pg.35]    [Pg.37]    [Pg.39]    [Pg.41]    [Pg.41]   


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