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The solid curve for desipramine in

The solid curve in each panel is the UY photoemission signal obtained from the silica substrate without platinum clusters and the dashed curves represent the UY signal obtained when clusters are present.

The solid curve is for the upper surface and the dotted line is for the lower surface. From ref. .

The solid curve is the best fit of the impedance spectrum by four RC meshes in series.

The solid curve is the dimensionless shear stress versus dimensionless shear rate yrd predicted by the Doi-Edwards constitutive equation, Eq.

The solid curve is the Mittag-Leffler function, the solution to the fractional relaxation equation. The dashed curve is the stretched exponential .

The solid curve is the normalized pulse width ctj 2 co of E 1- for the step profile. When the fiber materials are dispersive, the dashed curve plots the normalized pulse width cti zn, which shifts the optimum profile exponent from g p, s 1.98 to gopt -I- gopt 2.26, assuming weak guidance . For all three plots A 0.01, or 6c 0.14.

The solid curve labeled q x k Tai shows the shear traction versus distance kx hf, as determined from the numerical solution of the elastic membrane problem. The dashed curve shows the square root singular behavior of the shear traction anticipated in .

The solid curve represent the exact solution to the pulse voltage problem obtained numerically the dashed curve is an approximate solution to the problem shown by Eq.

The solid curve represents the solution to Example 12-4 in which a correct value of 0.547 moles is obtained for nL.

The solid curve shows the driving force VFm tending to extend a film crack versus the depth of penetration of that crack. The dashed curve shows the material resistance to extension as the function of depth, drawn in this case for Fs 2Ff.

The solid curve shows the fit of the model to experiment 99ma7. The fit parameters, in this case, are

The solid curve, already shown in

The solid curves and data points do not include the geometric phase. The short dashed curves and open squares include

The solid curves are and the dotted curves are x corrected for both mass flow and diffusion.

The solid curves are the best fits fiom Eq. . Strength-flaw size relations in the three examples of

The solid curves are the number of visible monolayers calculated by Monte Carlo for a well-ordered thermally vibrating crystal. Curve I in shows the expected behavior from

The solid curves in this figure show typical maximal beam intensities that can be obtained in antiparticle beams of Ax 1cm and Ad 10 as function of the particle velocity with presently available techniques. The dashed curve shows corresponding intensities of better defined beams, namely with Ax --2 mm and Ad - T.

The solid curves show the distribution of interface normal and shear traction near a film edge for the case when the elastic properties of the two materials are identical as determined by means of the nnmerical finite element method. The corresponding traction distributions based on plate theory and shown in Figure 4.5 are included as dashed curves for purposes of comparison.

The solid curves show the interface tractions between the film and substrate as determined from the numerical solution of the integral equation . The dashed curves show the corresponding internal stress resultants in eqnihbrinm with the computed interface tractions.

The solid curves were obtained by averaging Eq.

The SOLID CYLINDER primitive

The solid geometric model of complete denture

The solid gray horizontal lines indicate the vibrational frequencies given by the dynamical matrix of the original static configuration. The regions labeled I, IT IV, V, and VI are the same as those in

The solid line corresponds to the total ab initio energy for the pair interaction.



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