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The spaces of normal and exception behavior.

The spacing and the width of the detector elements are such that the spread of a given peak is roughly equal to its mean. Therefore, 2.02 and 2.99 pm spheres cannot be resolved. In both the monodisperse and bimodal systems, FDPA measurements of 1.09 pm spheres yield 2.0 pm. This is a limitation of the technique and the geometry of the detector. The input and measured mass fractions by FDPA are in quantitative agreement. Figure 4 is a comparison of the three different techniques for a mixture of 1.09 and 2.99 pm spheres. Again 1.09 pm is not detected by FDPA.

The spacing of lines in the primary plot is important for obtaining good replots.

The spacings of planes of hexagonal crystals. Above

The span of the spectrum of electromagnetic radiation used in spectroscopic investigations of organic compounds along with comparison of some of the various units commonly employed for wavelength and energy of the radiation on log scales

The Spanish synthesis of risperidone .

The spanning of the g-edges by hexafluoroacetylacetonates in the tetrakis-complexes of the lanthanides and the actinides

The spanning tree of five psycotropic agents obtained by the similarity analysis of the fragment spectra in

The spanning tree of twelve hydrocarbons obtained by the similarity analysis of the fragment spectra weighted by the sum of degree of the subgraph nodes. The similarity value in Eq was used for the analysis

The Spartan homepage

The spatial and temporaral scales of disturbance of the intertidal environment.

The spatial arrangement of interstitial g sites in the Cl 5-type lattice ,

The spatial arrangement of the furanose sugar and the base of a nucleoside, about the glycosidic linkage.

The spatial arrangement of the particles within a port Both up and down contain the same arrangement of four non-coplanar particles except that they face opposite directions

The spatial arrangement of the substituents ,

The spatial concentration profile of drug is considered constant assuming that cq is much higher than cs.

The spatial configuration of an s orbital.

The spatial configurations of the d oibitals.

The spatial configurations ofp orbitals.

The spatial confinement inside a nanotube gives rise to crystal structure completely different from those observed for the bulk phase

The spatial dependence of field strength for the two configurations of a magnetostatic trap

The spatial dependence of the amplitude of the TC fi chirality.

The spatial dependence of the charge density, the electric field, and the electric potential in the semiconductor at equihbrium for an n-type semiconductor metal junction, where all of the voltage is dropped in the semiconductor space-charge region. The origin of the x-axis is chosen for convenience as the point closest to the interface where the net charge in the semiconductor equals zero, The distance dependence of the electric potential. The electric potential in the bulk of the semiconductor has been defined as zero. Because the sign of the electric field strength is positive, the electric potential at the interface is more negative than in the bulk

The spatial dependence of the diffusion coefficient for approach of two pheres of diameter 0.5 nm in an hydrodynamic continuum. The various estimates

The spatial distribution of parallel magnetic field strength employing strong magnets 1550 G as measured with a Walker-MG 3D gauss meter.



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