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Evolution of the dimensionless power spectral density of de-

Evolution of the dimensionless power spectral density of moments y at a central point A near the obtuse angle real time is a t c.

Evolution of the dimensionless sinface deformation y as a function of dimensionless distance j

Evolution of the dipole moment and the open square to PCM calculations

Evolution of the dipole moment of acetone with the iteration step

Evolution of the dipole moment, the polarisability and the first and second hyperpolarisabilities of the model molecule of

Evolution of the dispersed morphology along the TSMEE mixing element at three operating conditions of the weak matrix Blend 1

Evolution of the dispersion D Do versus time at 650 C in pure N2

Evolution of the dispersive component of the surface free energy of esterified silicas versus heat treatment temperature.

Evolution of the dispersive component of the surface free energy of silicas versus heat treatment temperature.

Evolution of the distance R from the center of a box of ions of alkali halide crystals in water, and corresponding diagrams for CsF with the Cs atom having the same atomic weight as the F atom.

Evolution of the distribution of Ga liquid on a Pb crystal as temperature is increased from 586K.

Evolution of the distribution of sulphur leaving a refinery between 1996 and 2005

Evolution of the DOS in PbssSess at room temperature. The DOS fluctuates due to thermal atomic motions. Both electrons and holes relax within a picosecond. Holes decays faster than electrons due to higher DOS. The relaxation involves all starts at energies in the range of the photoexcited and band gap states.

Evolution of the double edge-notched impact strength, dNIS, with the logarithm of the melt flow rate, MFR, a at room temperature and b - 20 C. The test speed was abont 3.8 ms, the specimens were injection molded

Evolution of the double edge-notched impact strength, dNIS, with the logarithm of the melt flow rate, MFR, a at room temperature and b - 20 C. The test speed was about 3.8 ms4, the specimens were injection molded

Evolution of the double-layer thickness with the ionic strength of the solution for a 1 1 electrolyte.

Evolution of the DQ signal intensity

Evolution of the droplet size distribution with time for an OAV emulsion containing 90 wt oU and 24.4 mg of sUica particles.

Evolution of the dynamic boundary layer thickness

Evolution of the dynamic onset time, as a function of the average shear rate. Results are compared with those of Ziegleder shown in dashed lines. The slope of the lines is estimated with least squares.

Evolution of the E-modulus and Izod notched impact strength of composites based on PP MFR

Evolution of the effective plastic strain in a crystal oriented in the direction shocked to a peak pressure of 4.5 GPa.

Evolution of the effective thermal conductivity X of some monolithic silica aerogels .

Evolution of the eigenvalues as the translating mass, m, is varied



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