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Model calculation of the absorption, centered at 150 GHz, of dipole oscillators in aqueous solution, 10 volume fraction.

Model calculation of the data presented in

Model calculation of the influence of the ionic strength on the rate of proteolysis of K-casein by chymosin. Model parameters

Model calculation of the NMR spectrum for a non-linear modulation wave, corresponding to the INC phase of Sr2Si04 with a soliton density tis 0.5. The phase of the modulation nn

Model calculation of the partitioning of free radicals and total halogen content for chlorine, bromine, and iodine at 8 N and 50 N in December. From Solomon et al. .

Model calculation of the sulfate concentration profile in the deposition of a sediment avalanche on the continental slope off the coast of Uruguay see also.

Model calculation on the basis of Eq.

Model calculation on the basis of Eq. , simulating heat capacity measurements during cooling runs with the indicated rates Ta 2000 K, Tv

Model calculation simulating changes in ocean composition as primary igneous rock minerals react with a solution containing the proportions of excess volatiles shown in Table 10.4. Concentrations of dissolved species are shown relative to 1 kilogram of water, and the extent of reaction is measured by the amount of igneous-rock minerals destroyed. Changes in slopes on diagram are due to formation of sedimentary minerals.

Model calculation, . Once the wavefunction has localised in the solid-state there is little chance of back electron transfer from the band states.

Model calculations based on nation 5, of the pulse-pH

Model calculations for hydrogen isotope effects for proton transfer reactions from carbon to various bases, jr is the order of the reacting hydrogen bond .

Model calculations for the penetration kinetics of a soluble surfactant into a monolayer at different surface coverage 01 0 , D 5.10-6cmVs, co 2.28.109 cmVmol, b 1.69.108 cmVmol according to

Model calculations for the reflectivity Drude and the metallic particles are defined by the same parameters set the plasma frequency 2 eV, the scattering rate hr 0.2 eV. A filling factor 0.5 and a dielectric host-medium represented by a Lorentz harmonic oscillator with mode strength fttOy, 1 10 eV, damping ftF I eV and resonance frequency h H 15 eV were considered for the calculations.

Model calculations of hydraulic pressure throughout the PEFC for two current densities . This calculation is for a Nafion 117 membrane, humidifier temperatures of 105 C and cell temperature of 80 C, air-side pressure of 5 atm and fuel-side pressure of 3 atm. .

Model calculations of reflectivities . Top row

Model calculations of reflectivities matches the exact reflectivity well.

Model calculations of the absorption of dipole oscillators as in

Model calculations of the diurnal variation of J in the troposphere for the 10 of June 1996, Aghios Efstratios.

Model calculations of the excitation probabilities for the Ar 2s and 2p levels in the systems N Ar and O Ar as a function of the inverse projectile velocity. The calculations are based on the SHM matrix elements .

Model calculations of the expected fraction of metal ions precipitated as .

Model calculations of the magnetic field orientation of liquid crystals. Calculations were conducted using equations 2 and 3. In comparison is made between a nonreactive liquid crystal with a constant viscosity and a reactive liquid crystal with an exponentially

Model calculations of the temporal dependence of the vertical optical thickness of a nuclear dust cloud, averaged over the Northern Hemisphere particles.

Model calculations of the time development of transient T iring patterns in a batch reactor using the six-variable model of reactions . o 3 x 10 M, Llo 8.2 X 10 M, ClO lo 1 X 10 M, o 0.1 M. Length is 5 mm shown horizontally. Total time is 30 minutes shown vertically. Number of gridpoints is 400. Rate constants and diffusion coefficients are in the fourth column of Table II.

Model calculations of vacancysharing probabilities for the systems Si Ar and S Ar as a function of the inverse projectile velocity. The calculations are based on the SHM matrix elements . The solid and dashed lines refer to Ar L excitation via the coupling of cr and ir orbitals, respectively.



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