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Distribution average

Distribution Averages. The most commonly used quantities for describing the average diameter of a particle population are the mean, mode, median, and geometric mean. The mean diameter, d, is statistically calculated and in one form or another represents the size of a particle population. It is usefiil for comparing various populations of particles. [Pg.126]

Superfine PETN for use in EBW detonators and MDF is produced by quenching a hot ace tone soln in cold water. The resulting particle size distribution averages 10 microns, and irregular crystals are produced which are easier to initiate (Ref 80a)... [Pg.570]

Note that the additional factor within the average, the n j (1 — bj), would be zero for any solvent configuration in which a solvent molecule is found in the inner shell. Thus, this expression involves a potential distribution average under the constraint that no binding in the inner shell is permitted. We can formally write the full expression for the excess chemical potential as... [Pg.323]

Equations (5.2)—(5.4) and Figs. 5.1-5.3 illustrate the nature of the structural observables obtained from gas-electron diffraction the intensity data provide intemuclear distances which are weighted averages of the expectation values of the individual vibrational molecular states. This presentation clearly illustrates that the temperature-dependent observable distribution averages are conceptually quite different from the singular, nonobservable and temperature independent equilibrium distances, usually denoted r -type distances, obtained from ab initio geometry optimizations. [Pg.137]

Fig. 5.2 Radial distribution curves, Pv Fig. 5.2 Radial distribution curves, Pv <v(r) 2/r for different vibrational states of carbon monosulfide, C = S, calcualted2 for Boltzmann distributions, with pv = exp(—EJkT), at T = 1000K (top) and T = 5000K (bottom) arbitrarily selected for the sake of illustration, where Ev is the energy level of state v. The figure conveys an impression of how state-average distance values, which can be derived from experimental spectroscopic data, differ from distribution-average values, derived from electron diffraction data for an ensemble of molecules at a given vibrational temperature. Both observables in turn differ from the unobservable stateless equilibrium distances which are temperature-independent in the Born-Oppenheimer approximation.
This fact allows the effective relaxation of steric repulsion. The potential barrier for the motion around the C—C single bonds is smaller than that corresponding to the motion around the central C=C bond. Using the potential functions computed for these motions, and assuming a Boltzmann distribution, average torsional angles of 7.7 and 7.1, at 300 K, are obtained for rotations around Cl—C3 and C1=C2, respectively. This torsional motion seems to be due to the nonplanar structure observed experimentally. [Pg.10]

Particle size measurement, 18 132-156 data representation in, 18 133-138 distribution averages in, 18 134-136 ensemble methods for, 18 151-154... [Pg.674]

The dissolved polymer molecules are separated on the basis of their size relative to the pores of a packing material contained in a column. The chromatograms can be converted to molar mass distributions, average molar masses, Mn, M, and M, long-chain branching and its distribution. [Pg.170]

Distribution - Amiodarone has a very large but variable volume of distribution, averaging about 60 L/kg. One major metabolite, desethylamiodarone (DEA), accumulates to an even greater extent in almost all tissues. The drug is highly protein bound (approximately 96%). [Pg.469]

Distribution - Average volume of distribution is 0.45 L/kg (range, 0.3 to 0.7 L/kg). Theophylline does not distribute into fatty tissue. Approximately 40% is bound to plasma protein. Therapeutic serum levels generally range from 10 to 20 mcg/mL. [Pg.736]

Absorption/Distribution - Orally administered duloxetine is well absorbed. There is a median 2-hour lag until absorption begins, with C ax occurring 6 hours postdose. Food does not affect the C ax duloxetine but delays the time to reach peak concentration from 6 to 10 hours. The apparent volume of distribution averages approximately 1,640 L. Duloxetine is highly bound (more... [Pg.1069]

Absorption/Distrlbutlon - Phenytoin is slowly absorbed from the small intestine. Rate and extent of absorption varies and is dependent on the product formulation. Bioavailability may differ among products of different manufacturers. Administration IM results in precipitation of phenytoin at the injection site, resulting in slow and erratic absorption, which may continue for up to 5 days or more. Plasma protein binding is 87% to 93% and is lower in uremic patients and neonates. Volume of distribution averages 0.6 L/kg. Phenytoin s therapeutic plasma concentration is 10 to 20 mcg/mL, although many patients achieve complete seizure control at lower serum concentrations. [Pg.1209]

Plasma protein binding is 99.8%. It is extensively distributed into tissues that are prone to fungal invasion. Concentrations in the lung, kidney, liver, bone, stomach, spleen, and muscle were found to be 2 to 3 times higher than the corresponding plasma concentration. Following IV administration, the volume of distribution averaged 796 185 L. [Pg.1685]

For a harmonic oscillator, the probability distribution averaged over all populated energy levels is a Gaussian function, centered at the equilibrium position. For the classical harmonic oscillator, this follows directly from the expression of a Boltzmann distribution in a quadratic potential. The result for the quantum-mechanical harmonic oscillator, referred to as Bloch s theorem, is less obvious, as a population-weighted average over all discrete levels must be evaluated (see, e.g., Prince 1982). [Pg.28]

The main purpose of the method is to define molecular shapes through isodensity surfaces. Tests on a number of small molecules show that this aim is achieved with a great efficiency in computer time. Discrepancies between MEDLA densities and theoretical distributions, averaged over the grid points, are typically below 10% of the total density. While this does not correspond to an adequate accuracy for an X-ray scattering model, the results do provide important information on the shapes of macromolecules. [Pg.277]

The field of droplet statistics involves a strong mutual dependence between the experimental techniques which are used to obtain the drop-size data and the mathematical formalism required to interpret and summarize the data. Special experimental techniques may lead to drop-size distributions, averages, and measures of dispersion that are appropriate to no other technique. Any attempt to restrict all techniques to the use of certain prescribed distributions together with certain mean diameters appears doomed. At present, only general outlines of the mathematical criteria appropriate to all techniques are discernible. These criteria merely prescribe that the parameters appropriate to drop-size analysis should have known distributions, and that the various measures of... [Pg.164]

Stable colloidal forms of nanocomposites protected with the polymer 12a have been recently synthesized (Scheme 5) [75]. Gold colloidal particles were formed with narrow size distribution (average size 6 nm) via reduction of HAuCLt by 12a due to its electron donating property. The oxidized polymer then protected and stabilized the gold nanoparticles which were stable in... [Pg.87]

The ideal gas law has been used in many examples in earlier chapters, and some of the important physical properties of gases (the one-dimensional velocity distribution, average speed, and diffusion) were presented in Chapter 4. This chapter puts all of these results into a more comprehensive framework. For example, in Section 7.3 we work out how the diffusion constant scales with pressure and temperature, and we explore corrections to the ideal gas law. [Pg.149]

The dispersion contribution to the interaction energy in small molecular clusters has been extensively studied in the past decades. The expression used in PCM is based on the formulation of the theory expressed in terms of dynamical polarizabilities. The Qdis(r, r ) operator is reworked as the sum of two operators, mono- and bielectronic, both based on the solvent electronic charge distribution averaged over the whole body of the solvent. For the two-electron term there is the need for two properties of the solvent (its refractive index ns, and the first ionization potential) and for a property of the solute, the average transition energy toM. The two operators are inserted in the Hamiltonian (1.2) in the form of a discretized surface integral, with a finite number of elements [15]. [Pg.8]

PORE VOLUME DISTRIBUTION AVERAGE RP 51.9 TOTAL PORE VOLUME 0.4683 SUM AP 193.5... [Pg.138]

PORE VOLUME DISTRIBUTION AVERAGE RP 26 6 TOTAL PORE VOLUME 0.6572 SUM AP 691 9... [Pg.140]

PORE VOLUME DISTRIBUTION AVERAGE RP 24.1 TOTAL PORE VOLUME 0.4331 SUM AP 358.4... [Pg.141]

The reaction of nucleobase radicals with thiols is of importance in the context of chemical repair of DNA in cells that have been exposed to ionizing radiation. The thiol that is mainly responsible for this reaction is glutathione (GSH) that is present in cells at a concentration of 1-2 mM (unevenly distributed, average value).The reaction of GSH with the nucleobase radicals is not very fast, in the order of 10 Moreover, this reaction rarely restitutes the... [Pg.552]


See other pages where Distribution average is mentioned: [Pg.476]    [Pg.266]    [Pg.112]    [Pg.413]    [Pg.95]    [Pg.75]    [Pg.34]    [Pg.62]    [Pg.11]    [Pg.12]    [Pg.191]    [Pg.328]    [Pg.21]    [Pg.88]    [Pg.558]    [Pg.33]    [Pg.93]    [Pg.112]    [Pg.259]    [Pg.126]    [Pg.119]    [Pg.131]    [Pg.144]    [Pg.196]   


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Average Molecular Weights - Moments of the Distribution

Average Molecular Weights for the Most Probable Distribution

Average Values in Terms of Lower-Order Distribution Functions

Average composition distribution

Average probability distribution

Average probability distribution oscillators

Average sequence length mean distributions

Average, standard deviation, normal distribution

Averaged momentum distribution

Averaging over the initial distribution

Calculation of average values using the Maxwell distribution

Distribution averaging, inversion

Distribution coefficient weight-average

Distribution function calculation average value

Maxwell velocity distribution function average

Molecular mass distribution number-average

Molecular weight distribution averages

Molecular weight distribution number average

Number chain length distribution weight average

Particle Size Distributions and Averaged Diameters

Particle-size distribution volume average

Phase Space Distributions and Microcanonical Averages

Potential distribution theorem view of averages

Rate Distribution and Averages of Bimodal Polymer

Residence time distribution averaging uniformity

Size distribution function averaging

Time-averaged distribution

Velocity Distribution and Average Energy of Gases

Viscosity-average molecular weight distribution

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