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In sizing

Brownian movement The rapid and random movement of particles of a colloidal sol, observed brightly lit against a dark ground. First observed with a pollen suspension. The Brownian movement is due to the impact on the dispersed particles of the molecules of the dispersion medium. As the particles increase in size, the probability of unequal bombardment from different sides decreases, and eventually collisions from all sides cancel out and the Brownian movement becomes imperceptible at a particle size of about 3-4/z. From the characteristics of the movement, Perrin calculated Avogadro s number L. [Pg.69]

At lower temperatures, the crystals increase in size, and form networks that trap the liquid and hinder its ability to flow. The pour point is attained which can, depending on the diesel fuel, vary between -15 and -30°C. This characteristic (NF T 60-105) is determined, like the cloud point, with a very rudimentary device (maintaining a test tube in the horizontal position without apparent movement of the diesel fuel inside). [Pg.215]

Table 2 compares between the VIGRAL results and mechanical measurements of the simulated FBH defects. The table lists the size of the reflecting surface,, its depth location, the Yd, and the standard deviation of the depth information, o>i( y ). We note an excellent agreement between the VIGRAL and the mechanical measurements both in size and depth of the defects. [Pg.169]

As circular domains grow in size or number, the dipolar interactions between them increase until they form a hexagonal array of spacing... [Pg.139]

The illustrative data presented in Table VII-3 indicate that the total surface energy may amount to a few tenths of a calorie per gram for particles on the order of 1 /xm in size. When the solid interface is destroyed, as by dissolving, the surface energy appears as an extra heat of solution, and with accurate calorimetry it is possible to measure the small difference between the heat of solution of coarse and of finely crystalline material. [Pg.280]

Discuss briefly which techniques listed in Table VIII-1 give information that is averaged over, that is, is representative of a macroscopic region of surface and which ones give information characteristic of a particular microscopic region. Take the dividing line of macroscopic versus microscopic to be about 1000 atoms in size.. [Pg.312]

It is known that even condensed films must have surface diffusional mobility Rideal and Tadayon [64] found that stearic acid films transferred from one surface to another by a process that seemed to involve surface diffusion to the occasional points of contact between the solids. Such transfer, of course, is observed in actual friction experiments in that an uncoated rider quickly acquires a layer of boundary lubricant from the surface over which it is passed [46]. However, there is little quantitative information available about actual surface diffusion coefficients. One value that may be relevant is that of Ross and Good [65] for butane on Spheron 6, which, for a monolayer, was about 5 x 10 cm /sec. If the average junction is about 10 cm in size, this would also be about the average distance that a film molecule would have to migrate, and the time required would be about 10 sec. This rate of Junctions passing each other corresponds to a sliding speed of 100 cm/sec so that the usual speeds of 0.01 cm/sec should not be too fast for pressurized film formation. See Ref. 62 for a study of another mechanism for surface mobility, that of evaporative hopping. [Pg.450]

The oil droplets in a certain benzene-water emulsion are nearly uniform in size and show a diffusion coefficient of 3.75 x 10 cm /sec at 25°C. Estimate the number of benzene molecules in each droplet. [Pg.527]

The previous seetion showed how the van der Waals equation was extended to binary mixtures. However, imieh of the early theoretieal treatment of binary mixtures ignored equation-of-state eflfeets (i.e. the eontributions of the expansion beyond the volume of a elose-paeked liquid) and implieitly avoided the distinetion between eonstant pressure and eonstant volume by putting the moleeules, assumed to be equal in size, into a kind of pseudo-lattiee. Figure A2.5.14 shows sohematieally an equimolar mixture of A and B, at a high temperature where the distribution is essentially random, and at a low temperature where the mixture has separated mto two virtually one-eomponent phases. [Pg.626]

Figure Bl.18.12. Illustration that only light reflected from object points in the focal plane contributes to the image. If the light is reflected from areas below the focal plane, only a small fraction can pass through the pinliole so that light from those areas does not contribute to the image. The pinliole in front of the detector is exaggerated in size for the sake of presentation. Figure Bl.18.12. Illustration that only light reflected from object points in the focal plane contributes to the image. If the light is reflected from areas below the focal plane, only a small fraction can pass through the pinliole so that light from those areas does not contribute to the image. The pinliole in front of the detector is exaggerated in size for the sake of presentation.
Islands occur particularly with adsorbates that aggregate into two-dimensional assemblies on a substrate, leaving bare substrate patches exposed between these islands. Diffraction spots, especially fractional-order spots if the adsorbate fonns a superlattice within these islands, acquire a width that depends inversely on tire average island diameter. If the islands are systematically anisotropic in size, with a long dimension primarily in one surface direction, the diffraction spots are also anisotropic, with a small width in that direction. Knowing the island size and shape gives valuable infonnation regarding the mechanisms of phase transitions, which in turn pemiit one to leam about the adsorbate-adsorbate interactions. [Pg.1769]

A microelectrode is an electrode with at least one dimension small enough that its properties are a fimction of size, typically with at least one dimension smaller than 50 pm [28, 29, 30, 31, 32 and 33]. If compared with electrodes employed in industrial-scale electrosynthesis or in laboratory-scale synthesis, where the characteristic dimensions can be of the order of metres and centimetres, respectively, or electrodes for voltannnetry with millimetre dimension, it is clear that the size of the electrodes can vary dramatically. This enonnous difference in size gives microelectrodes their unique properties of increased rate of mass transport, faster response and decreased reliance on the presence of a conducting medium. Over the past 15 years, microelectrodes have made a tremendous impact in electrochemistry. They have, for example, been used to improve the sensitivity of ASV in enviroiunental analysis, to investigate rapid... [Pg.1938]

Metallic and semiconductor nanoparticles or nanocrystals —chunks of matter intennediate in size and physical properties between single atoms and tire macroscopic bulk materials—are of great interest botli for tlieir... [Pg.2500]

Additives, whether hydrophobic solutes, other surfactants or polymers, tend to nucleate micelles at concentrations lower than in the absence of additive. Due to this nucleating effect of polymers on micellization there is often a measurable erne, usually called a critical aggregation concentration or cac, below the regular erne observed in the absence of added polymer. This cac is usually independent of polymer concentration. The size of these aggregates is usually smaller than that of free micelles, and this size tends to be small even in the presence of added salt (conditions where free micelles tend to grow in size). [Pg.2603]

There is a marked contraction in size on the formation of an ion, the percentage contraction decreasing as the percentage loss in electrons decreases (for example Na Na" involves loss of one of eleven electrons, Cs -+ Cs" the loss of one of fifty-five electrons). Some values for Group II and III elements are shown in Tables 2.2 and 2.3 respectively. [Pg.29]

In most covalent compounds, the strong covalent bonds link the atoms together into molecules, but the molecules themselves are held together by much weaker forces, hence the low melting points of molecular crystals and their inability to conduct electricity. These weak intermolecular forces are called van der WaaFs forces in general, they increase with increase in size of the molecule. Only... [Pg.47]

To date there is no evidence that sodium forms any chloride other than NaCl indeed the electronic theory of valency predicts that Na" and CU, with their noble gas configurations, are likely to be the most stable ionic species. However, since some noble gas atoms can lose electrons to form cations (p. 354) we cannot rely fully on this theory. We therefore need to examine the evidence provided by energetic data. Let us consider the formation of a number of possible ionic compounds and first, the formation of sodium dichloride , NaCl2. The energy diagram for the formation of this hypothetical compound follows the pattern of that for NaCl but an additional endothermic step is added for the second ionisation energy of sodium. The lattice energy is calculated on the assumption that the compound is ionic and that Na is comparable in size with Mg ". The data are summarised below (standard enthalpies in kJ) ... [Pg.75]

Our work is targeted to biomolecular simulation applications, where the objective is to illuminate the structure and function of biological molecules (proteins, enzymes, etc) ranging in size from dozens of atoms to tens of thousands of atoms today, with the desire to increase this limit to millions of atoms in the near future. Such molecular dynamics (MD) simulations simply apply Newton s law to each atom in the system, with the force on each atom being determined by evaluating the gradient of the potential field at each atom s position. The potential includes contributions from bonding forces. [Pg.459]

The Web-based graphical user interface permits a choice from numerous criteria and the performance of rapid searches. This service, based on the chemistry information toolkit CACTVS, provides complex Boolean searches. Flexible substructure searches have also been implemented. Users can conduct 3D pharmacophore queries in up to 25 conformations pre-calculated for each compound. Numerous output formats as well as 2D and 3D visuaHzation options are supplied. It is possible to export search results in various forms and with choices for data contents in the exported files, for structure sets ranging in size from a single compound to the entire database. Additional information and down-loadable files (in various formats) can be obtained from this service. [Pg.263]


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See also in sourсe #XX -- [ Pg.290 ]




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Adjustment for Differences in Body Size Caloric Requirement Approach

Adjustment for Differences in Body Size Exposure Route

Adjustment for Differences in Body Size PBPK Models

Applications of Size Exclusion Chromatography in Pharmaceutical Analysis

Batch Size Increase in Dry Blending and Mixing

Batch Size Increase in Fluid-Bed Granulation

Bubble and Drop Size in Stirred Vessels

Chain configuration and size in solution

Changes in cell size

Concepts in Nanometer Size Architecture

Control of the Water Pool Size in Reverse Microemulsions

DETECTION AND DATA ANALYSIS IN SIZE EXCLUSION CHROMATOGRAPHY

Dendrimer Size Change in Different Solvents

Detectors in size-exclusion chromatography

Determination of Pore Size Distribution in Porous Media

Droplet size in emulsions

Droplet size in sprays

EMS IN SMALL AND MEDIUM SIZED COMPANIES

Eddy size distribution in a turbulent flow

Equal size CFSTR in series

Ethers ring size effects, in formation

Evaluation of Particle Size in Immiscible Blends

Example 3-13 System Head Using Two Different Pipe Sizes in Same Line

Exercise 15.1 Distribution of particles in suspension and grain size sorting resulting from settling

Exercise 17.1 Grain size sorting in a hydrocyclone

Experimental Investigation of Size Effects in Nanoferroics

Experiments in Conventional Size Channels

Extraction drop size in mixers

Factors Affecting Grain Size in a Compact Deposit

Flow Conditions in Small-sized Reactors

Flow Patterns in a Single Conventional Size Channel

Forces Involved in Size Reduction

Fragment Size Distributions in Dynamic Fragmentation

Fragment Size Predictions in Dynamic Fragmentation

Genome, size of in humans

Grain size distribution in a granular medium

Growth in size and period of limit cycle

Homogeneity Distribution in Size and Shape

Hydrodynamic Cavitation Synthesis of Nanostructured Catalysts in High-Phase Purities and Varying Grain Sizes

In situ particle size and shape analysis

In situ particle size measurement

Influence of reduction in grain size

Ionic Size in Solutions

J) coupling constants in other ring sizes

Making Particles Under 10 nm in Size

NMR Pore Size Measurements Using an Internal Magnetic Field in Porous Media

New Techniques in Sub-micron Particle Size Analysis The Controlled Reference Method

Oil in gas droplet size

Oil in water droplet size

On the Size-Induced Metal-Insulator Transition in Clusters and Small Particles

Onset of Nucleate Boiling in Conventional Size Channels

Optimal Sizing of Two CSTRs Connected in Series

Particle Size Distribution in Continuous Comminution Process

Particle Size of Ag NPs in Sol-Gel Films from Optical Absorption Spectra

Particle Size on Adhesive Force in Liquid Media

Particle size distribution in emulsion polymerization

Particle size distribution in suspension polymerization

Particle size in emulsions

Particle-size analysis in the process environment

Pb shift in the aerosol size distributions

Polydispersity in particle size

Polymer Size in the Amorphous State

Quantum-size Effects in Nanocrystalline Semiconductors

Retention in size-exclusion chromatography

Separation mechanism in size-exclusion chromatography

Shape Effect in Size Characterization

Shortcut methods for determining optimum line sizing in SI units

Size Consistency Problem in the Energy

Size Effect in the Dielectric Permittivity of Crystals

Size Effects in Coexistence Conditions

Size Effects in Interfacial Width

Size Effects in the Shape of Intrinsic Coexistence Profile

Size and Dipole Moment of Water Molecules in Solution

Size distribution in linear condensation

Size distribution of particles in the

Size effects in the growth of aerosol nanoparticles and their coalescence

Size in terms of electron density

Size limitations in solution-state NMR

Size of Primary Nanoparticles in Silane Plasma

Size quantization in semiconductors

Size- and Shape-selective Preparation of Metal Nanoparticles in the Zerovalent Form

Size-Dependent Diagram and Solubilities in Multicomponent Nanomaterials

Size-dependence of plastic yielding in thin films

Sizing in paper

Testing with the use of a large-size device, in air

Testing with the use of a small-size device, procedure B, in water

Testing with the use of an extra-large-size device, in air

The Sizes of Ions in Condensed Phases

The role of compliant-particle size in toughening glassy polymers

Time to Equilibrium and Transient Drop Size in Turbulent Flow

Trends in Atomic Size

Trends in Lattice Energies Ion Size

Trends in Size

Trends in Sizes of Ions

Tumors Up to Three Centimeters in Size

Uncertainty in the sizing calculation

Understanding the Nanoparticle Size Effect in Catalysis

Use of Size Exclusion Chromatography in Biopharmaceutical Development

Use of the Energy Balance in Reactor Sizing and Analysis

Variables Involved in Sample-Size Estimation

Variation in tower size factor with approach

Variations in Atomic Size

Variations in ring size

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