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Unequal

While a superstructure based on the structure in Fig. 16.26 allows for many structural options, it is not comprehensive. Wood, Wilcox, and Grossmanr showed how direct contact heat transfer by mixing at unequal temperatures can be used to decrease the number of units in a heat exchanger network. Floudas, Ciric, and Grossman showed how such features can be included in a heat exchanger network superstructure. Figure 16.27 shows the structure from Fig. 16.26 with possibilities for direct contact heat transfer included. In the... [Pg.395]

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]

Surface tension arises at a fluid to fluid interface as a result of the unequal attraction between molecules of the same fluid and the adjacent fluid. For example, the molecules of water in a water droplet surrounded by air have a larger attraction to each other than to the adjacent air molecules. The imbalance of forces creates an inward pull which causes the droplet to become spherical, as the droplet minimises its surface area. A surface tension exists at the interface of the water and air, and a pressure differential exists between the water phase and the air. The pressure on the water side is greater due to the net inward forces... [Pg.120]

Upon considering the observation that even with 4 segments a detectable diffracted signal was observed, most popularly employed 4 segment EMATs, with unequal spacing and 780 kHz were tried for TOFD measurements and found to be very promising. [Pg.725]

The MS approximation for the RPM, i.e. charged hard spheres of the same size in a conthuium dielectric, was solved by Waisman and Lebowitz [46] using Laplace transfomis. The solutions can also be obtained [47] by an extension of Baxter s method to solve the PY approximation for hard spheres and sticky hard spheres. The method can be fiirtlier extended to solve the MS approximation for unsynnnetrical electrolytes (with hard cores of unequal size) and weak electrolytes, in which chemical bonding is municked by a delta fiinction interaction. We discuss the solution to the MS approximation for the syimnetrically charged RPM electrolyte. [Pg.492]

With relatively simple spectra, it is usually possible to extract the individual coupling constants by inspection, and to pair them by size in order to discover what atoms they coimect. However, the spectra of larger molecules present more of a challenge. The multiplets may overlap or be obscured by the presence of several unequal but similarly sized couplings. Also, if any chiral centres are present, then the two hydrogens in a... [Pg.1455]

Therefore, unequal populations of tlnee triplet levels results. The T, and basis fiinctions can be... [Pg.1609]

The experiment starts at equilibrium. In the high-temperature approximation, the equilibrium density operator is proportional to the sum of the operators, which will be called F. If there are multiple exchanging sites with unequal populations, p-, the sum is a weighted one, as in equation (B2.4.31). [Pg.2100]

The unequal distribution of charge produced when elements of different electronegativities combine causes a polarity of the covalent bond joining them and, unless this polarity is balanced by an equal and opposite polarity, the molecule will be a dipole and have a dipole moment (for example, a hydrogen halide). Carbon tetrachloride is one of a relatively few examples in which a strong polarity does not result in a molecular dipole. It has a tetrahedral configuration... [Pg.51]

The domain Q is discretized into a mesh of five unequal size linear finite elements, as is shown in Figure 2.21. [Pg.44]

Here /, r and, v are unequal integers in the set 1, 2, 3. As already mentioned, in the thin-layer approach the fluid is assumed to be non-elastic and hence the stress tensor here is given in ternis of the rate of deforaiation tensor as r(p) = riD(ij), where, in the present analysis, viscosity p is defined using the power law equation. The model equations are non-dimensionalized using... [Pg.177]

The hydrogenation of 2 methyl(methylene)cyclohexane is an example of a stereo selective reaction meaning one m which stereoisomeric products are formed m unequal amounts from a single starting material (Section 5 11)... [Pg.309]

Section 13 11 Complicated splitting patterns can result when a proton is unequally cou pled to two or more protons that are different from one another... [Pg.576]

Tetragonal Two equal axes and one unequal axis mutually perpendicular One fourfold axis a = b c a = /3 = 7 = 90°... [Pg.333]

Triclinic Rhombohedral Three unequal axes intersecting obliquely Two equal axes making equal angle with each other No planes or axes of symmetry a b c y 90°... [Pg.333]

By way of illustration, very simple spectra for four substances (A, B, C, D) are shown (a) separately and (b) mixed in unequal proportions. The mixture spectrum is virtually impossible to decode if A, B, C, D are not known beforehand to be present. [Pg.255]

Naturally occurring isotopes of any element are present in unequal amounts. For example, chlorine exists in two isotopic forms, one with 17 protons and 18 neutrons ( Cl) and the other with 17 protons and 20 neutrons ( Cl). The isotopes are not radioactive, and they occur, respectively, in a ratio of nearly 3 1. In a mass spectrum, any compound containing one chlorine atom will have two different molecular masses (m/z values). For example, methyl chloride (CH3CI) has masses of 15 (for the CH3) plus 35 (total = 50) for one isotope of chlorine and 15 plus 37 (total = 52) for the other isotope. Since the isotopes occur in the ratio of 3 1, molecular ions of methyl chloride will show two molecular-mass peaks at m/z values of 50 and 52, with the heights of the peaks in the ratio of 3 1 (Figure 46.4). [Pg.339]

For a fixed extent of reaction, the presence of multifunctional monomers in an equimolar mixture of reactive groups increases the degree of polymerization. Conversely, for the same mixture a lesser extent of reaction is needed to reach a specified with multifunctional reactants than without them. Remember that this entire approach is developed for the case of stoichiometric balance. If the numbers of functional groups are unequal, this effect works in opposition to the multifunctional groups. [Pg.322]

An asymmetric rotor has all principal moments of inertia unequal ... [Pg.105]


See other pages where Unequal is mentioned: [Pg.335]    [Pg.146]    [Pg.202]    [Pg.265]    [Pg.290]    [Pg.404]    [Pg.498]    [Pg.177]    [Pg.357]    [Pg.484]    [Pg.1552]    [Pg.1570]    [Pg.1607]    [Pg.2106]    [Pg.2421]    [Pg.49]    [Pg.50]    [Pg.199]    [Pg.400]    [Pg.72]    [Pg.146]    [Pg.104]    [Pg.190]    [Pg.64]    [Pg.543]    [Pg.543]    [Pg.25]    [Pg.292]    [Pg.124]    [Pg.351]   
See also in sourсe #XX -- [ Pg.81 ]

See also in sourсe #XX -- [ Pg.81 ]




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AC Discharges with Unequal Area Electrodes

Applicability of the Limited Stressed States Theories for Materials Unequally Resistant to Tension and Compression

Binary distillation unequal molal latent heats

Cell division unequal

Chemical bonding unequal electronegativities

Chromatids, sister, unequal exchange

Concluding Remarks on Unequal Spatial Intervals

Cooperation of Unequal Actuators

Crossing-over unequal

Current approximation unequal intervals

Diffusion coefficient unequal

Effect of Unequal Diffusion Coefficients

Electron unequal sharing

Equal and Unequal Shares

Fermi resonances unequal damping

Implementing unequal intervals Crank-Nicolson

Implementing unequal intervals explicit methods

Interpolation of Unequally Spaced Points

Ionic bonds, 134 unequal electron

Ionic bonds, 134 unequal electron sharing

Recombination unequal crossing-over

Repulsion, electron-pair unequal

Resonance structures, unequal

Sharing Electrons—Unequally

Splitting, unequal

Substrate binding unequal

Tolerance unequal

UNEQual class modelling

Unequal Error Variances

Unequal Molal Heats of Vaporization

Unequal Reactivity of Functional Groups

Unequal Time Intervals

Unequal class models

Unequal crossover

Unequal functional group reactivity

Unequal intervals

Unequal intervals adaptive

Unequal intervals derivative approximations

Unequal intervals discretisation

Unequal intervals four-point derivatives

Unequal molal overflow

Unequal molal overflow, distillation

Unequal randomisation

Unequal sample size

Unequally Spaced Grids

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