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Solid principle states

A special short-lime performance of thermal insulation is the ablative protection on the bottom of asiroitautical capsules returning from outer space when they are heated to sudden high temperatures by impact with the atmosphere. As principles stated below indicate, ablation is the process of resisting heat flow by using absorplancc in changes of slate from solid to liquid and lo sapor of the ablative insulation, which is [hereby lost, so that a one-time or at most a lew times of exposure is practicable. [Pg.854]

You were first introduced to the common-ion effect in the previous chapter on acids and bases. The basic principle behind the effect relates back to Le Chatelier s Principle, which was first introduced in Chapter 13. If you recall, one aspect of Le Chatelier s Principle states that an increase in the concentration of a reactant will shift the equilibrium of the system in a way that will relieve the distress, or that will help reduce the concentration of the newly added reactant. When an ionic solute dissolves, it is broken into its constituent ions. When equilibrium is established, the dissolved solute is in equilibrium with its solid. At this point, if any of the constituent ions are added, they will cause a shift in the equilibrium. [Pg.358]

Figure 7 Principle of field electron emission spectroscopy, (a) Electrons in a free electron solid occupy states of surface density N(E) (i), tunnel through a triangular barrier (ii), to yield a TED spectrum (iii), and R(E) of unity (iv). (b) The enhanced density of occupied states lying AE below Fermi level Ef (i), produced by the broadened level of adatom A (ii), leads to change in the TED (iii), and a resultant peak in R(E) at AE below Ef (iv)... Figure 7 Principle of field electron emission spectroscopy, (a) Electrons in a free electron solid occupy states of surface density N(E) (i), tunnel through a triangular barrier (ii), to yield a TED spectrum (iii), and R(E) of unity (iv). (b) The enhanced density of occupied states lying AE below Fermi level Ef (i), produced by the broadened level of adatom A (ii), leads to change in the TED (iii), and a resultant peak in R(E) at AE below Ef (iv)...
Another important factor for coordination chemists is the general principle stated simply by Basolo solid salts separate from aqueous solution easiest for combinations of either small cation-small anion or large cation-large anion, preferably with systems having the same but opposite charges on the counter ions. Other factors governing solubility of salts are pH, interionic attraction, and the diverse ion effect, which will not be covered in detail here. [Pg.19]

Author of this article has made an attempt to extend further our notions of liquid [11,12]. It is considered now that sublimation is a direct transition from solid (crystalline) state of matter into gas. The author has propounded and substantiated the principle of least time for first-order phase transitions [11,13] it is shown by means of this principle that sublimation goes in two steps through a certain intermediate state in the form of surface film. It is concluded that this film consists of nonstructural liquidlike substance which is a certain antipode of liquid this liquidlike state of matter is named second licjuid [12]. [Pg.309]

In phenomenology terms, the principle states that when different phenomena are combined, the resulted dynamical system will carry only symmetries common to the phenomena involved. At a crystalline level, this means that the state of a solid system depends both on the symmetry of the crystal free of any external influence and on the S5mimetry of the action externally applied and independent by the crystal presence. [Pg.187]

Archimedes principle applies to specific weight of solids denser than water. The principle states that ... [Pg.308]

In practice, there often is something we can do to drive a reaction in the direction we want. Le Chatelier s principle states that a system at equilibrium responds to stress in such a way as to relieve that stress. This statement means that if we increase the concentration of one of the starting materials, an equilibrium process will be driven toward products. In Eqs. (8.1-8.3), if we increase [A] , the quantity [C] [D] /[B] must also increase to maintain K, and we will have more product. Similarly, if we can remove one product as it is formed, the equilibrium will be driven toward products. Perhaps either C or D is a solid that crystallizes out of solution or is a gas that can be driven off. As the concentration of this compound drops, the equilibrium will be disturbed and more C or D will be formed. [Pg.336]

However, most solids processing technology do not have this level of maturity yet. In this case, scale-up studies reduce uncertainties in the design and operation of the scaled unit most economically. On this basis, the starting point in scale-up must really be the commercial unit. In theory, once sufficient information for the commercial unit is known, scale-up can be done by applying the similarity principles from data collected on a smaller unit. The similarity principle states (3) Two processes can be considered similar if they take place in similar geometric space and all dimensionless groups required to describe the processes have the same numerical values. [Pg.460]

In general, pressure change has little effect on the solubility of a liquid or solid in water, but the solubility of a gas is very much affected by pressure. The qualitative effect of a change in pressure on the solubility of a gas can be predicted from Le Chatelier s principle. Le Chatelier s principle states that when a system in equilibrium is disturbed by a change of temperature, pressure, or concentration variable, the system shifts in equilibrium composition in a way that tends to counteract this change of variable. Let us see how Le Chatelier s principle can predict the effect of a change in pressure on gas solubility. [Pg.488]

With an irregular solid, like a rock, you can measure the volume by using the Archimedes principle. The Archimedes principle states that the volume of a solid is equal to the volume of water it displaces. Simply read the volume of water in a container, submerge the solid object, and read the volume level again. The difference is the volume of the object. [Pg.14]

Systems involving an interface are often metastable, that is, essentially in equilibrium in some aspects although in principle evolving slowly to a final state of global equilibrium. The solid-vapor interface is a good example of this. We can have adsorption equilibrium and calculate various thermodynamic quantities for the adsorption process yet the particles of a solid are unstable toward a drift to the final equilibrium condition of a single, perfect crystal. Much of Chapters IX and XVII are thus thermodynamic in content. [Pg.2]

The principal dilTerence from liquid-state NMR is that the interactions which are averaged by molecular motion on the NMR timescale in liquids lead, because of their anisotropic nature, to much wider lines in solids. Extra infonnation is, in principle, available but is often masked by the lower resolution. Thus, many of the teclmiques developed for liquid-state NMR are not currently feasible in the solid state. Furthemiore, the increased linewidth and the methods used to achieve high resolution put more demands on the spectrometer. Nevertheless, the field of solid-state NMR is advancing rapidly, with a steady stream of new experiments forthcoming. [Pg.1466]

NMR basic principles and progress specialised monograph giving detailed descriptions of specific areas of solid state NMR. [Pg.1499]

Exchange in the solid state follows die same basic principles as in liquids. The classic Cope re-arrangement of bullvalene occurs in both the liquid and solid state [25], and the lineshapes in the spectra are similar. [Pg.2110]

It follows from this discussion that all of the transport properties can be derived in principle from the simple kinetic dreoty of gases, and their interrelationship tlu ough k and c leads one to expect that they are all characterized by a relatively small temperature coefficient. The simple theory suggests tlrat this should be a dependence on 7 /, but because of intermolecular forces, the experimental results usually indicate a larger temperature dependence even up to for the case of molecular inter-diffusion. The Anhenius equation which would involve an enthalpy of activation does not apply because no activated state is involved in the transport processes. If, however, the temperature dependence of these processes is fitted to such an expression as an algebraic approximation, tlren an activation enthalpy of a few kilojoules is observed. It will thus be found that when tire kinetics of a gas-solid or liquid reaction depends upon the transport properties of the gas phase, the apparent activation entlralpy will be a few kilojoules only (less than 50 kJ). [Pg.112]

M Bee. Quasielastic Neutron Scattering Principles and Applications m Solid State Chemistry, Biology and Materials Science. Philadelphia Adam Hilger, 1988. [Pg.251]

D. Norman. J. Phys. C Solid State Phys. 19,3273, 1986. Reprinted with an appendix bringing it up to date in 1990 as pp. 197-242 in Current Topics in Condensed Matter Spectroscopy Adam HUger, 1990. An extensive review of SEXAFS and NEXAFS, concentrating on physical principles. [Pg.239]

Gurgel and Grenier s results showed the bed conductivity to increase from 0.14 to 0.17 W/mK as the pressure was raised from 4 mbar (evaporating pressure) to 110 mbar (condensing pressure). The principle reason stated for this small variation is the reduction in the gas conductivity with decreasing pressure (Knudsen effect) in the macropores. The solid grain conductivity varied linearly from 0.61 to 0.65 W/mK as the methanol concentration varied from 0 to 31%. [Pg.335]

Crystallography is a very broad science, stretching from crystal-structure determination to crystal physics (especially the systematic study and mathematical analysis of anisotropy), crystal chemistry and the geometrical study of phase transitions in the solid state, and stretching to the prediction of crystal structures from first principles this last is very active nowadays and is entirely dependent on recent advances in the electron theory of solids. There is also a flourishing field of applied crystallography, encompassing such skills as the determination of preferred orientations, alias textures, in polycrystalline assemblies. It would be fair to say that... [Pg.71]


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See also in sourсe #XX -- [ Pg.3895 ]




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