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Matter condensed states

It is because these primary and secondary bonds can form that matter condenses from the gaseous state to give liquids and solids. Five distinct condensed states of matter,... [Pg.42]

From X-ray measurements in the liquid crystalline phase it is impossible to determine the conformation of the molecules in the condensed state. Computer simulations give us information about the molecules internal freedom in vacuum, but the conformations of the molecules in the condensed state can be different because of intermolecular repulsion or attraction. But it may be assumed that the molecular conformations in the solid state are among the most stable conformations of the molecules in the condensed matter and therefore also among the most probable conformations in the liquid crystalline state. Thus, as more crystallo-graphically independent molecules in the unit cell exist, the more we can learn about the internal molecular freedom of the molecules in the condensed state. [Pg.192]

The basic modem data describing the atomic stmcture of matter have been obtained by the using of diffraction methods - X-ray, neutron and electron diffraction. All three radiations are used not only for the stmcture analysis of various natural and synthetic crystals - inorganic, metallic, organic, biological crystals but also for the analysis of other condensed states of matter - quasicrystals, incommensurate phases, and partly disordered system, namely, for high-molecular polymers, liquid crystals, amorphous substances and liquids, and isolated molecules in vapours or gases. This tremendous... [Pg.85]

Intermolecular forces are responsible for the condensed states of matter. The particles making up solids and liquids are held together by intermolecular forces, and these forces affect a number of the physical properties of matter in these two states. Intermolecular forces are quite a bit weaker than the covalent and ionic bonds discussed in Chapter 7. The latter requires several hundred to several thousand kilojoules per mole to break. The strength of intermolecular forces are a few to tens of kilojoules per... [Pg.86]

When atoms or molecules have less kinetic energy, or when that energy must compete with other effects (like high pressure or strong attractive forces), the matter ceases to be in the diffuse, gaseous state and comes together into one of the condensed states liquid or solid. Here are the differences between the other two ... [Pg.150]

The temperatures and pressures at which different types of matter switch between states depend on the unique properties of the atoms or molecules within that matter. Typically, particles that cire very attracted to one another and have easily stackable shapes tend toward condensed states at room temperature. Particles with no mutual attraction (or that have mutual repulsion) and with not so easily stackable shapes tend toward the gaseous state. Think of a football game between fiercely rival schools. When fans of either school sit in their own section of the stands, the crowd is orderly, sitting nicely in rows. Put rival fans in the same section of the stands, however, and they ll repel each other with great energy. [Pg.150]

As a possible mechanism we investigated the energy release produced by the phase transitions of the high density matter (transitions to the pion condensed state or to the quark matter) the newly born neutron star collapses due to the phase transitions between the second and the third bunch of the neutrino events and releases the energy necessary for the last three events. [Pg.430]

One of the most specific and unique features of low-molecular liquid crystals is their ability for orientation in external fields — mechanical, electric and magnetic. It is this property that establishes wide capabilities for technical application of liquid crystals. Today electric and magnetic optics of liquid crystals are an independent and useful for practics branch of the physics of the condensed state of matter 42 43 ... [Pg.225]

Interest in the field of nonlinear optics has grown tremendously in recent years. This is due, at least partially, to the technological potential of certain nonlinear optical effects for photonic based technologies. In addition, the responses generated through nonlinear optical interactions in molecules and materials are intimately related to molecular electronic structure as well as atomic and molecular arrangement in condensed states of matter. [Pg.37]

The robust, well-shielded cavity found in hemicarcerands offers tremendous scope for the use of these hosts as micro-reaction vessels in order to protect reactive species from bimolecular decomposition by isolating them from the outside medium. Furthermore, the unique intracavity environment with its fluid-like properties in which guest species are, formally, in a very condensed state at very high pressures, may well result in unique inclusion reactivity. Indeed, the inner volume of carcerands and hemicarcerands has been described as a new phase of matter distinct from solid, liquid and gas. A number of elegant demonstrations have been made of the potential of inclusion reactions, and there is clearly a great deal of scope for their use as molecular reaction vessels. [Pg.410]

The picture of formation of states with broken symmetry is of significant interest. Approximately 15 billion years ago, immediately after the Big Bang at the temperature of T 1045 K the Universe system was in a quite symmetric state with respect to all its elementary particles. By expansion and cooling, a series of consequent spontaneous SB took place resulting in states with consequently decreasing symmetry. At T 104 — 103 K the first elements of condensed matter -atoms—were formed. Further cooling lead to the next consequent spontaneous SB resulting in new phases of condensed states with lower symmetry. However, the mechanism of formation of these SB states and its relation to the structure of matter is not fully explored. [Pg.5]

Intermolecular forces are the attractive forces that hold molecules and ions together. These forces should not be confused with the intramolecular forces that hold the atoms together in a covalent molecule (see Lesson 11, Molecular Structure ). Intermolecular forces are grouped into four classifications, each supporting the existence of the condensed states of matter solids and liquids. In addition, these forces can also explain the nonideal behavior of certain gases. [Pg.101]

Recall that atoms can form stable units called molecules by sharing electrons. This is called intramolecular (within the molecule) bonding. In this chapter we will consider the properties of the condensed states of matter (liquids and solids) and the forces that cause the aggregation of the components of a substance to form a liquid or a solid. These forces may involve covalent or ionic bonding, or they may involve weaker interactions usually called intermolecular forces (because they occur between, rather than within, molecules). [Pg.765]

Condensed states of matter liquids and solids. (16.1) Conduction bands the molecular orbitals that can be occupied by mobile electrons, which are free to travel throughout a metal crystal to conduct electricity or heat. (16.4) Conjugate acid the species formed when a proton is added to a base. (7.1)... [Pg.1100]

MD simulations today, are the only reliable way to perform many-body calculations in the condensed states of matter. This computational disciplin has, within the last three decades, become an established area of Science and is continously developing with faster computers, more efficient algorithms and improved, more detailed physical models to treat molecular systems. [Pg.232]

A. V. Sechkarev and P. T. Nikolaenko. Investigation of intermolecular dynamics in the condensed states of matter by the method of vibrational spectroscopy. Part 1 Intensity distribution and intermolecular light scattering spectra in the neighborhood of the Rayleigh line. Izv. Vuz. Fiz. [U.S.S.R.), 4 104-110 (1969). [Pg.492]

As discussed in Section 9.2.3, despite the apparent ID nature of matter filling the channels, atoms in adjacent ICs of a bundle can interact with each other. In that case, a fuUy 3D condensation transition with a nonzero critical temperature can happen where the final condensed state is an anisotropic liquid [47-49]. This state is much more stable than the ID liquid for example, the binding energy of a He system [47, 48] increases from 2 to 16 mK. Although the interchannel interaction is very weak compared with the gas-gas interaction inside the channels, its presence is enough to drive the transition. On the... [Pg.199]

It should be pointed out that H-bonding plays a fundamental role in molecular recognition in biological systems and in all systems associated with architecture of crystal or condensed state of matter [5, 6]. These kinds of interactions are in principle of a long-distant type but these aspects will not be discussed in this review. [Pg.418]

Plasma is the most common state of matter condensation liquid... [Pg.366]

From the electron configuration one can easily infer whether or not an atom (or ion) is paramagnetic. This conclusion applies only to the free individual atom and the student is cautioned not to draw conclusions about condensed states of matter of the element. Thus the free aluminum atom has one unpaired electron, but aluminum metal is diamagnetic, as is well known. [Pg.114]

Castleman A Wand Mark T D 1986 Cluster ions their formation, properties, and role in elucidating the properties of matter in the condensed state Gaseous Ion Chemistry and Mass Spectrometry ed J H Futrell (New York Wley)... [Pg.826]

Structural information about melting processes is growing quite rapidly in bulk and in its significance for the chemical physics of condensed states of matter. General statistical considerations about the numbers of ways of constructing the solid phase Wg and the liquid phase and the application of the Boltzmann expression... [Pg.459]


See other pages where Matter condensed states is mentioned: [Pg.113]    [Pg.114]    [Pg.42]    [Pg.127]    [Pg.86]    [Pg.4]    [Pg.252]    [Pg.113]    [Pg.114]    [Pg.337]    [Pg.153]    [Pg.398]    [Pg.398]    [Pg.183]    [Pg.317]    [Pg.1]    [Pg.171]    [Pg.6]    [Pg.317]    [Pg.814]    [Pg.22]    [Pg.410]    [Pg.435]    [Pg.435]    [Pg.252]   
See also in sourсe #XX -- [ Pg.765 ]




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