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Field of oscillating

The field of oscillating reactions, or periodic reactions, or chemical clocks, came out of this background indeed quite a number of chemical systems have been described, which show this oscillating, periodic, regular behavior (Field, 1972 Briggs and Rauscher, 1973 Shakhashiri, 1985 Noyes, 1989 Pojman etal, 1994 Jimenez-Prieto etal., 1998). [Pg.109]

The development of an adequate mechanism for the BZ reaction required nearly 15 years from the discovery of oscillations in that system, and refinement of that mechanism is still under way56. It is a measure of the progress in the field of oscillating reactions that only 15 months after the design of the first chlorite oscillator, a mechanism for that system seems well within reach. Without setting forth a full mechanistic treatment, which is not yet available, we sketch here what we believe to be the key elements in the oscillation of the chlorite-iodate-arsenite oscillator and, by extension, several of the related systems to be discussed below. A partial mechanism for the prototype chlorite-iodide system will be presented in the following section. [Pg.19]

In this article an attempt is made to include some new contributions to bring the field of oscillations in the dynamics of chemical reactions up to date. To provide a continuation, the basic structure of the paper follows the outline of the previous article which will be referred to as (G G). Moreover, some recent studies have also been added to the field, and they are included as additional sections. These new sections are L. Oxidation by Chlorite M. Miscellaneous Studies and N. General Models and Mathematical Techniques. [Pg.77]

A characteristic property of all electromagnetic radiation is the frequency of the field of oscillation, v, which remains invariant as the wave travels through any medium. The frequency is related to the velocity of the wave, c, and the wavelength, X, by the equation vA = c. It follows from this relationship that both X and c... [Pg.14]

In linear, spherical and synnnetric tops the components of a along and perpendicular to the principal axis of synnnetry are often denoted by a and respectively. In such cases, the anisotropy is simply Aa = tty -If the applied field is oscillating at a frequency w, then the dipole polarizability is frequency dependent as well a(co). The zero frequency limit of the dynamic polarizability a(oi) is the static polarizability described above. [Pg.189]

The second way to achieve quadrahire is to introduce another field, E, (called a local oscillator) designed in frequency and wavevector to conjugate (go into quadrahire) in its complex representation with the new field of interest. Thus in the heterodyne case, the signal photons are derived fromcr. jy i. or Sj (lieterodyne) x x X... [Pg.1182]

Calculations within tire framework of a reaction coordinate degrees of freedom coupled to a batli of oscillators (solvent) suggest tliat coherent oscillations in the electronic-state populations of an electron-transfer reaction in a polar solvent can be induced by subjecting tire system to a sequence of monocliromatic laser pulses on tire picosecond time scale. The ability to tailor electron transfer by such light fields is an ongoing area of interest [511 (figure C3.2.14). [Pg.2987]

The electric field of electromagnetic radiation completes 4.00 x lO - " complete cycles in 1.00 s. What are the period and frequency of the oscillation, and what is its wavelength What is the frequency in units of cm ... [Pg.166]

Near the outlet from the torch, at the end of the concentric tubes, a radio high-frequency coil produces a rapidly oscillating electromagnetic field in the flowing gas. The applied high-frequency field couples inductively with the electric fields of the electrons and ions in the plasma, hence the name inductively coupled plasma or ICP. [Pg.395]

As our discussion of scattering proceeds, we shall examine the coupling between the oscillating electrical field of light and the electrons of the scatterer in detail. First, it is useful to consider the interaction of an electric field with matter, as this manifests itself in the dielectric behavior of a substance. This will not only introduce us to the field-matter interaction, but will also provide some relationships which will be useful later. [Pg.666]

Fig. 1. An incident electromagnetic field of intensity, having an associated electric field, U, induces dipole oscillation in the absorbers. The transmitted... Fig. 1. An incident electromagnetic field of intensity, having an associated electric field, U, induces dipole oscillation in the absorbers. The transmitted...
C. H. Townes (Massachusetts Institute of Technology), and N. G. Basov and A. M. Prokhorov (Moscow) fundamental work in the field of quantum electronics, which led to the construction of oscillators and amplifiers based on the maser-laser-principle. [Pg.1302]

Townes s academic life continued. He served as provost of MIT from 1961 to 1966. In 1964, Townes received the Nobel Prize in physics for work in quantum electronics leading to construction of oscillators and amplifiers based on the maser-laser principle. He was named university professor at the University of California-Berkeley in 1967. There he worked for more than 20 years in astrophysics. Ironically, this field is one of many that were transformed by die laser, and Townes often tised lasers in his subsequent research. [Pg.1143]

The induced absorption band at 3 eV does not have any corresponding spectral feature in a(co), indicating that it is most probably due to an even parity state. Such a state would not show up in a(co) since the optical transition IAK - mAg is dipole forbidden. We relate the induced absorption bands to transfer of oscillator strength from the allowed 1AS-+1 (absorption band 1) to the forbidden 1 Ak - mAg transition, caused by the symmetry-breaking external electric field. A similar, smaller band is seen in EA at 3.5 eV, which is attributed to the kAg state. The kAg state has a weaker polarizability than the mAg, related to a weaker coupling to the lower 1 Bu state. [Pg.118]

The electric field of plane-polarized light oscillates in a single plane. It can be prepared hy passing ordinary, unpolarized light through a polarizer, which consists of a material that allows the light to pass only if the electric field is aligned in a certain direction. [Pg.797]


See other pages where Field of oscillating is mentioned: [Pg.212]    [Pg.444]    [Pg.197]    [Pg.188]    [Pg.5]    [Pg.7]    [Pg.205]    [Pg.108]    [Pg.212]    [Pg.444]    [Pg.197]    [Pg.188]    [Pg.5]    [Pg.7]    [Pg.205]    [Pg.108]    [Pg.284]    [Pg.1125]    [Pg.1126]    [Pg.1179]    [Pg.1181]    [Pg.1570]    [Pg.1886]    [Pg.1942]    [Pg.2457]    [Pg.369]    [Pg.370]    [Pg.379]    [Pg.27]    [Pg.140]    [Pg.1]    [Pg.334]    [Pg.444]    [Pg.48]    [Pg.193]    [Pg.156]    [Pg.52]    [Pg.52]    [Pg.139]    [Pg.448]    [Pg.189]    [Pg.128]    [Pg.323]   
See also in sourсe #XX -- [ Pg.147 ]




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