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Balance resonator

As mentioned in Sect. 2.1, the stationary concentration of propagating radicals in radical polymerization is too low to be detected by commercially available ESR spectrometers. Hence, it is necessary for ESR measurement of growing radicals in radical polymerization to have a spectrometer which is sensitive to very low concentrations, say, down to at least 10" M. The ESR spectrometer improved by Bresler et al. using a balance resonator permitted evaluation of the rate constants of... [Pg.257]

A few TCRs to balance the reactive power supply. They may generate harmonics, which must be suppressed to avoid any resonance. T.SCs and TCRs are monitored through a feedback control system,... [Pg.805]

Flexible rotor balancing must be performed with the rotor whirl configuration approximating the mode in question. The operating speed(s) is in the vicinity of a major flexible mode resonance (damped critical speed). As these two speeds approach one another, a tighter... [Pg.588]

Assume that oscillatory excitation torque of Tq sin cot is applied to the system in Figure 9-14. By definition, when the excitation frequency coincides with the torsional natural frequency of the model, all torques will balance and the system will be in a state of resonance. [Pg.392]

Both phenanthrene and anthracene have a tendency to undergo addition reactions under the eonditions involved in eertain eleetrophilic substitutions. For example, in the nitration of anthracene in the presence of hydrochloric acid, an intermediate addition product can be isolated. This is a result of the relatively close balance in resonance stabilization to be regained by elimination (giving an anthracene ring) or addition (resulting in two benzenoid rings). [Pg.569]

Longitndinal ont-of-balance forces. For a Z-confignration pipe layont there is a steady force between the two bends generated by the pressnre difference in the gas while the pressnre front moves between the two bends. This gives a longer dnration to the force which can approach the resonant freqnency of the pipe. [Pg.144]

The net effect is, therefore, a balance of these two components. Some of the results of the separation may be surprising, such as the relatively small contribution that resonance makes to the overall substituent effect of p-NOj. Another interesting result is the predominant resonance contribution in the alkyl series this (if real) must be attributed to hyperconjugation. [Pg.327]

Formation of a quinonoid carboline-type anhydro-base requires loss of resonance stabilization of the indole moiety. In the carboline anhydro-bases this is counterbalanced by the preservation of a 677 system in the hetero ring. No such balancing factor is present in the case of 3,4-dihydro-j3-carboline derivatives. Formation of the exocyclic anhydro-base in the latter case preserves benzenoid resonance. It is noteworthy that in the two cases where formation of a carboUne-type anhydro-base was reported in dihydro derivatives additional aromatic conjugation is present. [Pg.193]

If the operator removes the rotor from the balancing shaft without marking the point of bore and shaft contact, it may not be in the same position when reassembled. This often shifts the rotor by several mils as compared to the axis on which it was balanced, thus causing an imbalance to be introduced. The vibrations that result are usually enough to spoil what should have been a precision balance and produce a barely acceptable vibration level. In addition, if the resultant vibration is resonant with some part of the machine or structure, a more serious vibration could result. [Pg.936]

The quartz balance is a tool for detecting the increase (or decrease) of the film mass deposited onto the surface of a quartz resonator, connected to the driving circuit, and registering the shift in a frequency. The dependence is expressed by the Sauerbray equation (Sauerbray 1964) ... [Pg.186]

This favors a sample s contraction V is the volume). This attractive force, which will be temperature dependent, is balanced by the regular temperature-independent elastic energy of the lattice Fsiast/V = K/2) 6V/V). Calculating the equilibrium volume from this balance allows us to estimate the thermal expansion coefficient a. More specifically, the simplest Hamiltonian describing two local resonances that interact off-diagonally is... [Pg.181]

Malik, N.A., Otiko, G. and Sadler, P.J. (1980) Control of intra- and extra-cellular sulfhydryl-disulfide balances with gold phosphine drugs Phosphorus-31 nuclear magnetic resonance studies of human blood. Journal of Inorganic Biochemistry, 12, 317-322. [Pg.315]

Fig. 9.34 Monitoring of inelastic excitations by nuclear resonant scattering. The sidebands of the excitation probability densities for phonon creation, S(E), and for annihilation, S —E), are related by the Boltzmann factor, i.e., S(—E) = S E) tTvp —Elk T). This imbalance, known as detailed balance, is an intrinsic feature of each NIS spectrum and allows the determination of the temperature T at which the spectrum was recorded... Fig. 9.34 Monitoring of inelastic excitations by nuclear resonant scattering. The sidebands of the excitation probability densities for phonon creation, S(E), and for annihilation, S —E), are related by the Boltzmann factor, i.e., S(—E) = S E) tTvp —Elk T). This imbalance, known as detailed balance, is an intrinsic feature of each NIS spectrum and allows the determination of the temperature T at which the spectrum was recorded...
The principle of operation of a quartz balance can be easily described if an AC potential is placed across a quartz piezoelectric crystal, the crystal will oscillate spatially and the amplitude of this oscillation is greatest at the resonance frequency of the crystal. This resonance frequency, /0, is a function of several parameters, including the mass of the crystal, and the mass of foreign material placed on the crystal. In fact, the change in the resonance frequency, A/0, on placing some foreign material on it is given approximately... [Pg.210]

Figure 12. Hydrogen bond involving a Fermi resonance damping parameters switching the intensities. The lineshapes were computed within the adiabatic and exchange approximations. Intensities balancing between two sub-bands are observed when modifying the damping parameters (a) with y0 =0.1, and y5 = 0.8 (b) with ya = ys = 0.8 (c) with yB — 0.8 and ys — 0.1. Common parameters oto = 1, A = 150cm, 2g)5 = 2850cm-1, and T = 30 K. Figure 12. Hydrogen bond involving a Fermi resonance damping parameters switching the intensities. The lineshapes were computed within the adiabatic and exchange approximations. Intensities balancing between two sub-bands are observed when modifying the damping parameters (a) with y0 =0.1, and y5 = 0.8 (b) with ya = ys = 0.8 (c) with yB — 0.8 and ys — 0.1. Common parameters oto = 1, A = 150cm, 2g)5 = 2850cm-1, and T = 30 K.

See other pages where Balance resonator is mentioned: [Pg.247]    [Pg.29]    [Pg.259]    [Pg.109]    [Pg.114]    [Pg.221]    [Pg.444]    [Pg.195]    [Pg.387]    [Pg.34]    [Pg.35]    [Pg.2505]    [Pg.464]    [Pg.838]    [Pg.594]    [Pg.331]    [Pg.312]    [Pg.183]    [Pg.245]    [Pg.90]    [Pg.17]    [Pg.360]    [Pg.312]    [Pg.194]    [Pg.312]    [Pg.383]    [Pg.228]    [Pg.782]    [Pg.386]    [Pg.83]    [Pg.227]    [Pg.31]    [Pg.283]   
See also in sourсe #XX -- [ Pg.257 ]




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