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Kinetic energy degradation

Magnetic sector mass spectrometers accelerate ions to more than 100 times the kinetic energy of ions analysed in quadrupole and ion trap mass spectrometers. The higher accelerating voltage contributes to the fact that ion source contamination is less likely to result in degraded sensitivity. This is particularly important for analysis that requires stable quantitative accuracy. [Pg.388]

On the other hand, the effective collision concept can explain the Arrhenius term on the basis of the fraction of molecules having sufficient kinetic energy to destroy one or more chemical bonds of the reactant. More accurately, the formation of an activated complex (i.e., of an unstable reaction intermediate that rapidly degrades to products) can be assumed. Theoretical expressions are available to compute the rate of reaction from thermodynamic properties of the activated complex nevertheless, these expression are of no practical use because the detailed structure of the activated complexes is unknown in most cases. Thus, in general the kinetic parameters (rate constants, activation energies, orders of reaction) must be considered as unknown parameters, whose values must be adjusted on the basis of the experimental data. [Pg.13]

Fig. 1.5. Ion image of S+ (a) produced from CS2 in an intense laser field (0.36PW/cm2), recorded with a position-sensitive detector (PSD). The small hole in the central part of the accumulated image is ascribable to the degraded sensitivity of the central part of the detector. The coincidence ion images of S+ (b-d), and the corresponding kinetic energy release distributions (e-f) obtained for the (1,1), (1,1,1) and (1,1,2) Coulomb explosion pathways, respectively... Fig. 1.5. Ion image of S+ (a) produced from CS2 in an intense laser field (0.36PW/cm2), recorded with a position-sensitive detector (PSD). The small hole in the central part of the accumulated image is ascribable to the degraded sensitivity of the central part of the detector. The coincidence ion images of S+ (b-d), and the corresponding kinetic energy release distributions (e-f) obtained for the (1,1), (1,1,1) and (1,1,2) Coulomb explosion pathways, respectively...
Since pulsed laser ionization produces well defined packets of ions and electrons, TOF analysers (which essentially are magnetically shielded, electric-field-free drift tubes with apertures and an electron multiplier) can readily be used. TOF resolution for slow electrons can approach 3 meV, and throughput is similar to that of electrostatic analysers operating without an extraction field (i.e. a detection efficiency < 1%). The kinetic energy is obtained from the flight time, which is proportional to the reciprocal velocity, (KE) /2, whereas the resolution varies as (KE)/2. Thus, the resolution for 1-5 eV electrons is comparable to that for electrostatic analysers, but degrades seriously for 5-10 eY electrons. [Pg.136]

This derivation neglects the correction of kinetic energy loss due to nonuniformity of flow in both cross sections and the frictional degradation of energy during passage through the constriction. This is corrected by the introduction of a numerical coefficient, Cd ... [Pg.3863]


See other pages where Kinetic energy degradation is mentioned: [Pg.366]    [Pg.366]    [Pg.283]    [Pg.420]    [Pg.404]    [Pg.520]    [Pg.307]    [Pg.430]    [Pg.153]    [Pg.27]    [Pg.429]    [Pg.196]    [Pg.95]    [Pg.153]    [Pg.257]    [Pg.404]    [Pg.451]    [Pg.34]    [Pg.240]    [Pg.404]    [Pg.419]    [Pg.420]    [Pg.34]    [Pg.157]    [Pg.6]    [Pg.245]    [Pg.87]    [Pg.88]    [Pg.430]    [Pg.477]    [Pg.478]    [Pg.192]    [Pg.35]    [Pg.138]    [Pg.199]    [Pg.20]    [Pg.165]    [Pg.431]    [Pg.434]    [Pg.477]    [Pg.478]    [Pg.102]    [Pg.370]    [Pg.278]    [Pg.241]   
See also in sourсe #XX -- [ Pg.730 ]




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