Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Estimation magnetic parameters

Ferromagnetic-Paranugnetic Transition The Estimation of Magnetic Parameters... [Pg.11]

The low-atomic-character state (85MA) can be interpreted (19) in terms of the loose ion-pair picture (Fig. 6), or alternatively, as a large-radius monomeric state [af, estimated (17) to be in the region 10-15 A], Experimental magnetic parameters and unpaired electron spin densities at the metal nucleus for the MA species are shown in Table II. [Pg.164]

One of the most characteristic properties of crosslinked rubbers is the ability to swell in appropriate solvents to a constant volume. Not only is this property exploited for estimation of parameters such as crosslink densities and polymer-solvent interaction parameters, but the resultant change in nuclear magnetic resonance (NMR) parameters allows a large number of new and interesting NMR experiments. It is the aim of this chapter to introduce some simple concepts of polymer swelling and to examine the information obtainable for the range of NMR experiments possible on swollen gels. [Pg.491]

Schematically, a suitable computational method should thus meet two requirements first, it should provide reliable estimates of the structural and magnetic parameters of open shell systems, and, second, it should take into account the influence of the environment on the magnetic properties of these systems. Schematically, a suitable computational method should thus meet two requirements first, it should provide reliable estimates of the structural and magnetic parameters of open shell systems, and, second, it should take into account the influence of the environment on the magnetic properties of these systems.
Electron Spin Echo Envelope Modulation (ESEEM) and pulse Electron Nuclear Double Resonance (ENDOR) experiments are considered to be two cornerstones of pulse EPR spectroscopy. These techniques are typically used to obtain the static spin Hamiltonian parameters of powders, frozen solutions, and single crystals. The development of new methods based on these two effects is mainly driven by the need for higher resolution, and therefore, a more accurate estimation of the magnetic parameters. In this chapter, we describe the inner workings of ESEEM and pulse ENDOR experiments as well as the latest developments aimed at resolution and sensitivity enhancement. The advantages and limitations of these techniques are demonstrated through examples found in the literature, with an emphasis on systems of biological relevance. [Pg.13]

The main shortcoming of the two-pulse experiment is that the primary echo decays within the phase memory time, 7m, which is often very short. This can prevent the observation of low-frequency modulations, and thus the estimation of the magnetic parameters can become uncertain. Another important limitation arises from the spectrometer deadtime u (typically 100-150 ns at X-band frequencies), which restricts the observation of the signal to times t > ti. The loss of the initial part of the time trace can cause severe distortions in the frequency-domain spectrum, especially in disordered systems where destructive interference from differ-... [Pg.23]

Figure 8 Isotropic magnetic parameter gis and Aisofor TEMPO in a series of protic and aprotic solvents and their mixtures 1, water 2, water/ethanol solution (7 3, v/v) 3, water/ethanol solution (3 7, v/v) 4, methanol 5, ethanol 6, isopropanol 1, acetone 8, olive oil/ethanol solution (9 1, w/w) 9, acetonitrile 10, olive oil 11, toluene 12, hexane. The isotropic g-factor of TEMPO in water was taken as a reference point i.e. Agiso = 0). The estimated errors are within the size of the symbols. Magnetic parameters for TEMPO partitioned in the lipid phase of the DPPC bilayer are shown as filled sguares. Parameters corresponding to the membrane in the gel phase (before the main phase transition) are marked as A and above the phase transition piso at ca. 45 °C) are marked as B. Parameters for two components of TEMPO in non-agueous phase of DPPC bilayer interdigitated by 1.2 M ethanol are marked as C and D... Figure 8 Isotropic magnetic parameter gis and Aisofor TEMPO in a series of protic and aprotic solvents and their mixtures 1, water 2, water/ethanol solution (7 3, v/v) 3, water/ethanol solution (3 7, v/v) 4, methanol 5, ethanol 6, isopropanol 1, acetone 8, olive oil/ethanol solution (9 1, w/w) 9, acetonitrile 10, olive oil 11, toluene 12, hexane. The isotropic g-factor of TEMPO in water was taken as a reference point i.e. Agiso = 0). The estimated errors are within the size of the symbols. Magnetic parameters for TEMPO partitioned in the lipid phase of the DPPC bilayer are shown as filled sguares. Parameters corresponding to the membrane in the gel phase (before the main phase transition) are marked as A and above the phase transition piso at ca. 45 °C) are marked as B. Parameters for two components of TEMPO in non-agueous phase of DPPC bilayer interdigitated by 1.2 M ethanol are marked as C and D...
Canne and co-workers have presented EPR studies of three prokaryotic enzymes of the xanthine oxidase family, namely quinoline 2-oxidoreductase, quinaldine 4-oxidase, and isoquinoline l-oxidoreductaseJ In quinoline 2-oxidoreductase a neutral flavin radical was observed, while in quinaldine 4-oxidase an anionic radical was detected. The rapid Mo(V) signal was observed in all three enzymes with only small differences in magnetic parameters. From spectra simulations of Mo (/ = 5/2) substituted quinoline 2-oxidoreductase, a deviation of 25° between the maximal g and Mo-hfc tensor component was derived. The Mo(V) species was detected in small amounts upon reduction with substrates in quinoline 2-oxidoreductase and quinaldine 4-oxidase, but showed a different kinetic behaviour with an intense EPR signal in isoquinoline 1-oxidoreductase. The two [2Fe-2S] clusters produced different EPR signals in all three enzymes and, in isoquinoline 1-oxidoreductase, revealed a dipolar interaction, from which a maximum distance of 15 A was estimated. [Pg.247]

One of the recent advances in magnetic studies is that it enables not only the estimation of the average volume v of clusters from the LF and HF approximations of the Langevln function, but also enables to compute particle size distribution based on an assumed function. By judiciously combining the parameters of the Langevln and of the "log normal function, we obtained a particle (cluster) size distribution of Y Fe203 in ZSM-5. The essential features of such computation are shown in Fig. 6. [Pg.507]

To illustrate the utility of the MWBD method, a series of commercial polyvinyl acetates and low density polyethylenes are analyzed. Either kinetic models or 13c nuclear magnetic resonance results are used to estimate the branching structural parameter. [Pg.147]

In view of the central role that a magnetisation density plays for magnetic neutron scattering, it is useful to define a parameter for each reflection, called a canting angle, which gives a quantitative estimate of the deviation from the collinear approximation. The idea is as follows. [Pg.260]


See other pages where Estimation magnetic parameters is mentioned: [Pg.148]    [Pg.261]    [Pg.165]    [Pg.64]    [Pg.165]    [Pg.90]    [Pg.56]    [Pg.312]    [Pg.456]    [Pg.185]    [Pg.209]    [Pg.116]    [Pg.48]    [Pg.48]    [Pg.56]    [Pg.329]    [Pg.1486]    [Pg.2109]    [Pg.30]    [Pg.101]    [Pg.262]    [Pg.53]    [Pg.35]    [Pg.435]    [Pg.572]    [Pg.204]    [Pg.231]    [Pg.148]    [Pg.95]    [Pg.58]    [Pg.78]    [Pg.113]    [Pg.19]    [Pg.29]    [Pg.125]    [Pg.135]    [Pg.139]   
See also in sourсe #XX -- [ Pg.244 , Pg.246 ]




SEARCH



Magnetism parameters

Parameter estimation

© 2024 chempedia.info