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Magnetic absorber

Time-reversal experiments have been carried out using a magnetic source of Os in iron metal and magnetic absorbers of iridium in iron [75, 76]. A value for 8 = +0-556(10) was obtained during these measurements. [Pg.522]

Figure 8.4. Influence of ihe shape efleci (conical poinis) on the radioelectric performances of a magnetic absorber (loaded polyuurethane elastomer with 25% vol. ex-carbonyl iron... Figure 8.4. Influence of ihe shape efleci (conical poinis) on the radioelectric performances of a magnetic absorber (loaded polyuurethane elastomer with 25% vol. ex-carbonyl iron...
When the applied magnetic field is swept to bring the sample into resonance, MW power is absorbed by the sample. This changes the matching of the cavity to the waveguide and some power is now reflected and passes via the circulator to the detector. This reflected radiation is thus the EPR signal. [Pg.1561]

In absorption spectroscopy a beam of electromagnetic radiation passes through a sample. Much of the radiation is transmitted without a loss in intensity. At selected frequencies, however, the radiation s intensity is attenuated. This process of attenuation is called absorption. Two general requirements must be met if an analyte is to absorb electromagnetic radiation. The first requirement is that there must be a mechanism by which the radiation s electric field or magnetic field interacts with the analyte. For ultraviolet and visible radiation, this interaction involves the electronic energy of valence electrons. A chemical bond s vibrational energy is altered by the absorbance of infrared radiation. A more detailed treatment of this interaction, and its importance in deter-... [Pg.380]

If energy of the proper frequency is supplied, a transition between these quantum states occurs with the absorption of an amount of energy equal to the separation of the states. The frequency of the absorbed radiation lies in the radio-frequency range and depends on the local magnetic field at the atom in question. [Pg.463]

In practice, NMR spectrometers vary the magnetic field strength and measure the value at which a constant radio frequency is absorbed. [Pg.463]

Nuclear magnetic resonance (nmr) requires an atomic nuclei that can absorb a radio-frequency signal impinging it in a strong magnetic field to give a spectmm. The field strength at which the nucleus absorbs is a function of both the nucleus and its immediate electronic environment. The atoms normally used for nmr analysis are as follows (34) H, F, P, Si, and Of these, the most commonly used in polymer analyses are... [Pg.148]

Nuclear Magnetic Resonance. The nmr spectmm of aromatic amines shows resonance attributable to the N—H protons and the protons of any A/-alkyl substituents that are present. The N—H protons usually absorb in the 5 3.6—4.7 range. The position of the resonance peak varies with the concentration of the amine and the nature of the solvent employed. In aromatic amines, the resonance associated with N—CH protons occurs near 5 3.0, somewhat further downfield than those in the aliphatic amines. [Pg.232]

Composition The law of mass aclion is expressed as a rate in terms of chemical compositions of the participants, so ultimately the variation of composition with time must be found. The composition is determined in terms of a property that is measured by some instrument and cahbrated in terms of composition. Among the measures that have been used are titration, pressure, refractive index, density, chromatography, spectrometry, polarimetry, conduclimetry, absorbance, and magnetic resonance. In some cases the composition may vary linearly with the observed property, but in every case a calibration is needed. Before kinetic analysis is undertaken, the data are converted to composition as a function of time (C, t), or to composition and temperature as functions of time (C, T, t). In a steady CSTR the rate is observed as a function of residence time. [Pg.707]

These are meant for parallel connections to absorb the reactive power (capacitive current) of the. system and are generally used on transmission and large distribution networks, as shown in Figure 27.8. They may have a fixed or variable reactance, rated continuously, and any of the magnetic characteristics as illustrated in Figure 27.2. Broadly speaking, they can perform the following functions ... [Pg.850]

Debris with particularly good absorbent qualities such as wood, some paper products, paper, cloth materials, etc., are go candidates for shredding so that they can be included in the remediation process. Materials that are not porous and are not adsorbent are glass, plastic, metal objects, some types of construction debris, tanks, etc., are good candidates for manual or magnetic separation. [Pg.171]

A scram causes the control rods to drop into the core, absorb neutrons and stop the chain reaction. Some rods perform both controlling and scram functions. The control rods are raised to increase the neutron flux (and power) or lowered to reduce it by magnetic jacks (W and CE) or a magnetic "clamshell" screw (B W). The chemical volume and control system (CVCS - not siiown) controls the water quality, removes radioactivity, and varies the reactivity by controUing the amount of a boron compound that is dissolved in the water - called a "poison." Thus, a PWR coiiirols reactivity two ways by the amount of poison in the water and by moving the control rods. [Pg.208]

Figure 4-6 illustrates the relaxational eontribution to the motion. Figure 4-6A shows moment vectors for a spin system in the absenee of the rf field (Hi = 0) the magnetization eomponents are = Mq, = 0, My = 0, beeause in the xy plane the magnetization eomponents caneel. In the presenee of the rf field at the resonanee frequency the spin system absorbs energy, increasing the angle between Ho and M and perturbing the thermal equilibrium so that and My components are induced and M < Mo (Fig. 4-6B). With the passage of time (comparable to the relaxation times Tj and Tj), relaxation back to the equilibrium configuration takes place, so M. increases toward Mo, whereas nd My decrease toward zero as a consequence of the gradual loss of coherence of the moment vectors. Figure 4-6 illustrates the relaxational eontribution to the motion. Figure 4-6A shows moment vectors for a spin system in the absenee of the rf field (Hi = 0) the magnetization eomponents are = Mq, = 0, My = 0, beeause in the xy plane the magnetization eomponents caneel. In the presenee of the rf field at the resonanee frequency the spin system absorbs energy, increasing the angle between Ho and M and perturbing the thermal equilibrium so that and My components are induced and M < Mo (Fig. 4-6B). With the passage of time (comparable to the relaxation times Tj and Tj), relaxation back to the equilibrium configuration takes place, so M. increases toward Mo, whereas nd My decrease toward zero as a consequence of the gradual loss of coherence of the moment vectors.

See other pages where Magnetic absorber is mentioned: [Pg.185]    [Pg.185]    [Pg.391]    [Pg.810]    [Pg.1552]    [Pg.1879]    [Pg.1880]    [Pg.60]    [Pg.186]    [Pg.207]    [Pg.320]    [Pg.53]    [Pg.179]    [Pg.337]    [Pg.460]    [Pg.75]    [Pg.321]    [Pg.202]    [Pg.2484]    [Pg.223]    [Pg.724]    [Pg.237]    [Pg.238]    [Pg.227]    [Pg.228]    [Pg.667]    [Pg.147]    [Pg.289]    [Pg.521]    [Pg.155]    [Pg.155]    [Pg.156]    [Pg.159]    [Pg.164]    [Pg.165]    [Pg.170]    [Pg.956]    [Pg.463]   


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Optically detected magnetic resonance absorbance

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