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Magnetic field, and microwaves

Fig. 14.12 Schematic illustration of magnetic field and microwave effects in radical-pair chemistry. Fig. 14.12 Schematic illustration of magnetic field and microwave effects in radical-pair chemistry.
Physical agents in the environment that may cause illness include solar ultraviolet (UV) radiation, ionizing radiation (produced by radioactive materials and X-rays), extreme temperatures, noise, vibrations, and particulates. The most famous particulates inducing adverse health effects include asbestos and silica dust. Other physical agents, such as electric or magnetic fields and microwaves, may also cause adverse health effects, but there is of yet not enough solid evidence to support or refute this hypothesis. [Pg.1013]

Direct measurement of magnetic field and microwave frequency An absolute measurement is possible by simultaneously measuring the microwave frequency and the magnetic field at the centre of the ESR signal using the equation g = 0.0714477 Ve(MHz)/Bo(mT), where Bo is the field at the centre of the signal and v is the microwave frequency. An accurate microwave frequency meter is often standard equipment of commercial instruments, while the calibration of the magnetic field has to be checked by a field meter usually based on NMR. [Pg.91]

Besides the conventional Grimm-type dc source, which has dominated the GD-OES scene for approximately 30 years, other discharge sources are well known. Among those are various boosted sources which use either an additional electrode to achieve a secondary discharge, or a magnetic field or microwave power to enhance the efficiency of excitation, and thus analytical capability none of these sources has, however, yet been applied to surface or depth-profile analysis. [Pg.223]

Other NDE Methods The following methods also have applications magnetic field testing, microwave inspection, thermal inspection, and holography. [Pg.168]

Means to confine the plasma have been ihe major objective of fusion power research in several countries for a number of years. Methods researched lor confining the plasma include the use of strong magnetic fields and inertial confinement methods in which the fuel is pelletized in a special way and fusion reactions are initiated either by laser beams, beams of panicles, and heating the plasma with high power microwave radiation.2 Other means are being researched. [Pg.695]

Microwaves consist of electric and magnetic fields, and they propagate in space. Electric fields are primarily responsible for physical effects on the tissue. The energy distribution and thus the speed of absorbing energy and warming up vary topographically. In... [Pg.102]

Magnetic resonance the absorption of energy that occurs when certain nuclei (e.g., H, 13 C, 31P, 15N), which have a spin state, are placed in a strong magnetic field and simultaneously irradiated with electromagnetic (microwave) radiation. [Pg.524]

In order to obtain a Larmor resonance line we have to vary the frequency of the microwave field and count the number of spin Hips per unit time. In order to avoid saturation effects the microwave field amplitude was kept low. The resonance curve obtained in the described manner is rather asymmetric. The lineshape can be described using the known spatial configuration of the magnetic field and a thermal distribution of the axial energy. A least squares fit to the data points as shown in Fig. 9 leads to a fractional uncertainty of about 10-6 and the g factor can be quoted with the same error [9]. [Pg.212]

Figure 9.26. Left lower rotational levels of SO 3 in zero magnetic field, and the transitions observed (see chapter 10). Right microwave magnetic resonance transitions observed in SO at 8762 MHz [56]. Figure 9.26. Left lower rotational levels of SO 3 in zero magnetic field, and the transitions observed (see chapter 10). Right microwave magnetic resonance transitions observed in SO at 8762 MHz [56].
In the microwave ion beam experiments described in this section, it is important to identify the microwave mode corresponding to the resonance line studied in a magnetic field. For a TM mode the microwave electric field along the central axis of the waveguide is parallel to the static magnetic field. We then put p = 0 in equation (10.161) so that the Zeeman components obey the selection rule AMj = 0. Alternatively in a TE mode the microwave electric field is perpendicular to the static magnetic field and the selection rule is A Mj = 1. This is the case for the Zeeman pattern shown in figure 10.73 each J = 3/2 level splits into four Mj components and the six allowed transitions should,... [Pg.823]


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And microwaves

Microwave field

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