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Microwave radiation cavity absorption

The setup for ESR spectroscopy is a cross between NMR and micro-wave techniques (Section 5.8). The source is a frequency-stabilized klystron, whose frequency is measured as in microwave spectroscopy. The microwave radiation is transmitted down a waveguide to a resonant cavity (a hollow metal enclosure), which contains the sample. The cavity is between the poles of an electromagnet, whose field is varied until resonance is achieved. Absorption of microwave power at resonance is observed using the same kind of crystal detector as in microwave spectroscopy. Sensitivity is enhanced, as in microwave spectroscopy, by the use of modulation The magnetic field applied to the sample is modulated at, say, 100 kHz, thus producing a 100-kHz signal at the crystal when an absorption is reached. The spectrum is recorded on chart paper. [Pg.189]

For example the efficiency of microwave absorption (i.e., amount of the microwave energy absorbed by a solution compared to the entire microwave energy emitted to the reactor cavity) was measured for n-hexane/2-propanol mixtures (Table 2.1). While pure n-hexane absorbs only little microwave energy, a mixture of 90 wt.-% n-hexane and 10 wt.-% 2-propanol clearly show a significant effect. Moreover, a mixture of 80 wt.-% n-hexane and 20 wt.-% 2-propanol already absorbs microwave radiation with an efficiency that is comparable of that of pure 2-propanol. As additional increase of the amount of 2-propanol does not lead to any further increase of efficiency [37]. [Pg.19]

Microwave-based meters have also been used to monitor water content in emulsions (39). Microwave techniques can be used in two ways Either the attenuation of the microwave radiation due to absorption by the water phase is measured, or capacitance or resonance changes in a microwave cavity are noted. The capacitance-change method is much more sensitive, although both, like the gamma-ray absorption method, are limited in that solids content must be constant or zero in order to accurately interpret the information obtained. Both of these techniques are applicable to field situations and on-line monitoring. [Pg.88]

The a.c. conductivity may be determined from the absorption coefficient for microwaves, or from the alternation in the resonance response of a tuned circuit either in the megacycle region (tank circuit) or in the microwave region (resonant cavity). The attenuation (j8) (in dB cm ) of microwave radiation of frequency co by a flame containing... [Pg.187]

In this chapter, we describe the technique of Fourier transform microwave spectroscopy. We distinguish here two rather different types of sample absorption cells which require somewhat different theoretical descriptions. First, we describe the theory for the relatively broad-band waveguide absorption cell in which the radiation is described as a traveling wave. Second, we describe the narrow-band Fabry-Perot cavity absorption cell in which the radiation is described as a standing wave. [Pg.207]

Without a thermal radiation field in the resonantly tuned cavity, the populations N n,T) and N(n — I, T) of the Rydberg levels should be a periodic function of the transit time T = djv, with a period Tr that corresponds to the Rabi oscillation period. The incoherent thermal radiation field causes induced emission and absorption with statistically distributed phases. This leads to a damping of the Rabi oscillation (Fig. 9.75b). This effect can be proved experimentally if the atoms pass a velocity selector before they enter the resonator, which allows a continuous variation of the velocity and therefore of the transit time T = d/v. n Fig. 9.76 the schematic drawing of the experimental setup with microwave resonator, atom source and detector is shown. [Pg.556]

Rotational transitions correspond to photon wavelengths in the microwave region. The radiation sources in microwave spectrometers are klystron tubes, which were originally developed for radar apparatuses in World War II. Hollow metal wave guides carry the radiation to the sample cell, which is a hollow metal cavity, and the resonant radiation in the cavity is sampled to detect absorption. Microwave spectroscopy has played an important role in identifying molecules in interstellar space, but it is not a common tool in many chemical laboratories. [Pg.962]


See other pages where Microwave radiation cavity absorption is mentioned: [Pg.402]    [Pg.193]    [Pg.194]    [Pg.115]    [Pg.193]    [Pg.581]    [Pg.431]    [Pg.581]    [Pg.914]    [Pg.456]    [Pg.65]    [Pg.1012]    [Pg.87]    [Pg.459]    [Pg.195]    [Pg.623]    [Pg.124]    [Pg.479]    [Pg.915]    [Pg.1216]    [Pg.171]    [Pg.121]    [Pg.320]   
See also in sourсe #XX -- [ Pg.303 , Pg.304 ]




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