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First derivative EPR spectrum

A spectroscopically demonstrated molecular property of SOM relating to the degree of humification is the SFR concentration, as measured by EPR (Riffaldi and Schnitzer, 1972 Schnitzer and Levesque, 1979 Martin-Neto et al., 1991 Senesi et al., 1996 Jerzykiewicz et al., 1999 Watanabe et al., 2005). The content of paramagnetic species is proportional to the EPR spectrum area that can be obtained by double integration of the first derivative EPR spectrum, which is normally detected. An approximation commonly used to obtain the relative area of free radicals is the... [Pg.657]

Figure 5.7 First-derivative EPR spectrum obtained after y-irradiation at 77 Kof 1.75 mol% heptane in CCfF ... Figure 5.7 First-derivative EPR spectrum obtained after y-irradiation at 77 Kof 1.75 mol% heptane in CCfF ...
Figure 4, First derivative EPR spectrum of Zn(II)-doped Cuf(FAA)j en compared with that of the purple isomer Cu... Figure 4, First derivative EPR spectrum of Zn(II)-doped Cuf(FAA)j en compared with that of the purple isomer Cu...
Fig. 33 Time-sweep first derivative EPR spectrum of TTF+" recorded at constant magnetic induction using liquid liquid electrochemical EPR cell. The organic phase (DCE) contained 5 mM TTF,... Fig. 33 Time-sweep first derivative EPR spectrum of TTF+" recorded at constant magnetic induction using liquid liquid electrochemical EPR cell. The organic phase (DCE) contained 5 mM TTF,...
Fig. 12. (A) First-derivative EPR spectra of complex I treated with NADH or NADPH. Conditions complex I, 46 mg/ml temperature 14°K microwave frequency 9.225 GHz power, 2 mW, modulation amplitude, 6.3 G gain, 50. g — 2 was at 3295 G. Where indicated IJS mAf NADH or NADPH was added. Small letters of the alphabet in this, (B), (C), and Fig. 13 denote the same signals as in Fig. 4. (B) The EPR spectrum of NADH-treated complex I shown in (A) at gain of 200 and 03 mW power. (C) The EPR spectrum of NADPH-treated complex I shown in (A) at gain of 200 and 03 mW power. From Hatefi and Hanstein (80). Fig. 12. (A) First-derivative EPR spectra of complex I treated with NADH or NADPH. Conditions complex I, 46 mg/ml temperature 14°K microwave frequency 9.225 GHz power, 2 mW, modulation amplitude, 6.3 G gain, 50. g — 2 was at 3295 G. Where indicated IJS mAf NADH or NADPH was added. Small letters of the alphabet in this, (B), (C), and Fig. 13 denote the same signals as in Fig. 4. (B) The EPR spectrum of NADH-treated complex I shown in (A) at gain of 200 and 03 mW power. (C) The EPR spectrum of NADPH-treated complex I shown in (A) at gain of 200 and 03 mW power. From Hatefi and Hanstein (80).
Figure Bl.15.6. The EPR spectrum of tire perinaphthenyl radical in mineral oil taken at room temperature. (A) First derivative of the EPR absorption x with respect to the external magnetic field, Bq. (B) Integrated EPR spectrum. Figure Bl.15.6. The EPR spectrum of tire perinaphthenyl radical in mineral oil taken at room temperature. (A) First derivative of the EPR absorption x with respect to the external magnetic field, Bq. (B) Integrated EPR spectrum.
The characteristic derivative-shaped feature at g 1.94 first observed in mitochondrial membranes has long been considered as the sole EPR fingerprint of iron-sulfur centers. The EPR spectrum exhibited by [4Fe-4S] centers generally reflects a ground state with S = I and is characterized by g values and a spectral shape similar to those displayed by [2Fe-2S] centers (Fig. 6c). Proteins containing [4Fe-4S] centers, which are sometimes called HIPIP, essentially act as electron carriers in the photoinduced cyclic electron transfer of purple bacteria (106), although they have also been discovered in nonphotosynthetic bacteria (107). Their EPR spectrum exhibits an axial shape that varies little from one protein to another with g// 2.11-2.14 and gi 2.03-2.04 (106-108), plus extra features indicative of some heterogeneous characteristics (Pig. 6d). [Pg.443]

For maximum ENDOR enhancement, the Zeeman modulation amplitude has to be about one half of the width of the EPR line which is saturated at an extremum of its first derivative. However, in an EPR spectrum with line widths of typically 1 mT this Zeeman modulation contributes 20 kHz to the width of a proton ENDOR line. It turns out that in many cases a remarkably better resolution of the spectra may be obtained with a single coding in which only the rf field is modulated. [Pg.7]

The second thing that EPR can tell us is concentration. As with all forms of spectroscopy, the intensity of an EPR absorption peak is proportional to the concentration of the analyte giving rise to this absorption. (Care - because we record an EPR spectrum as a first derivative, the concentration of analyte is in fact proportional to the integral of the EPR peak height.) However, EPR is so powerful a technique that to determine a concentration alone would be wasteful. [Pg.250]

Next, we pass analyte through the EPR cell at a constant flow rate, V/, and determine the intensity of the EPR signal, S. (Remember that the EPR spectrum is in fact a first derivative, so the concentration of the radical that is generated is proportional to the integral of the peak.) We then vary the flow rate V/ and monitor the corresponding peak intensities. [Pg.252]

Electron spin relaxation in aqueous solutions of Gd3+ chelates is too rapid to be observed at room temperature by the usual pulsed EPR methods, and must be studied by continuous wave (cw) techniques. Two EPR approaches have been used to study relaxation studies of the line shape of the cw EPR resonance of Gd3+ compounds in aqueous solution, and more direct measurement of Tle making use of Longitudinally Detected EPR (LODEPR) [70]. Currently, LODESR is available only at X-band, and the frequency dependence of relaxation is studied by following the frequency dependence of the cw EPR line shape, and especially of the peak-to-peak line width of the first derivative spectrum (ABpp). [Pg.221]

With the use of lock-in detection, the measured EPR signal corresponds to the first derivative of the radical absorption spectrum. The 1st integral of a measured EPR spectrum as a function of the magnetic field is computed according to... [Pg.316]

Derivative Detection of EPR Transition. The EPR spectrum is usually displayed as the first derivative of the absorption y"(H), because the nonresonant low-frequency and low-amplitude RF modulation (co1/ 2% = typically 100 kHz) applied to the coils near the magnet is detected by a rectifier in addition to the drop in microwave power level due to the RF resonant absorption (typically co0/27c = 9.1 GHz if H0 = 0.34T) The signal is processed by a phase-sensitive circuit, which detects a back-and-forth sweep across resonance in small magnetic field increments (relative to the DC field and to the width of the measured spectrum), thus generating a response df /dH (see Fig. 11.60). [Pg.724]

Most X-band EPR spectra of transition metals are recorded at low temperatures (4-lOOK) using high-purity quartz tubes (no paramagnetic impurities) with a sample volume of about 300 pL. The minimum concentration of the sample depends on the broadness of its spectrum. Because EPR spectra are recorded as a first derivative (see subsequent text), the relationship between concentration, signal amplitude and spectral linewidth can be approximated as... [Pg.6479]

One of the first things one notices about an EPR spectrum is that it is a first-derivative spectrum rather than the more typical absorption presentation. This is due to an instrumental artifact. To enhance the sensitivity of the EPR spectrometer, the magnetic field is modulated. To obtain field modulation, a small set of Helmholtz coils are place about the sample in line with the external field. These coils allow the amplitude of the external field, to change by a small amount ( 0.01 20G) at a frequency of 100 kHz (smaller frequencies can also be used, but are less sensitive). Because the spectrometer is tuned to only detect signals that change amplitude with field changes at... [Pg.6479]

Figure 1 Experimental and simulated EPR spectra of oxidized CooA at pH 7.4. Experimental conditions temperature, 2 K microwave frequency, 35.106GHz microwave power, 20p,W 100 kHz field modulation amplitude, 0.4 mT time constant, 128 ms scan time, 4 min. Lower traces, in absorption line-shape (due to rapid-passage conditions), are the experimental spectrum (blue) and a digital integration of the simulated spectrum (red). Upper traces in first-derivative lineshape are a digital derivative of the experimental spectrum (blue) and the simulated spectrum (red). Simulation parameters component (a) g = [2.60, 2.268, 1.85], (b) g = [2.47, 2.268, 1.90] Gaussian single-crystal linewidths (half-width at half-maximum) W = [500, 200, 400] MHz. Simulated spectra for (a) and (b) are added in the ratio 2 1 to give the summed spectrum shown... Figure 1 Experimental and simulated EPR spectra of oxidized CooA at pH 7.4. Experimental conditions temperature, 2 K microwave frequency, 35.106GHz microwave power, 20p,W 100 kHz field modulation amplitude, 0.4 mT time constant, 128 ms scan time, 4 min. Lower traces, in absorption line-shape (due to rapid-passage conditions), are the experimental spectrum (blue) and a digital integration of the simulated spectrum (red). Upper traces in first-derivative lineshape are a digital derivative of the experimental spectrum (blue) and the simulated spectrum (red). Simulation parameters component (a) g = [2.60, 2.268, 1.85], (b) g = [2.47, 2.268, 1.90] Gaussian single-crystal linewidths (half-width at half-maximum) W = [500, 200, 400] MHz. Simulated spectra for (a) and (b) are added in the ratio 2 1 to give the summed spectrum shown...
The intensity of the signal must be obtained in the absence of any power saturation. Since the EPR signal consists of a first derivative, rather than an absorbance, this must also be factored into the analysis. Usually double integration of the spectrum is performed over a defined scan range (after careful adjustment to the baseline). Alternatively, for a single symmetric first derivative line, the following simple relation may be used ... [Pg.24]

Figure 2 Acquisition of an EPR spectrum for an unpaired 5=1/2 electron, a) Energy-level diagram as a function of magnetic field, b) absorption/emission of microwave energy because of the field of resonance, and c) first derivative of the energy absorption profile, for example, an EPR spectrum. Figure 2 Acquisition of an EPR spectrum for an unpaired 5=1/2 electron, a) Energy-level diagram as a function of magnetic field, b) absorption/emission of microwave energy because of the field of resonance, and c) first derivative of the energy absorption profile, for example, an EPR spectrum.

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