Nuclear Overhauser enhancement difference measurements

In this section, I review the work on nuclear multi-spin relaxation phenomena - the work where one of the involved spins belongs to electron will be covered in section 2.7. We begin with the cross-relaxation (nuclear Overhauser enhancement, NOE) measurements and continue with experiments designed for saturation transfer difference (STD) measurements. Next, we turn to investigations of more complicated multispin relaxation phenomena such as cross-correlated relaxation. Finally, papers devoted to relaxation-optimized methods and to large spin systems are also included in this section. 

Nuclear Overhauser enhancement (NOE) spectroscopy has been used to measure the through-space interaction between protons at and the protons associated with the substituents at N (20). The method is also useful for distinguishing between isomers with different groups at and C. Reference 21 contains the chemical shifts and coupling constants of a considerable number of pyrazoles with substituents at N and C. NOE difference spectroscopy ( H) has been employed to differentiate between the two regioisomers [153076 5-0] (14) and [153076 6-1] (15) (22). N-nmr spectroscopy also has some utility in the field of pyrazoles and derivatives. 

The 50.31 MHz 13C NMR spectra of the chlorinated alkanes were recorded on a Varian XL-200 NMR spectrometer. The temperature for all measurements was 50 ° C. It was necessary to record 10 scans at each sampling point as the reduction proceeded. A delay of 30 s was employed between each scan. In order to verify the quantitative nature of the NMR data, carbon-13 Tj data were recorded for all materials using the standard 1800 - r -90 ° inversion-recovery sequence. Relaxation data were obtained on (n-Bu)3SnH, (n-Bu)3SnCl, DCP, TCH, pentane, and heptane under the same solvent and temperature conditions used in the reduction experiments. In addition, relaxation measurements were carried out on partially reduced (70%) samples of DCP and TCH in order to obtain T data on 2-chloropentane, 2,4-dichloroheptane, 2,6-dichloroheptane, 4-chloroheptane, and 2-chloroheptane. The results of these measurements are presented in Table II. In the NMR analysis of the chloroalkane reductions, we measured the intensity of carbon nuclei with T values such that a delay time of 30 s represents at least 3 Tj. The only exception to this is heptane where the shortest T[ is 12.3 s (delay = 2.5 ). However, the error generated would be less than 10%, and, in addition, heptane concentration can also be obtained by product difference measurements in the TCH reduction. Measurements of the nuclear Overhauser enhancement (NOE) for carbon nuclei in the model compounds indicate uniform and full enhancements for those nuclei used in the quantitative measurements. Table II also contains the chemical... 

Little difference was noted when peak heights were used. The error in the T data is less than + 10%. Nuclear Overhauser enhancement factors (q) were obtained by measuring the integrated intensity of peaks in a difference spectrum from one with enhancement minus one with no enhancement and dividing that value by the integral from the one with no enhancement i.e. n ( nOe no nOe / (I nOe" Accuracy should be 10% or better. Linewidtns were measured at half heights, and chemical shifts are relative to TMS. 

Notably, two isomeric products can be generated. The usual infrared (IR) and mass spectra as well as H and 13C NMR chemical shifts could not define which isomer was formed. The authors used different NMR techniques, such as 2-D heteronuclear multiple bond correlation (HMBC) experiments and phase-sensitive nuclear overhauser enhancement spectroscopy (NOESY) measurements to elucidate the product s structure. 

NMR observations basically contain spin relaxation processes which are associated with molecular motions with different specific frequencies in a given system. For quantitative measurements to determine the compositions of the system or selective measurements of particular components with different relaxation parameters, it is essential, therefore, to understand the principle of the relaxation mechanism. When our interest is focused on molecular motions, spin relaxation parameters such as spin-lattice relaxation time T, spin-spin relaxation time T2, and the nuclear Overhauser enhancement (NOE), are directly measured as a function of temperature or field frequency by using appropriate pulse sequences. Such temperature or frequency dependencies of the spin relaxation parameters are analyzed in terms of appropriate models to obtain detailed information of molecular motions with frequencies of Hz in the system. In this chapter, the basic theories and analyses... 

Commonly 1/7,°° is easily evaluated through the measurement of the nuclear Overhauser enhancement when the two H nuclei resonate at different frequencies. [16]... 

IT was calculated for different temperatures. The nuclear Overhauser enhancement factors T were set as independent of temperature, which was confirmed by our results. Table 2 lists measured and calculated relaxation times and rates for the silane mixture mentioned above. 

Such pulse programs are also used to enable other special ID experiments such as saturation or nonexcitation of a large solvent resonance (these are different in that the former method will also saturate NH or OH protons in the molecules under study through the mechanism of chemical exchange), or the measurement of nuclear Overhauser enhancement effects... 

Such pulse programs are also used to enable other special one-dimensional experiments such as saturation or nonexcitation of a large solvent resonance (these are different in that the former method will also saturate NH or OH protons in the molecules under study through the mechanism of chemical exchange), or the measurement of nuclear Overhauser enhancement (NOE) effects which are often used to provide distinction between isomeric structures or to provide estimates of internuclear distances. Pulse programs are also used for measuring NMR spectra of nuclei other than and sometimes in order to probe connectivity between protons and the heteronucleus. In this case, pulses or irradiation can be applied on both the heteronucleus and channels in the same experiment. The commonest use is in NMR where all spin-spin couplings between the nuclei and nuclei are removed by... 

Nuclear Overhauser enhancements are not just an experimental curiosity. They are independent relaxation parameters which can be used to investigate molecular motions in detail. Also, the technique of measuring specific H- H Overhauser enhancements by NOE difference spectroscopy detects spatial rather than chemical proximity and hence adds a powerful new tool to conformational and structural analysis. 

Nuclear Overhauser effect (NOE) difference measurements were used to assign structure 79 for the product of reaction of diphenylnitrile imine with 5-ethylsulfonyl-2-methyl(27/)pyridazinone. Thus in the H NMR spectrum the ot/, o-protons of the arylhydrazino moiety (which were identified by two-dimensional heteronuclear multiple quantum correlation (2-D HMQC) spectroscopy) were shown in differential NOE (DNOE) experiment to be significantly enhanced on irradiation of pyridazine hydrogen H-7, proving their steric proximity <2000JST13>. 

A conformational comparative study has been performed on a penem, a carbapenem, and a 1/3-methylcarbapenem, bearing the same C-2 and C-6 side chains, using both NMR and theoretical tools. The corresponding calculations have been performed at the 3-21G level using the ab initio MO method, while 111 NMR measurements and nuclear Overhauser effect (NOE) enhancements were carried out in DzO solution. It arose from this study that there are conformational differences in the side chains of these three compounds in the physiological environment in particular, the conformation of the C-6 side chain in the penem appears to be different from that in the carbapenem <1998BMC367>. 

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