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Chemical shift, and

A simple, non-selective pulse starts the experiment. This rotates the equilibrium z magnetization onto the v axis. Note that neither the equilibrium state nor the effect of the pulse depend on the dynamics or the details of the spin Hamiltonian (chemical shifts and coupling constants). The equilibrium density matrix is proportional to F. After the pulse the density matrix is therefore given by and it will evolve as in equation (B2.4.27). If (B2.4.28) is substituted into (B2.4.30), the NMR signal as a fimction of time t, is given by (B2.4.32). In this equation there is a distinction between the sum of the operators weighted by the equilibrium populations, F, from the unweighted sum, 7. The detector sees each spin (but not each coherence ) equally well. [Pg.2100]

Figure B2.4.5. Simulated lineshapes for an intennolecular exchange reaction in which the bond joining two strongly coupled nuclei breaks and re-fomis at a series of rates, given beside tlie lineshape. In slow exchange, the typical spectrum of an AB spin system is shown. In the limit of fast exchange, the spectrum consists of two lines at tlie two chemical shifts and all the coupling has disappeared. Figure B2.4.5. Simulated lineshapes for an intennolecular exchange reaction in which the bond joining two strongly coupled nuclei breaks and re-fomis at a series of rates, given beside tlie lineshape. In slow exchange, the typical spectrum of an AB spin system is shown. In the limit of fast exchange, the spectrum consists of two lines at tlie two chemical shifts and all the coupling has disappeared.
NMR spectra are basically characterized by the chemical shift and coupling constants of signals. The chemical shift for a particular atom is influenced by the 3D arrangement and bond types of the chemical environment of the atom and by its hybridization. The multiplicity of a signal depends on the coupling partners and on the bond types between atom and couphng partner. [Pg.518]

Inc, [34], is an example of a software package that can calculate 3D geometries, chemical shifts, and coupling constants using semi-empirical approaches (Figure 10.2-2). [Pg.521]

Figure 10.2-2. Calculatiorr of H NMR chemical shifts and coupling constants arrd simulation of the spectrum with HyperChem 7. Figure 10.2-2. Calculatiorr of H NMR chemical shifts and coupling constants arrd simulation of the spectrum with HyperChem 7.
A useful empirical method for the prediction of chemical shifts and coupling constants relies on the information contained in databases of structures with the corresponding NMR data. Large databases with hundred-thousands of chemical shifts are commercially available and are linked to predictive systems, which basically rely on database searching [35], Protons are internally represented by their structural environments, usually their HOSE codes [9]. When a query structure is submitted, a search is performed to find the protons belonging to similar (overlapping) substructures. These are the protons with the same HOSE codes as the protons in the query molecule. The prediction of the chemical shift is calculated as the average chemical shift of the retrieved protons. [Pg.522]

Commercial implementations of this general approach are ACD/I-Lab [36], Specinfo (Chemical Concepts) [37], WINNMR (Bruker), and KnowItAll (Bio-Rad) [38]. Figure 10.2-3 shows the workspace generated by ACD/I-Lab after predicting a H NMR spectrum. ACD calculations are currently based on over 1 200 000 experimental chemical shifts and 320 000 experimental coupling constants [36]. [Pg.522]

Ah initio methods are applicable to the widest variety of property calculations. Many typical organic molecules can now be modeled with ah initio methods, such as Flartree-Fock, density functional theory, and Moller Plesset perturbation theory. Organic molecule calculations are made easier by the fact that most organic molecules have singlet spin ground states. Organics are the systems for which sophisticated properties, such as NMR chemical shifts and nonlinear optical properties, can be calculated most accurately. [Pg.284]

Katritzky and Topsom have reviewed the information available, largely from infrared and n.m.r. studies, concerning the distortion of the tt-electron system in the benzene ring brought about in the ground state by substituents. Of particular interest is the observation that both n.m.r. studies (of m- F and chemical shifts) and infrared investigations (of the intensities of bands due to certain skeletal vibrations) suggest that the value of Taft s [Pg.226]

Making allowance for those effects gives a good correlation between the chemical shifts and the it- and/or tr-electron density of the carbon atom bearing the proton (133, 236,237). [Pg.70]

TABLE 1-34. PROTON CHEMICAL SHIFTS AND COUPLING CONSTANTS... [Pg.73]

Chemical shifts and coupling constants are described in Tables III-5 and m-6 (112-114). [Pg.345]

The —OH proton of a primary alcohol RCH2OH is vicinal to two protons and its sig nal would be expected to be split into a triplet Under certain conditions signal splitting of alcohol protons is observed but usually it is not Figure 13 21 presents the NMR spec trum of benzyl alcohol showing the methylene and hydroxyl protons as singlets at 8 4 7 and 2 5 respectively (The aromatic protons also appear as a singlet but that is because they all accidentally have the same chemical shift and so cannot split each other)... [Pg.544]

Chapter 13 Spectroscopy has been supple mented by an expanded discussion of H and C chemical shifts and a new section on 2D NMR A new box Spectra by the Thousands points the way to websites that feature libraries of spectra and spectroscopic problems of every range of difficulty... [Pg.1331]

The section on Spectroscopy has been retained but with some revisions and expansion. The section includes ultraviolet-visible spectroscopy, fluorescence, infrared and Raman spectroscopy, and X-ray spectrometry. Detection limits are listed for the elements when using flame emission, flame atomic absorption, electrothermal atomic absorption, argon induction coupled plasma, and flame atomic fluorescence. Nuclear magnetic resonance embraces tables for the nuclear properties of the elements, proton chemical shifts and coupling constants, and similar material for carbon-13, boron-11, nitrogen-15, fluorine-19, silicon-19, and phosphoms-31. [Pg.1284]

C-nmr data have been recorded and assigned for a great number of hydantoin derivatives (24). As in the case of H-nmr, useful correlations between chemical shifts and electronic parameters have been found. For example, Hammett constants of substituents in the aromatic portion of the molecule correlate weU to chemical shifts of C-5 and C-a in 5-arylmethylenehydantoins (23). Comparison between C-nmr spectra of hydantoins and those of their conjugate bases has been used for the calculation of their piC values (12,25). N-nmr spectra of hydantoins and their thio analogues have been studied (26). The N -nmr chemical shifts show a linear correlation with the frequencies of the N—H stretching vibrations in the infrared spectra. [Pg.250]

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. [Pg.308]

Proton chemical shifts and spin coupling constants for ring CH of fully aromatic neutral azoles are recorded in Tables 3-6. Vicinal CH—CH coupling constants are small where they have been measured (in rather few cases) they are found to be 1-2 Hz. [Pg.13]

C and H chemical shifts and the corresponding coupling constants have been determined for the chelate (225 M = Zn(II)) (81M105). [Pg.228]

A number of MO calculations has been carried out, and these have had mixed success in predicting chemical reactivity or spectroscopic parameters such as NMR chemical shifts and coupling constants. Most early calculations did not take into account the contribution of the sulfur 3d-orbitals to the ground state, and this accounts for some of the discrepancies between calculations and experimental observations. Of the MO methods used, CNDO/2 and CNDO/S have been most successful the INDO approximation cannot be used because of the presence of the sulfur atom. [Pg.132]

H NMR Chemical Shifts and Coupling Constants of Isothiazoles (IS) with Exocyclic Conjugation X... [Pg.137]


See other pages where Chemical shift, and is mentioned: [Pg.64]    [Pg.1450]    [Pg.1455]    [Pg.1510]    [Pg.2098]    [Pg.2098]    [Pg.519]    [Pg.354]    [Pg.354]    [Pg.67]    [Pg.342]    [Pg.345]    [Pg.1278]    [Pg.405]    [Pg.405]    [Pg.408]    [Pg.409]    [Pg.55]    [Pg.308]    [Pg.62]    [Pg.63]    [Pg.64]    [Pg.183]    [Pg.185]    [Pg.190]    [Pg.190]    [Pg.197]   


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C Chemical Shifts and Coupling Constants

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Carbon alkane and cycloalkane chemical shifts

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Examples of -coupling and Chemical Shift Evolution

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F Chemical Shifts of Allenes and Alkynes

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H and 13C Chemical Shifts

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Nuclear Screening and the Chemical Shift

Nuclear magnetic resonance chemical shifts and

Pb Chemical Shifts and Structure

Proton Chemical Shifts and Structure

Quadrupole coupling constant and chemical shift anisotropy

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