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THE ANALYSIS OF THE 1 H-NMR SPECTRA OF N-ARYLMETHACRYLAMIDES
Ding Youjun, Qi Daquan, Zhu Xincun, Pan Jingqi
Chinese Journal of Magnetic Resonance, 1989, 6(1): 13-20.
The N-Arylmethacrylamides including N-Phenylmethacrylamide(N-PhMA), N-p-Tolylmelhacrylamide (N-p-TMA), N-o-Tolylmethacrylamide(N-o-TMA),N-p-Bromomethacrylamide(N-p-BrPhMA),N-p-Nitrophenylmethacrylamide (N-p-NPhMA), N-o-Nitrophenylmethacrylamide (N-o-NPhMA), were prepared via the acid route and the chemical shifts of these N-Arylmethacrylamide were determined (see Table 1) on a Varian FT-80A NMR spectrometer.
The substituent groups affect the chemical shifts of adjacent aryl protons as shown in Table 2. Since chemical shifts depends on the electron density around the aryl proton, the methyl group, which is a weak electron releasing group on the benzene ring, increases the electron density on the aryl proton thus will tend to cause an up-field shift; the nitro group, which is a strongly electron withdrawing group on the benzene ring, decreases the electron density on the aryl proton, thus will tend to cause a down-field shift. As an evidence the shifts dH are 7.54ppm, 7.44ppm, 7.76ppm for N-PhMA, N-p-TMA, and N-p-NPhMA, respectively.
In compounds N-o-NPhMA and N-o-TMA the protons labelled dH at lower fields than those in N-p-NPhMA and N-p-TMA, since the former lies in the deshielding zone of the carbonyl group.
This is illustrated below:
The values of the chemical shifts of the six kinds of N-Aryimcthacrylamide were estimated so as to obtain a good agreement between observed and calculated.
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NMR SPECTRA OF RANDOM BUTADIENE-STYRENE COPOLYMER QUANTITATIVE CALCULATION OF DIAD SEQUENCE STRUCTURE
Peng Qinji, Zhang Minjia, Wang Jinliang, Chen Weijie, Yu Fengnian
Chinese Journal of Magnetic Resonance, 1989, 6(1): 21-28.
The compositions of sixteen diads of random butadiene-styrcne copolymers were calculated by using aliphatic carbon portion of the 13 C-NMR spectra, based on the assignment in the previous paper. Compositions of the four monomer units deduced from the calculation were consistent with the results obtained from 1 H-NMR spectra. In the polymerization system, the average sequence lengths of diads and the average permanence ratio of four monomer units indicate that the styrcne unit (S) tends to form short block polymers, vinyl unit (v) shows a tendency to combine with the other three monomer units, trans-1, 4-butadiene unit (t) and cis-1, 4-butadiene unit (c) show tendency to form structures containing alternating units besides the block polymers formed from themselves. The results prove that 13 C-NMR is a powerful tool for investigating the microstructure of butadiene-styrcne copolymers.
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EPR SPECTRA, MAGNETIC PROPERTIES AND ELECTRONIC STRUCTURE OF[Cu2 (O COO C-O-N H-O-CH3 )4 (DMF2 )]·4DMF
Sun Qiongli, Cong Aizhen, Huang Xin
Chinese Journal of Magnetic Resonance, 1989, 6(1): 47-52.
The EPR spectra of binuclear copper (Ⅱ) cluster
·4DMF (1)
in solide and solution at room temperature and 77K have been measured. Three groups of lines are observed. They are attributed to two station of the unpaired elec-tron, in the title compound respectively. One is similar to those of a mononuclcar copper sen which present spectra of groups Ⅰ and Ⅱ, while the spectrum of group Ⅲ manifests itself as a triplet state of two coppers coupling dimer.
In this paper, the EPR parameters for the triplet state of dimeric copper are calculated by spin Hamiltonian formula
H S =
β HgS+DS
z 2 +E(S
x 2 -S
y 2 )-(2)/3D
By comparison of the title compound (1) with
·4DMF (2)
it is found that there are some differences in the ligand structure, i. e. the difference in the position of Benzenering connecting to CH
3 (the former, meta whereas the latter, patra), resulting in the differences of magnetic parameters (effect magnetic mo ment, parameter of the magnetic exchange interaction J, relative electron spin concentration
ρ and h. f. s. parameters).
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THE RELATIONSHIP BETWEEN THE POSITIONS OF EACH TRANSITION IN ABX SYSTEM AND THEIR RELATIVE SIGNS OF COUPLING CONSTANTS IN NMR
Tao Jiaxun, Qi Quan
Chinese Journal of Magnetic Resonance, 1989, 6(1): 93-96.
According to the theory of ABC system, theoretical spectra of ABX system were calculated by varying|J|< 16Hz and the positions and intensities of each specific transitions were analyzed The general rules of the position of each transition in ABX system with various values of coupling constants and their signs were found out Then, a simple procedure was designed by which relative signs of couping constants can be obtained without calculating precisely through intensities of each peak, as follows: 1. To distinguish the four peaks of each A, B, X nuclei in ABX system and to give their marks in order, respectively. (For example, from left to right, a1 ~a4 ,b1 ~b4 ,and x1 ~x4 , neglecting the mixing transitions.) 2. To get a related diagram discribing the relationship between each peak using double resonance methods. 3. Through inter-exchanging of the marks of the same kind of peaks, finally you can always let a1 , b1 , x1 to be at the bottom and a4 , b4 , x4 on the top as a usual diagram of energy level. 4. If you don't need to inter-exchange any marks of peaks, the signs of three coupling constants are the same; if you need to do, then, the sign of coupling constant between relative nuclei due to inter-exchanging must be opposite sign to the other two.