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P. No6ak et al. / Spectrochimica Acta Part A 54 (1998) 327–333
2
2
2
Ph type, where Ph refers to phenyl and Z to a
bridging group (CꢀC, CꢀO, CꢀN, NꢀN, etc.),
affects NMR parameters throughout the
molecule. Thus, deuterium causes perturbations in
13C nuclear shielding up to ten bonds away [4].
Besides, some isotope effects are interesting be-
cause of their dependence on structural parame-
ters, such as torsional angles [5] and lone-pair
interaction [4e]. For a series of isotopically la-
belled 1 investigated here (Scheme 1), it is shown
that long range deuterium isotope effects and
2H1), 5 (97% H1), 6 (95% H1), 7 (91% H1), 8
2
2
2
(97% H1), 9 (79% H2), 10 (97% H5), 11 (96%
2
2
2
2H5), 12 (92% H6), 13 (85% H6), 14 (92% H10),
15 (89% H11) and 16 (99% 15N).
2
2.2. NMR measurements
NMR spectra were recorded with Varian Gem-
ini 300, Bruker AM-360 and Varian Unity Inova
600 spectrometers, operating at 75.4, 90.6 and
150.9 MHz for the 13C resonance, respectively.
Samples were measured at 294 K in 5 mm tubes.
Variable temperature measurements were per-
formed in the temperature range of 274–324 K.
Sample concentrations were 0.15–0.20 M. Deu-
terium from the solvent was used as the lock
signal and TMS as the internal standard. Narrow
region spectra with spectral widths of 500–2000
Hz were zero-filled to 64 K, thus obtaining a
digital resolution better than 0.03 Hz per point
(i.e. 90.2 ppb for 13C at 150.9 MHz) after
Fourier transformation.
Isotope effects were determined as a difference
between chemical shifts of the light and heavy
isotopomer (D=lL-lH), expressed in parts per
billion (ppb) units. Standard deviations are given
in Table 1. For non-additivity estimations total
errors were obtained by summing up the individ-
ual mean square errors of the corresponding ef-
fects.
1
their non-additivity on H and 13C chemical shifts
of the imino group are a sensitive probe of molec-
ular geometry.
2. Experimental
2.1. Preparation of isotopomers
Trans-N-benzylideneaniline isotopomers (tBA)
(2–16) were prepared by the addition of specifi-
cally deuteriated anilines to corresponding ben-
zaldehydes [6]. The isotopomers were purified by
recrystallization from 85% ethanol. The melting
point of all synthesised compounds was 50–52°.
Benzaldehyde (Kemika), aniline (Fluka), h-2H-
2
benzaldehyde (Merck), H5-benzaldehyde (Merck)
and 2H5-aniline (Campro Scientific) were commer-
cial products. 2-, 3- and 4-2H-aniline were synthe-
sised by catalytic hydrogenolysis of 2-, 3- and
4-bromoaniline, respectively, with 5% palladium
on charcoal and deuterium gas in tetrahydrofuran
[7]. 2-, 3- and 4-2H-benzaldehydes were prepared
by the following reactions: 2-, 3- and 4-2H-tolue-
nes were mixed with N-bromosuccinimide and
dibenzoylperoxide to give 2-, 3- and 4-2H-benzyl-
bromides, respectively. Benzylbromides were then
allowed to react with hexamethylenetetramine in a
mixture of acetic acid and water [8]. 2-, 3- and
4-2H-toluenes were synthesised from respective
bromotoluenes via the Grignard reaction with
magnesium activated using 1,2-dibromoethane as
entrainer [9]. The reaction mixture was quenched
3. Results and discussion
3.1. Deuterium isotope effects
1H and 13C NMR spectra (Figs. 1 and 2) of the
imino group (–ChHhꢀNh–) in deuteriated isoto-
pomers of 1 reveal a number of interesting isotope
effects (Table 1). All observed deuterium effects at
H-h are negative, i.e. deshielding, while the effects
at C-h are either positive (shielding) or negative
(Table 1). The effects at H-h are much smaller
than those at C-h, primarily due to the relatively
narrow 1H chemical shift range. From this reason,
intrinsic isotope effects on 1H chemical shifts have
rarely been reported in the literature [10]. In de-
termination of such effects (Fig. 1), high precision
measurements are required.
2
with H2O.
The deuterium contents, determined with an
Extrel FTMS 2001 DD mass spectrometer, were
2
2
the following: 2 (90% H1), 3 (90% H1), 4 (90%