E2 and E1cb Mechanistic Borderline
reaction can no longer compete, the E1cb mechanism
becomes the predominant reaction pathway.
As stated in the Introduction, the change of the
mechanism from E2 to E1cb could occur by the merging
of the transition state, if it is difficult for the energy
maximum of the E2 mechanism and an energy well of
the E1cb mechanism to coexist for a single compound at
almost the same position on the energy diagram.1-4
However, if the positions of the transition states are
significantly different, they should be able to coexist, as
observed in the E2 and E1 borderline.5-7 The change in
elimination mechanism observed in the present study is
concluded to be of this type. Because the E2 transition
state is located near the center of the horizontal reaction
coordinate, which is far from the position of the E1cb
transition state, there seems to be no reason for why the
two transition states cannot coexist. Furthermore, the
mechanism changes systematically from the concurrent
E2 and E1cb mechanisms to E2 as the E2 transition state
is stabilized by the better leaving group and to the E1cb
extreme when the strongly electron-withdrawing â-aryl
group stabilizes the latter transition state. To our knowl-
edge, this is the first example that shows a gradual
change in the elimination reaction mechanism from E2
to E1cb via a competing E2 and E1cb mechanism
wrought by the systematic variation of the reactant
structure.
F IGURE 5. Reaction coordinate diagram for the ketene-
forming elimination. The effect of the change to a poorer
leaving group and a weaker base are shown by the shift of
the transition state from A to B and A to C, respectively.
Exp er im en ta l Section
observed increase in the |âlg| values as the catalyst is
made less basic (Table 4) is another manifestation of this
effect, i.e., pxy ) ∂âlg/∂pKBH > 0. On the More-O’Ferall-
J encks diagram in Figure 5, a change to a poorer leaving
group will raise the energy of the bottom edge of diagram
shifting the transition state toward the product and the
E1cb intermediate. The transition state on the horizontal
reaction coordinate will then move toward the left, with
more proton transfer and a larger â, as depicted by a shift
from A to B on the energy diagram (Figure 5).1-3
Similarly, a weaker base will raise the energy of the left
side of the diagram and shift the transition state from A
to C to increase in the extent of CR-OAr bond cleavage
(Figure 5).1-3 The positive pxy coefficients are not consis-
tent with an E1cb mechanisms for which pxy ) 0 is
expected but provide additional support for the concerted
E2 mechanism.1-3
Ch a n ge of th e Mech a n ism . The kinetic results
described above clearly indicate that the elimination
mechanism changes from E2 to a competing E2 and E1cb
to E1cb as the reactant structure is changed from 1c-e
to 1a ,b to 2a . The most reasonable explanation for this
result is as follows. As discussed above, the position of
the E2 transition state for the reactions from 1e could
be located at A in Figure 5. As the leaving group is made
poorer (1c,d ), the reactant-like E2 transition state gradu-
ally changes to the E1cb-like, as indicated by a shift from
A to B (vide supra). When the leaving group ability is
further decreased to Y ) H and OMe (1a ,b), the E2
transition state is destabilized and the E1cb mechanism
emerges simultaneously. It is interesting to note that the
E2 transition states for eliminations from 1a ,b are more
E1cb-like than 1c-e (vide supra). Finally, when the
carbanion intermediate is stabilized by the strongly
electron-withdrawing â-aryl group (2a ), so that the E2
Ma ter ia ls. 4-Nitrophenyl p-nitrophenylacetate (1a ) and 2,4-
dinitrophenyl p-nitrophenylacetate (1e) were available from
previous study.9 Aryl p-nitrophenylacetates (1b-d ) were
prepared from 4-nitrophenylacetic acid and substituted phe-
nols in the presence of Et3N and 2-chloro-N-methylpyridinum
iodide as previously reported.9 p-Nitrophenyl 2,4-dinitrophe-
nylacetate (2a ) was prepared by treating 2,4-ditrophenylacetyl
chloride with 1 equiv of the sodium 4-nitrophenoxide in
methylene chloride as previously reported.26 The yield (%),
melting points (°C), IR (KBr, CdO, cm-1), NMR (300 MHz,
CDCl3), and combustion analysis data for the new compounds
are as follows.
2-Met h oxy-4-n it r op h en yl p-Nit r op h en yla cet a t e (1b ).
Yield 34%; mp 101 °C; IR 1759 (CdO); 1H NMR δ 3.88 (s, 3H),
4.04 (s, 2H), 7.17 (d, 1H, J ) 8.7 Hz), 7.58 (d, 2H, J ) 8.7 Hz),
7.83 (d, 1H, J ) 2.6 Hz), 7.89 (dd, 1H, J ) 8.7, 2.6 Hz), 8.25
(d, 2H, J ) 8.7 Hz). Anal. Calcd for C15H12N2O7: C, 54.22; H,
3.64; N, 8.43. Found: C, 54.27; H, 3.65; N, 8.36.
2-Ch lor o-4-n itr oph en yl p-Nitr oph en ylacetate (1c). Yield
29%; mp 128 °C; IR 1764 (CdO); NMR δ 4.09 (s, 2H), 7.33 (d,
1H, J ) 8.7 Hz), 7.60 (d, 2H, J ) 8.7 Hz), 8.20 (dd, 1H, J )
8.4, 2.7 Hz), 8.28 (d, 2H, J ) 8.4 Hz), 8.36 (d, 1H, J ) 2.7 Hz).
Anal. Calcd for C14H9N2O6Cl: C, 49.94; H, 2.69; N, 8.32.
Found: C, 49.90; H, 2.68; N, 8.23.
2-Tr iflu or om et h yl-4-n it r op h en yl p -Nit r op h en yla ce-
ta te (1d ). Yield 25%; mp 131 °C; IR 1765 (CdO); NMR δ 4.08
(s, 2H), 7.49 (d, 1H, J ) 8.7 Hz), 7.55 (d, 2H, J ) 8.7 Hz), 8.26
(d, 2H, J ) 8.7 Hz), 8.45 (dd, 1H, J ) 8.7, 2.6 Hz), 8.58 (d, 1H,
J ) 2.6 Hz). Anal. Calcd for C15H9N2O6F3: C, 48.66; H, 2.45;
N, 7.57. Found: C, 48.67; H, 2.57; N, 7.60.
p-Nitr oph en yl 2,4-Din itr oph en ylacetate (2a). Yield 32%;
mp 136 °C; IR 1759 (CdO); NMR δ 4.43 (s, 2H), 7.30 (d, 2H,
J ) 8.9 Hz), 7.70 (d, 1H, J ) 8.9 Hz), 8.30 (d, 2H, J ) 9.3 Hz),
8.54 (dd, 1H, J ) 9.3, 2.4 Hz), 9.07 (d,1H, J ) 2.4 Hz). Anal.
Calcd for C14H9N3O8: C, 48.40; H, 3.67; N, 12.10. Found: C,
48.35; H, 3.55; N, 12.05.
Acetonitrile was purified as described before.9 The solutions
+
of R2NH/R2NH2 in 70 mol % MeCN(aq) were prepared by
dissolving equivalent amount of R2NH and R2NH2+ in 70 mol
J . Org. Chem, Vol. 67, No. 15, 2002 5237