C O M M U N I C A T I O N S
Figure 1. Binding capacities of SPP for EA9A in acetonitrile after heating
(83 °C, 26 h) in solvents of varying polarity (From left to right: cyclohexane,
dioxane, ethyl acetate, tert-butanol, acetonitrile, 2-propanol, ethanol, ethanol/
water (1:1), water).
Figure 3. Measured EA9A binding capacities of SPP ([) and CP (9)
after repeatedly heating (83 °C, 26 h) in acetonitrile and then in water. The
SPP was also repeatedly shaken in acetonitrile and then water without
heating (2).
In summary, the programmable polymers based on restricted
rotation were developed that can be reversibly shaped at elevated
temperatures and can maintain these solvent-induced conformational
changes on cooling to room temperature.
Acknowledgment. This work was supported by the NSF (CHE
0616442).
Supporting Information Available: Experimental details, NMR
spectra, and crystallographic data. These material is available free of
Figure 2. Change in binding capacity over 26 h for a high-affinity SPP
heated (83 °C) in acetonitrile (9) and a low-affinity SPP heated (83 °C) in
water ([).
affinity SPP (prepared by heating in water) was heated in a less
polar solvent (acetonitrile) at 83 °C. The systematic transformation
into a low-affinity SPP was followed over 26 h (Figure 2, 9). The
complementary experiment was also performed in which a low-
affinity SPP (prepared by heating in CH3CN) was heated in water.
The systematic transformation into a high-affinity polymer appeared
to occur at the same rate. This was confirmed by kinetic analyses
of the rate curves. Both rate curves could be fit to first-order kinetic
equations, yielding rates of 3.1 and 3.6 × 10-4 s-1. The rate order
and activation energies (27.1 and 27.0 kcal/mol) of the solvent-
imprinting processes were of similar magnitudes to the rotational
barrier of 4 and other structurally similar N-arylimides.4,10 The high
activation barriers were also consistent with the ability of the SPPs
to maintain their solvent-induced changes for a week without a
measurable change in binding capacity.11
We have previously demonstrated that the conformational
changes of atropisomeric systems are reversible, allowing the
properties to be repeatedly “written” and “erased”.4a-c To test
whether similar levels of reversibility could be observed in the SPP,
a sample was repeatedly heated (83 °C, 26 h) in acetonitrile and
water (Figure 3, [). The solvent-induced switching was shown to
be reversible and proceeded with high fidelity. The binding
capacities of the high- and low-affinity SPP states remained constant
over 5 cycles. Control studies were also carried out to verify that
the solvent-induced changes were due to rotation about the
Caryl-Nimide bonds and were not due to differences in hydration or
swelling of the polymers after heating in the different solvents. First,
the SPP was subjected to the same cycle of immersion in CH3CN
and water but without heating (Figure 3, 2). Second, a control
polymer (CP) made with monomer 3 was tested that lacked
restricted rotation. Both cases did not display the solvent-memory
effects, as the binding capacities remained relatively constant
(Figure 3, 9). The control studies showed that (1) the combination
of solvent and heat were necessary to change the binding properties,
(2) the presence of monomer 1 with restricted rotation was essential,
and (3) the switching process cannot be explained by the presence
of residual solvent in the polymers gels.
References
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(6) The rotational barrier of 1 could not be measured because the bicyclic bridge
sterically biases the atropisomer to form only a single isomer. After
polymerization, this steric bias is removed as the bicyclic ring is broken in
the ROMP. Thus, the fused ring system of compound 4 is a more
appropriate model for the C-N rotational barrier in the ROMP product.
(7) For a binding study, 60 mg of polymer were shaken with 0.1 mM EA9A
in CH3CN (2.5 mL). The concentration of EA9A in the supernatant was
measured by UV-vis (257 nm) and compared with the original stock
solution.
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(11) Using the Eyring equation, a barrier of 27.1 kcal/mol equates to a half-life
of 56 days at 25 °C.
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