EQCM Investigations of a Thin Polymer Film
This Application Note is intended to provide the reader with a general framework for characterization of an electroactive polymer film. Electropolymerization is a convenient way to control film growth either through repeated cycling, potential steps, or current steps. Examination of the film redox behavior in monomer-free, fresh electrolyte provides insight on doping and dedoping of these polymer films.
Polybithiophene films were assembled by cycling an Au-coated 10 MHz quartz crystal between 0 and 1.5 V in the presence of 1 mM bithiophene solution containing 100 mM tetrabutylammonium perchlorate (TBAP) in acetonitrile (MeCN). Potentials are reported against a Ag|Ag+ pseudo-reference electrode. The PTFE cell was outfitted with a PTFE O-ring to prevent swelling from the acetonitrile and placed inside a VistaShield™. The cell was connected to an eQCM10M™ Quartz Crystal Microbalance which was coupled to a Reference 600+™. Both instruments were connected to a computer running Resonator™ software. Bithiophene electropolymerizes via a two-electron oxidation at potentials greater than ~1.25 V versus a Ag|Ag+ pseudo-reference electrode.
Results and Analysis
Figure 1 shows two cycles of film growth. Cycle 1 (blue curve) shows only background (non-Faradaic) current until the potential is greater than 1.25 V. Cycle 2 shows additional Faradaic current beginning at approximately 0.75 V due to oxidation of the polymer film. Polymerization still happens at potentials greater than 1.25 V. The small spike at 1.1 V is related to an irreversible film rearrangement, for subsequent cycles (seen when thicker films were prepared) show no current spike.
Figure 1: Electropolymerization of 1 mM bithiophene in 0.1 M TBAP/MeCN. Scan rate was 50 mV/s.
After the film was deposited, the cell was washed with MeCN and then refilled with monomer-free electrolyte. Cycling of the polymer film revealed a broad-shaped couple at approximately 1 V (Figure 2). Mass increases during oxidation and decreases during reduction, respectively, yet does not return to the initial value indicating some loss of solvent, electrolyte, or polymer film.
Figure 2: Mass and current versus voltage for one cycle of polybithiophene in 0.1 M TBAP/MeCN. Scan rate was 100 mV/s.
Echem Analyst™ software calculates mass changes based on ∆fseries, the change in series resonant frequency, using the rewritten Sauerbrey1 equation below:
where Df is the change in frequency and Cf is the theoretical calibration factor, 226 Hz cm2/µg, for a 10 MHz AT-cut quartz crystal. Mass change plotted against charge for a cycle in monomer-free electrolyte reveals information about mobile species during oxidation and reduction. Figure 3 shows the change in mass (∆m) versus the charge (C) for the first redox cycle.
Figure 3: Change in mass versus charge for one redox cycle of polybithiophene in 0.1 M TBAP/MeCN. Scan rate was 100 mV/s.
The overall slope during oxidation is 1916 µg/C. This can be converted to a molar mass by the following equation
where F is Faraday’s constant, and n is the number of electrons. Here n = 1 because each thiophene in the polymer ring is being oxidized. The molar mass of 185 g/mol indicates that one perchlorate (99.5 g/mol) and approximately two molecules of MeCN (41 g/mol) enter the film for each electron that leaves the film.
Closer examination of Figure 3 reveals differences in slope within the oxidation and reduction. Note that the beginning of the oxidation has a lower slope than the second half of the oxidation. Upon scan reversal, the slope is lower initially. Because electroneutrality must be maintained—one anion per electron—we can attribute these differences to differences in solvent ingress/egress. Solvent ingress is slower in the first part of the oxidation and the first part of the reduction.
A future application note will deal with thicker polybithiophene films which become viscous and swell when cycled in the presence of electrolyte. In these instances, mass measurements must be examined with a bit of skepticism because viscoelastic losses and density changes can also contribute to frequency changes. Please see our Basics of a Quartz Crystal Microbalance application note for more information on how viscoelasticity and density affect measurements.
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