Page 68 - Analytical Electrochemistry 2d Ed - Jospeh Wang
P. 68

2-4  ELECTROCHEMICAL QUARTZ CRYSTAL MICROBALANCE                 53



                              a

                              b


                              c                           d






                                            e

            FIGURE 2-20  The quartz crystal microbalance: a, the quartz crystal; b, the gold electrode; c
            and d, connecting metal wires; e, the base.


            in the bulk of the wafer. Surface reactions involving minor mass changes can cause
            perturbation of the resonant frequency of the crystal oscillator. The frequency
            change …Df † is related to the mass change …Dm† according to the Sauerbrey equation:

                                                   p
                                                2
                                   Df ˆ 2 Dmnf =A mr                      …2-19†
                                                     
                                                0
            where n is the overtone number, f  0  is the base resonant frequency of the crystal
                                                 2
            (prior to the mass change), A is the area (cm ), m is the shear modulus of quartz
                                                                  3
                              1
                    11
            (2:95   10 gcm  1  s †, and r is the density of quartz (2.65 g cm ). As expected
            from the negative sign, decreases in mass correspond to increases in frequency and
            vice versa. The Sauerbrey equation forms the basis for the excellent mass sensitivity
            of the EQCM. In-situ mass changes of 1 ng cm  2  can thus be detected. Such high
            sensitivity and in-situ capability represent the major advantages of EQCM experi-
            ments.
              The EQCM is very useful for probing processes that occur uniformly across the
            surface. Numerous surface reactions have been investigated, including deposition or
            dissolution of surface layers and various uptake processes (such as doping=undoping
            of conducting polymers or ion-exchange reactions at polymer ®lms). Such changes
            can be probed using various controlled-potential or controlled-current experiments.
            In these experiments, one of the electrodes (on the wafer) contacts the solution and
            serves as the working electrode in the electrochemical cell, to allow simultaneous
            frequency and current measurements. For example, Figure 2-21 displays the
            frequency (mass) versus potential pro®les, and the corresponding cyclic voltammo-
            grams, during the uptake of a multiply charged complex ion at an ion exchanger-
            coated electrode. Other useful examples of probing the uptake of mobile species by
            polymer-coated electrodes have been given by Hillman et al. (66). Application of the
            Sauerbrey equation to the study of polymeric ®lms in solutions requires adherence to
            the rigid ®lm approximation (i.e., behavior of an elastic, solvent-free thin layer).
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