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Liquid-carrier-based, ion-selective electrodes have been successfully employed for decades and for many ions, highly specific sensors are available 22-26. When used in the extracellular space (ECS) of vertebrate brain preparations, one must keep in mind, however, that this is a quite invasive technique: while the width of the ECS is only around 20-50 nm, the diameter of ion-selective microelectrodes is about 1 µm (double-barreled electrodes) or larger (concentric electrodes). The tips of ion-selective microelectrodes will thus not only damage tissue during their impalement of the tissue, but also enlarge the ECS, favouring an underestimation of ion transients. Despite these pitfalls, extracellular ion transients in response to neuronal activity are remarkably consistent between different laboratories 7,8, attesting to the reliability of this method.
The performance and suitability of ion-selective electrodes is dependent on their sensitivity and selectivity, which is defined by the sensor cocktail ('liquid membrane ionophore') used. Sensor cocktails contain a special carrier molecule, e.g. valinomycin for K+-selective microelectrodes which exhibits a high selectivity for potassium 27. Notwithstanding, cross-reactivity with other ions can occur and must be tested. Valinomycin exhibits a significant cross-reactivity for ammonium, which has to be considered when interpreting results (e.g. 11,12). Furthermore, because the voltage-response of the ionophores follows a Nernstian behavior (cf. equation 1), the signal-to-noise ratio and detection threshold depend on the concentration of the ion to be measured. Thus, while small [K+]o transients evoke large voltage changes against the low baseline [K+]o, small [Na+]o transients are much more difficult to detect against the high baseline [Na+]o (cf. Figure 5 and 6).
The performance of ion-selective electrodes is also determined by the temporal resolution, which is largely governed by its electrical time constant. The latter is mainly determined by the axial resistance of the sensor, and by the distributed capacitance along the length of the pipette, between its internal solutions and the external fluid. In the double-barreled configuration, the resistance is high, owing to the long column of backfilled ion sensor. For a given insulating dielectric (in this case borosilicate glass), the capacitance is governed by the dielectric thickness. In double-barreled electrodes, the dielectric width amounts to the glass wall of the pipette. As the glass thins close to the tip, the dielectric width falls, and the capacitance increases. These factors combine to produce electrodes with response times that range from several hundred milliseconds to several seconds, as these factors are varied.
A major advantage of the concentric design is that both the axial resistance and the capacitance to the bath are greatly diminished. The concentric pipette shunts most of the resistance of the backfilled ion exchanger, leaving only a remnant in the last few micrometers before the tip. In addition, the filling solution within the concentric pipette is physically distanced from the bath, separated by the thickness of two glass walls, greatly reducing the capacitance. As shown earlier 10, the combined effect of reduced resistance and capacitance is an improvement in temporal resolution of two orders of magnitude. In the case of concentric Ca2+ and pH microelectrodes, 90% response times were as low as 10-20 msec 10. A related advantage of the concentric design is the lower noise level (cf. Figure 8). Owing to the greatly reduced resistance, voltage transients from any ambient noise are minimized. Moreover, recovery from such transients is rapid, because of the fast time constant. Such artifacts are therefore small and fast, and have a less disruptive effect on physiological recordings (cf. Figure 8).
There are also disadvantages of the concentric technique. First, their assembly is more complex, and time-consuming. A second disadvantage is the need to place a separate reference microelectrode with its tip, entailing use of either a separate micromanipulator or a specialized dual manipulator. Finally, double-barreled microelectrodes can be extended to a triple-barreled design, allowing detection of two different ion species at the same time 28, which is not possible for concentric electrodes.
Most common pitfalls
Inefficient silanization.
The most important step, and principal obstacle in fabrication of any liquid-sensor based ion-selective microelectrode is the silanization procedure. When electrodes fail to respond to changes in specific ion concentration, or respond with a sub-Nernstian response (i.e., well less than 58 mV per ten-fold concentration difference), poor efficacy of silanization is typically the cause. In our experience, this can occur if atmospheric humidity is too high, or too low, typical of conditions at the height of summer, or winter, respectively. If it is feasible to exert some control over room humidity, these problems may be overcome.
Electrode resistance is too high.
If needed, the resistance of the ion-sensitive barrel can be reduced by bevelling. To this end, expose its tip to a strong jet of an abrasive suspended in water for a couple of seconds. This will cause its upmost tip to break and lower the resistance to the desired value.
Salt bridges.
Salt bridges between the ion and reference barrels result in poorly or none-responding electrodes and can thus also greatly confound their performance in the calibration. As mentioned above (see point 1.6.), this is mainly an issue when double-barreled theta glass is chosen, but is a rare occurrence when using the offset, twisted barrel technique described here.
With ease of fabrication in mind, the original double-barreled design of Lux 29 can often be used profitably. This method utilizes pre-filling of the ion and reference barrels with salt solutions, a fast exposure to a silane solution by its suction and expulsion from the tip, following by incorporation of ion-exchanger, also via the tip (see 30,31). These electrodes can be fabricated in roughly 10 min, but their tip size is typically 4 µm or more and they are more prone to fail during an experiment. In contrast, silanization methods that involve exposure to silane vapor and heating can produce electrodes with smaller tips that last days, and sometimes weeks.
Taken together, there are several protocols and approaches on how to prepare ion-selective microelectrodes. Here, we have described two main procedures for fabrication of twisted double-barreled as well as concentric microelectrodes which work well and reliably in our laboratories, with an overall success rate of close to 100%. Importantly, these techniques will be transferable to measurement of other ions species, including pH or calcium, and will also be applicable to other preparations than the brain, including fluid-filled cavities or fluids in general. Last, but not least, ion-selective microelectrodes allow determination of ion concentrations inside cells. Because of their relatively large tip size (~ 1 µm), this will, however, be possible only in cells with a large cell body, e.g. such as found in invertebrate preparations 28,32.