Admittance detection, more commonly called capacitively coupled contactless conductivity detection, is widely used. While the true conductance of a solution is linear with concentration up to ∼1 mequiv/L, the admittance signal is nonlinear. In small-bore capillaries and highly resistive solutions, such as in suppressed open tubular ion chromatography (SOTIC), the admittance signal is exponentially related to concentration. Solution contact conductivity detection is common in microfluidics, but no true conductivity measurement efforts have been made with conventional capillaries in the last two decades. We examine five solution contact cell geometries: (A) wire/disk electrodes perpendicular to the flow direction, (B) annular tubular electrodes facing the flow (that exits through the center tube), (C) ring-disk electrodes facing the flow that exits through the annulus, (D) coplanar parallel wire/disk electrodes facing the flow that exits around the electrodes, and (E) planar electrodes separated by a thin insulating layer with a through-hole in which the liquid flows. Present limitations of the available components as well as the designs themselves do not allow type A and B cells to reach low enough dispersion levels. Types C-E all produce the same efficiency for chloride in a SOTIC setup (12000 ± 200 plates/m), limited by dispersion in the suppressor. Further choice and refinement will be dictated by the availability of a lower dispersion suppressor. All such contact conductance results were linear with concentration, and initial results suggest that attainable LODs will be competitive with those from benchtop ICs.