1958
DOI: 10.1021/j150559a013
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The Determination of the Electrical Conductivities of Some Concentrated Electrolyte Solutions Using a Transformer Bridge

Abstract: A method for the determination of the conductivities of solution without the use of contacting or dipping electrodes is described. This involves the use of a transformer ratio-arm bridge operating a t audio-frequencies, and this is described in detail. Results obtained for concentrated solutions of barium chloride, magnesium sulfate and potassium ferro-and ferricyanides are given.

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Cited by 37 publications
(5 citation statements)
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“…The ohmic contribution to total cell resistance depends not only on the concentration of the electrodically active ions, i.e., the cations in the Fe(CN)/Fe(CN) couple, but also depends on the sum of any ohmic contributions from the anions and the background electrolyte. Table 1118, 19 shows the various contributions in the electrolyte which give a total solution conductivity, tot, of Ca. 19.6 S m. The total ohmic contribution to the total cell resistance can be determined from this using (3E/a1).…”
Section: Resultsmentioning
confidence: 99%
“…The ohmic contribution to total cell resistance depends not only on the concentration of the electrodically active ions, i.e., the cations in the Fe(CN)/Fe(CN) couple, but also depends on the sum of any ohmic contributions from the anions and the background electrolyte. Table 1118, 19 shows the various contributions in the electrolyte which give a total solution conductivity, tot, of Ca. 19.6 S m. The total ohmic contribution to the total cell resistance can be determined from this using (3E/a1).…”
Section: Resultsmentioning
confidence: 99%
“…For Ganymede, we simulate a second ocean layer at the water-rock interface at a depth of 900 km. Lying under 530 km of ice VI (Vance et al, 2018), this layer is modeled as a 30-km-thick high-conductivity region (20 S/m) corresponding to a nearly saturated MgSO 4 solution, consistent with (Hogenboom et al, 1995) and (Calvert et al, 1958). The influence of such a layer (dotted lines in Figure 6) is a ∼1% decrease in amplitude at the orbital period of 171.57 h. The amplitude decrease results from mutual induction between the conducting layers at this period.…”
Section: Amplitude and Phase Delay Of The Diffusive Responsementioning
confidence: 93%
“…For Ganymede, we simulate a second ocean layer at the water–rock interface at a depth of 900 km. Lying under 530 km of ice VI (Vance et al., 2018), this layer is modeled as a 30‐km‐thick high‐conductivity region (20 S/m) corresponding to a nearly saturated MgSO 4 solution, consistent with (Hogenboom et al., 1995) and (Calvert et al., 1958). The influence of such a layer (dotted lines in Figure 6) is a ∼1% decrease in amplitude at the orbital period of 171.57 h. The amplitude decrease results from mutual induction between the conducting layers at this period.…”
Section: Diffusive Induction In Jupiter's Ocean Moonsmentioning
confidence: 93%