Our project requires a convenient way to measure ion selectivity and biofilm robustness. Although ion selectivity and robustness are difficult to measure directly, the so-called open circuit potential provides a convenient indicator of both ion selectivity and robustness.
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Consider a perfect cation exchange membrane which allows all cations to pass but blocks all anions. If such a membrane is used to separate two compartments containing water with different NaCl concentrations, selective diffusion of ions takes place. Specifically, positively charged sodium ions diffuse across the membrane in the towards the lower salt concentration. | Consider a perfect cation exchange membrane which allows all cations to pass but blocks all anions. If such a membrane is used to separate two compartments containing water with different NaCl concentrations, selective diffusion of ions takes place. Specifically, positively charged sodium ions diffuse across the membrane in the towards the lower salt concentration. | ||
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Hence, a net positive charge is transported across the membrane. Thus, one compartment gains a net positive charge while the other gains a net negative charge. This difference in charge between the compartments creates an electric field, which counteracts the diffusion of sodium across the membrane. The famous Nernst equation predicts that all diffusion stops when a potential difference of 86 mV is reached. | Hence, a net positive charge is transported across the membrane. Thus, one compartment gains a net positive charge while the other gains a net negative charge. This difference in charge between the compartments creates an electric field, which counteracts the diffusion of sodium across the membrane. The famous Nernst equation predicts that all diffusion stops when a potential difference of 86 mV is reached. | ||
Revision as of 14:43, 17 September 2015
Open circuit voltage
Consider a perfect cation exchange membrane which allows all cations to pass but blocks all anions. If such a membrane is used to separate two compartments containing water with different NaCl concentrations, selective diffusion of ions takes place. Specifically, positively charged sodium ions diffuse across the membrane in the towards the lower salt concentration.
figure: diffusion across a membrane
Hence, a net positive charge is transported across the membrane. Thus, one compartment gains a net positive charge while the other gains a net negative charge. This difference in charge between the compartments creates an electric field, which counteracts the diffusion of sodium across the membrane. The famous Nernst equation predicts that all diffusion stops when a potential difference of 86 mV is reached.
Since a potential difference is only observed if selective diffusion takes place and, moreover, the potential at which the net charge flow is zero is dependent on the selectivity of the membrane, measurements of the open circuit potential can be used to calculate the (apparent) selectivity of the membrane.
The core of our setup consists of a flow cell originally designed as a microbial fuel cell. This cell consists of two compartments through which water flows are directed using two dropping funnels. These funnels can be loaded salt solutions of different concentrations.
The potential between the two compartments was measured using two commercial Ag/AgCl reference electrodes connected to a PREMA 5000 multimeter. The measurements for non-GMO membranes were repeated using a high quality potentiostat <model no?> to check if the multimeter was not drawing too much current.