Source Data for Baldelli et al., Performance of single nanopore and multi-pore membranes for blue energy
Description
HOW TO read and utilized all the files used to create Figure 2 of the manuscript.
The files are divided in two folders:
- Charge: in the "Charge" folder, two files can be found: rt_2nm.log and rt_5nm.log.
In these files, 4 tables are reported. Each table represents the ionic currents
(I- and I+) versus the surface charge density, for a zero applied external voltage
and for different nanopore geometries.
In particular, in the rt_2nm.log file, the charge-current curves for the conical
and bullet-shaped nanopores with a tip radius (rt) of 2 nm are reported.
In rt_5nm.log, charge-current curve for all the geometries and for rt = 5 nm are reported.
In principle, these files can be used to evaluate the transference number t-, Eq.(1) and
then Eq.(3) and Eq.(4) of the manuscript it is possible to draw all the
panels in Fig.2 maintaining the error low.
To compute the total current, that is the osmotic current since no external voltage is
applied, sum the second and the third column with their sign.
In both the files: use the first table per conical nanopore performance; the second table
for BS2 nanopore performance; use the third table for BS4 nanopore performance;
use the fourth table for BS6 nanopore performance
- Voltage: the "Voltage" folder is divided in other two sub-folders rt_2nm and rt_5nm.
In this folder the complete I-V curvers for all the surface charge considered in the
manuscrip are reported.
In rt_2nm (rt_5nm) subfolder the I-V curves for the nanopores characterized
by a tip radius (rt) of 2 nm (5 nm) are reported.
In each sub-folder the I-V, one file for each surface charge considered can be found.
For instance, the file rt2nm_160mCm2.log contains the I-V curves for all the geometries
with a surface charge of 160 mC/m^2.
In the following, we explained how to obtain each panels of Fig.2 of the main manuscript.
Note that the second row of Fig.2 (panels b,d,f and h)
can be drawn in the same way of the first row (panels a,c,e and g), hence
in the following we explain only how to draw the first rows and the same approach
remains valid for the second one.
Let's start using files in the rt_2nm sub-folders.
- Panel (a): The osmotic current I_o, is the current for a zero applied
external voltage.
Therefore, this panel can be drawn using the first row of each column for all the files
in the sub-folder. Note that in the first row of a table the current for a zero voltage
is reported.
The second way to draw this panel is using the Charge/rt_2nm.log file.
In fact in this file the current for zero voltage and for all the charges is reported.
- Panel (c): The membrane potential E_m is the voltage measured across the membrane
at zero current condition. Therefore can be obtained through the I-V curve
observing at which voltage value the current curve intersects the voltage axis itself.
For those files that contain separate ionic and cationic currents, these should be
summed to obtain the total current I_tot. If the file only contains tables with a
voltage column and I_tot, then the second column can be used directly.
- Panel (e): The transference number t_- can be calculated using the Eq.(1).
For those files that contain separate ionic and cationic currents, t_- can be
calculated using the second (anionic current I-)
and third column (cationic current I+) (and Eq.(1)).
For those file that contain only I_tot, t- can be calculated by inverting Eq.(3)
(considering the activity coefficients equal to 1), having previously calculated
the membrane potential E_m (see the previous point).
- Panel (g): From the I-V curve, draw the P-V curve and then estimate the maximum power.
If the file contains the anionic and cationic current separately, sum these currents
to obtain I_tot and then using it to draw the P-V curve.
If only I_tot is reported, use it directly to plot the P-V curve.
For the panels (b, d, f and h) use the same approach but working with the data reported
in the rt_5nm sub-folder.
Files
IV_file.zip
Files
(25.4 kB)
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