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This command opens a dialog box that enables the user to specify the following parameters referring to the active experiment:

 

MessExperimentDlg

 

tipbulb A value of Cdl (F) written in magenta indicates that a time/potential dependent double layer capacity has been entered by the user. The polynomial coefficients describing the dependence of the double layer capacity as function of the electrode potential can be edited by clicking with the right mouse button while the cursor is localized over the input field associated with Cdl (F).

 

1. Scan Parameters

Scan segment, Estart (V), Eend (V), v (V/s)
DigiElch provides a highly flexible definition of the potential scan used in the cyclic voltammetric experiment. The overall scan can be composed of any number of scan segments characterized by starting potential, Estart (V), end-potential, Eend (V) and scan rate, v (V/s). In the case of cyclic voltammetry a scan segment is identical with a half cycle (i.e. forward or backward scan) where the scan rate in each individual scan segment may be different.
tipbulbIn practice the number of applicable scan segments is restricted by the memory capacity of the potentiostat.

Potential steps (V)
By default the experiment is executed with potential steps of 1mV unless the potential steps need to be adjusted such as to match the entered scan rate. Values grater than 1mV are used only if the desired scan rate cannot be reached due to the limited sampling speed of the potentiostat.

tipbulbValues plotted on a grey background are automatically filled in. They are "read only" and cannot be edited/modified. This ensures, for instance, a "smooth scan" where the starting potential of a scan is always equal to the end potential of the previous scan.
 

Removing scan segments:
A scan segment (and all subsequent scan segments) can be removed by entering an empty string into the associated Eend - input filed. For instance, if a user wants to run only the first scan segment, an empty string must be entered into the input field "Eend (V)" associated with the scan index 2.

 

2. Pre-Equilibrium

Disabled , Enabled, Smart
When using the experimental CV in a Data Fitting Project the simulation(s) will be forced to be executed for the selected Pre-Equilibrium option.

3. Diffusion

Semi-Infinite 1D
When using the experimental file in a Data Fitting Project the diffusion will be treated in one space direction either by making use of symmetry properties of the electrode or by neglecting contributions from other space directions. The user should be aware that this approach may lead to a considerable error in the current density when approximating a "small" planar (in fact two-dimensional) electrode in terms of an infinitely large (in fact one-dimensional) electrode.

Finite 1D
When using the experimental file in a Data Fitting Project the simulation referring to this file is executed for a thin layer electrode. When selecting this mode, a dialog field appears that enables the user to enter the Thickness of the thin layer electrode and the right-hand boundary condition can be selected for each species listed in Species.
 
Diffusion_Finite
 

Semi-Infinite 2D
When using the experimental file in a Data Fitting Project diffusion is simulated in two space directions. This option is much more time consuming because diffusion occurring parallel to the electrode surface is not neglected when using this option.

Hydrodynamic
diffusion is simulated for a Rotating Disc Electrode (RDE).  When selecting this option, two dialog fields appear which enable the user to enter the rate of rotation, W(rad/s), and the kinematic viscosity, V(cm²/s).

tipbulbWhen using the experimental CV in a Data Fitting Project the simulation(s) will be forced to be executed for the selected mode of Diffusion and Boundary condition.

 

4. Geometry

Depending on the selected option for Diffusion the following geometry options are available
 

diffusion mode

electrode geometry

input parameter 1

input parameter 2

Hydrodynamic

Planar

electrode Radius (cm)

none

Semi-Infinite 2D

Band

electrode Width (cm)

electrode Length (cm)

"

Disk

electrode Radius (cm)

none

Finite 1D

Planar

electrode Area (cm²)

none

Semi-Infinite 1D

Planar

electrode Area (cm²)

none

"

Spherical (Ro)

electrode Radius (cm)

none

"

Spherical (Hg)

Mass (mg) of mercury drop

none

"

Hemispherical

electrode Radius (cm)

none

"

Cylindrical

electrode Radius (cm)

electrode Length (cm)

"

Hemicylindrical

electrode Radius (cm)

electrode Length (cm)

 

When selecting Spherical (Hg) the user has the choice to specify whether a particular species is going to form an amalgam (i.e. diffusing into the mercury drop) or not (see point 6).

 
tipbulbWhen using the experimental file in a Data Fitting Project the simulation referring to this file will be executed for the specified Geometry.

 

5. Experimental Parameters

Instrumental Parameters

Delay time (s)
The time elapsing before starting the experiment. When working with an automated mercury drop electrode a delay time of a few second is required to minimize the convection effected by the growth of the mercury drop.
 

Pre-Drops
When working with an automated mercury drop electrode n+1 mercury drops are produced (where n is the number of Pre-Drops) but the experiment is executed only at the last drop. Helps to improve the reproducibility of the produced mercury drops.
 

Current Range
The Current Range of the potentiostat used in the experiment. (see Potentiostat's manual for more details)
 

Amplification
The factor with which the originally measured current signal is amplified by the potentiostats hardware. (see  Potentiostat's manual for more details)
 

IE-Filter
Setting of the hardware filter applied to the originally measured current signal. (see  Potentiostat's manual for more details)
 

IE-Stability
The stability setting (applied to the current-to-voltage-converter) of the potentiostat (see  Potentiostat's manual for more details)
 

CA-Speed
The speed setting of the control-amplifier in the potentiostat (see  Potentiostat's manual for more details)
 

Ru-Compensation (Ohm)
Value of the ohmic resistance that will be compensated for by positive feedback (from the output of the current-to-voltage-converter to the input of the control-amplifier).

 

Ru-Measurement

Amplitude (V)
Amplitude of the AC-Signal used for measuring the uncompensated ohmic resistance, Ru (Ohm), and the double layer capacity, Cdl (F).
 

Frequency (Hz)
Frequency of the AC-Signal used for measuring the uncompensated ohmic resistance, Ru (Ohm), and the double layer capacity, Cdl (F).
 

Current Range
The Current Range of the potentiostat with which the measurement of the uncompensated ohmic resistance, Ru (Ohm), and the double layer capacity, Cdl (F) is started. Will be automatically optimized.

 

Amplification
The post amplification factor used for measuring the uncompensated ohmic resistance, Ru (Ohm), and the double layer capacity, Cdl (F).

 

Experimental Conditions

Ru (Ohm)
Uncompensated ohmic resistance which has been measured or entered. When using the experimental CV in a Data Fitting Project the simulation(s) will be forced to be executed for an uncompensated ohmic resistance equal to Ru (Ohm) - Ru-Compensation (Ohm).
 

Cdl (F)
The double layer capacity which has been measured or entered. If the dependence of Cdl (F) on the electrode potential is already known when doing the experiment and expressible in polynomial form it can be entered by clicking with the right mouse button while the cursor is localized over the input field of Cdl (F) :
 
CdDlg
 
Cdl (F) is the constant value of the double layer capacity left over in the limiting case where the dependence of the double layer capacity on the electrode potential expressed by C1, C2, C3 and C4 remains negligibly small. After closing this dialog box only the value of Cdl (F) is displayed in the list of Experimental Conditions but the value of Cdl (F) is written in magenta if one of the coefficients C1, C2, C3, C4 is different from zero. When using the experimental CV in a Data Fitting Project the simulation(s) will be forced to be executed for these values.
 

Temp (K)
When using the experimental CV in a Data Fitting Project the simulation(s) will be forced to calculate the Nernst-factor for this temperature.
 

tipbulbThe values entered for Ru (Ohm) and Cdl (F) will be overwritten each time when executing the Command: Measure IR-Drop & Run or IR-Drop.
 

 

6. Species

Click on the first empty input field headlined Species to add a name for each species for which the analytical concentration is explicitly known when running the experiment(s). When using the experimental CV in a Data Fitting Project the simulation(s) will be forced to use the entered analytical concentration provided a species with exactly the same name is found in the mechanism entered for the Data Fitting Project.
 

Entering species concentrations when mixing different volumes of stock solutions
 

1.Enter the names of the underlying species

StockSolution1

 

 

 

 

2.Click with the right mouse button on the list containing the species names and enter the volumes and concentrations of the stock solutions from which the sample is prepared.
 

StockSolution2
 

3.The concentration referring to this mixture will be displayed in the Species list after closing the dialog box with OK.

 

7. C-Bypass Stabilization

The stabilization level adjusted at this slider bar takes effect only if the reference and counter electrode are connected by a switchable capacitor shown as shown in the following picture (referring to the Reference 600 Misc I/O Connector)

IRKStab

 

 

 

The following capacitors can be recommended:
 

C1 0.1 nF

C2 0.22 nF

C3 0.44 nF

C4 1 nF

C5 2.2 nF

C6 4.7nF

C7 10 nF

 

The optimal value is found by "trial and error". It enables the user to conduct fully IR-compensated CV experiments using scan rates higher than 100 V/s in combination with the CA-Speed level "very fast".

 
Line 7 of the Reference 600 Misc I/O Connector can be used to trigger the generation of a mercury drop for a Controlled Growth Mercury Electrode (see, for instance, the CGME distributed by BASi).