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<strong>XII</strong> <strong>Iberian</strong> <strong>Meeting</strong> <strong>of</strong> <strong>Electrochemistry</strong> & <strong>XVI</strong> <strong>Meeting</strong> <strong>of</strong> <strong>the</strong> Portuguese Electrochemical Society O C 02<br />

Convolutive modelling with Ma<strong>the</strong>matica ® using Oldham-<br />

Mahon-Myland h i (t) functions. C r E q mechanism in C V.<br />

M. J. Barrera-Niebla 1 , M.J. González Morín 1 , M. R. García Hernández 2 ,<br />

D.M. Grandoso Medina 1 , L.C. Fernández Mérida 1<br />

1 Physical Chemistry Department. University <strong>of</strong> La Laguna. La Laguna. 2 Consejería de Presidencia,<br />

Justicia y Seguridad. Gobierno de Canarias.TENERIFE. CANARY ISLANDS. SPAIN.<br />

mbarnie@ull.es<br />

Convolutive Modelling is an important methodology <strong>of</strong> Semiintegral and Convolution<br />

<strong>Electrochemistry</strong> [1]. We model with Ma<strong>the</strong>matica ® s<strong>of</strong>tware, in order to overcome <strong>the</strong><br />

advanced ma<strong>the</strong>matics, <strong>the</strong> I E curves for a C r Eq<br />

mechanism at planar electrodes.<br />

The mentioned methodology employs <strong>the</strong> universal convolution algorithm <strong>of</strong> Oldham<br />

and <strong>the</strong> extended semiintegrals M R (t)<br />

and M P (t)<br />

. The mechanism represented by<br />

k<br />

k<br />

f<br />

<br />

<br />

<br />

S(<br />

soln)<br />

<br />

R(<br />

soln)<br />

R(<br />

soln)<br />

ne P(<br />

soln)<br />

(1)<br />

k'<br />

kb<br />

allows us to infer for k k'<br />

<strong>the</strong> following expression for h R (t)<br />

, namely<br />

<br />

2k<br />

k'<br />

1<br />

2exp ( k k')<br />

t<br />

h R ( t)<br />

<br />

2( k k')<br />

t<br />

<br />

<br />

<br />

2<br />

<br />

2 k t<br />

k'<br />

exp<br />

<br />

k k'<br />

<br />

<br />

<br />

Erfi<br />

3/ 2 <br />

( k k')<br />

<br />

<br />

<br />

k'<br />

t <br />

<br />

Erfi<br />

k k'<br />

<br />

k t <br />

<br />

<br />

k k'<br />

<br />

<br />

required to calculate, with Ma<strong>the</strong>matica ® , <strong>the</strong> single integral <strong>of</strong> equation (2) needed in<br />

<strong>the</strong> convolutive modelling. When k k'<br />

an easier equation is obtained.. These<br />

methodologies let us to obtain <strong>the</strong> files: M R (t)<br />

, M P (t)<br />

, and in duplicate, I (E)<br />

. A very<br />

basic program written for Ma<strong>the</strong>matica ® is reported to model I E curves. We check<br />

<strong>the</strong>se files with those obtained by convolutive modelling with Oldham-Mahon-Myland<br />

g(t)<br />

functions and by digital simulation with DigiSim ® and DigiElch ® . This comparison<br />

was made with <strong>the</strong> assistance <strong>of</strong> SigmaPlot ® s<strong>of</strong>tware. The agreement is excellent. The<br />

methodologies employed are based in <strong>the</strong> following convolutions<br />

dh t<br />

I t M t i ( )<br />

( ) i ( )* i R,<br />

P<br />

(3)<br />

dt<br />

The extended semiintegrals M R (t)<br />

and M P (t)<br />

are connected with electrode surface<br />

concentrations by a linear relation with known parameters. Hence <strong>the</strong> C R ( 0, t)<br />

and<br />

C P ( 0, t)<br />

files are obtained in a straightforward procedure and are complementary with<br />

<strong>the</strong> concentration pr<strong>of</strong>iles C R ( x,<br />

1 t ) and C P ( x,<br />

1 t ) determined by digital simulation.<br />

(2)<br />

Acknowledgements: To Pr<strong>of</strong>essor Keith B. Oldham, Peter J. Mahon and Jan C. Myland.<br />

References<br />

[1] Barrera-Niebla, M.J.. Semiintegral and Convolution <strong>Electrochemistry</strong>. Research line.<br />

Department <strong>of</strong> Physical Chemistry. (2010). La Laguna University. Tenerife. Canary Islands.<br />

September, 811, 2010. ISEL - Lisbon 41

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