wave initiation in the ferroin /ferriin- catalysed bz reaction with visible light

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Wave Initiation in the Ferroin/Ferriin-Catalysed BZ Reaction with Visible Light Rita Tóth and Vilmos Gáspár Institute of Physical Chemistry University of Debrecen 4010 Debrecen, P.O. Box 7, Hungary Andrew Belmonte and Megan C. O'Connell Department of Mathematics Pennsylvania State University, University Park, PA 16802 USA Annette Taylor and Stephen K. Scott School of Chemistry University of Leeds, Leeds LS2 9JT, UK The illum ination isprovided in a region ofm em brane sufficiently long afterthepassage ofan oxidation front red spot 6 safterlaseroff increasing blue spot t = 18 and 32 s laseron for5 s The illum ination isprovided closerto the oxidation front red spot im mediately afterlaseroff increasing bluespiral t = 10 and 14 s sustained spiral t = 62 s laseron for3 s red spot 6 safterlaseroff increasing blue spiral t = 16 and 46 s sustained spiral t = 190 s Illum ination in theresting orrecovered statesdoesnot lead to initiation ofoxidation structures b)high loading M echanism proposal Thisband extendsto the w avelength ofthe light (632.8 nm )used here. T he m ore likely absorber isferriin. Ferroin (red, reduced form ofthe catalyst): m ax = 510 nm , m ax = 11100 m ol -1 dm 3 cm -1 Ferriin (blue,oxidized form ofthe catalyst): m ax = 590 nm , m ax = 600 m ol -1 dm 3 cm -1 Photoreduction ofFe(phen) 3 3+ proceedsatthisw avelength w ith a quantum efficiency ofca. 2 10 2 in 0.05 M H 2 SO 4 in the presence of organic reducing species. [6] The reduction isbelieved to proceed through the form ation ofaligand- m etal charge transfer(LM C T)excited state w ith electron transferfrom the solvent. Ferriin + h Ferroin Introduction Belousov-Z habotinsky (B Z)reaction: achem ical excitable m edium E ffectsoflighton the B Z system : •U V illum ination suppresses oscillationsin the cerium -catalysed system [1] •U V illum ination initiates w aves in the ferroin-catalysed system [2] •Ferroin-and Ru(bpy) 3 2+ catalysed system s are sensitiveto visiblelight, cerium -catalysed system isunaffected [3] •V isible light inhibitsspiralsand changestheirbehavior[4]. Experim ents •V isiblelightofwavelength = 632,8 nm , H e-N e (red)laser •circularpolysulfonem em brane (G elm an) pore size0.45 m , 47 m m diameter loaded w ith bathoferroin •B Z reaction m ixture w ithout catalyst: [m alonic acid]= 0.213 M , [N aB rO 3 ]= 0.213 M , [H 2 SO 4 ]= 1.596 M , [N aBr]= 0.162 M , and [(N H 4 ) 2 SO 4 ]= 0.64 M . The m em brane isin the ‘resting’steady state laseron for5 s(illum inated area ca. 2 m m 2 ) red spot 6 safterlaseroff increasing blue spot t = 16 and 26 s Illum inating a sm allregion ofthe m em brane a)low loading x:autocatalyst(H BrO 2 ) z:oxidised form ofthe catalyst(ferriin) : dim ensionlessrate coefficient forthephotoreduction step :light intensity Explanation oftheeffectofvisible light M odified Tyson-Fifem odel z x dt dz q x q x fx x x dt dx )] ( 1 [ , ) ( ) ( ) 1 ( x z Increasing C hanging the intensity ofillum ination changes the position of z-nullcline ( dz/dt = 0)defined as: ) ( 1 x z laser off laser on laser off x z x z x z steady-state low value of z (red) low value of x new steady-state low ervalue of z (m ore red) slightly increased value of x butlessthan threshold Thesystem returns to the originalsteady state. N o excitation in the centre ofillum ination. > 0 laser off laser on laser off x z x z x z steady-state low value of z (red) low value of x new steady-state low ervalue of z (m ore red) highervalue of x over the threshold The system returns to the originalsteady state. A n excitation occurs in the centre of illum ination, and a chem icalw ave isinitiated. >> 0 [1]V .A . Vavilin, A . M . Zhabotinsky, and A .N . Zaikin, Russ. J . Phys. Chem., 1968, 42 , 1649. [2]H .Busseand B . Hess, Nature, 1973, 244 , 203. [3]V .Gáspár, G . Bazsa,and M .T.Beck, Z. Phys. Chem. (Leipzig), 1983, 264 , 43. [4]O . Steinbock, V.Zykov,and S.C. M üller, Nature, 1993, 366 , 322. [5]A . Belm onteand J.-M . Flesselles, Phys. Rev. L ett., 1996, 77 , 1174. [6]V . Balzani and V. C arassiti, P hotochemistry of C oordination C ompounds, A cadem ic Press,London, 1970. R eferences

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Wave Initiation in the Ferroin /Ferriin- Catalysed BZ Reaction with Visible Light. Rita Tóth and Vilmos Gáspár Institute of Physical Chemistry University of Debrecen 4010 Debrecen, P.O. Box 7, Hungary. Annette Taylor and Stephen K. Scott School of Chemistry University of Leeds, - PowerPoint PPT Presentation

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Page 1: Wave Initiation in the  Ferroin /Ferriin- Catalysed BZ Reaction with Visible Light

Wave Initiation in the Ferroin/Ferriin-Catalysed BZ Reaction with Visible LightRita Tóth and Vilmos GáspárInstitute of Physical ChemistryUniversity of Debrecen4010 Debrecen, P.O. Box 7, Hungary

Andrew Belmonte and Megan C. O'ConnellDepartment of MathematicsPennsylvania State University,University Park, PA 16802 USA

Annette Taylor and Stephen K. ScottSchool of ChemistryUniversity of Leeds,Leeds LS2 9JT, UK

The illumination is provided in a region of membranesufficiently long after the passage of an oxidation front

red spot6 s after laser off increasing blue spot

t = 18 and 32 s

laser on for 5 s

The illumination is provided closer to the oxidation front

red spotimmediatelyafter laser off

increasing blue spiralt = 10 and 14 s sustained spiral

t = 62 s

laser on for 3 s

red spot6 s after laser off

increasing blue spiralt = 16 and 46 s

sustained spiralt = 190 s

Illumination in the resting or recovered states does not lead to initiation of oxidation structures

b) high loading

Mechanism proposal

This band extends to the wavelength of the light (632.8 nm) used here. The more likely absorber is ferriin.

Ferroin (red, reduced form of the catalyst):max = 510 nm, max = 11100 mol-1 dm3 cm-1

Ferriin (blue, oxidized form of the catalyst):max = 590 nm, max = 600 mol-1 dm3 cm-1

Photoreduction of Fe(phen)33+ proceeds at this wavelength with a

quantum efficiency of ca. 2 10 2 in 0.05 M H2SO4 in the presence oforganic reducing species. [6]

The reduction is believed to proceed through the formation of a ligand-metal charge transfer (LMCT) excited state with electron transfer fromthe solvent.

Ferriin + h FerroinFerriin + h Ferroin

Introduction Belousov-Zhabotinsky (BZ) reaction: a chemical excitable medium

Effects of light on the BZ system:• UV illumination suppresses oscillations in the cerium-catalysed system [1]• UV illumination initiates waves in the ferroin-catalysed system [2]• Ferroin- and Ru(bpy)3

2+ catalysed systems are sensitive to visible light, cerium-catalysed system is unaffected [3]• Visible light inhibits spirals and changes their behavior [4].

Experiments• Visible light of wavelength = 632,8 nm, He-Ne (red) laser• circular polysulfone membrane (Gelman) pore size 0.45 m, 47 mm diameter loaded with bathoferroin

• BZ reaction mixture without catalyst: [malonic acid] = 0.213 M, [NaBrO3] = 0.213 M, [H2SO4] = 1.596 M, [NaBr] = 0.162 M, and [(NH4)2SO4] = 0.64 M.

The membrane is in the ‘resting’ steady state

laser on for 5 s (illuminated area ca. 2 mm2 )

red spot 6 s after laser off

increasing blue spott = 16 and 26 s

Illuminating a small region of the membranea) low loading

x: autocatalyst (HBrO2)z: oxidised form of the catalyst (ferriin): dimensionless rate coefficient for the photoreduction step : light intensity

Explanation of the effect of visible lightModified Tyson-Fife model

zxdtdz

qxqxfxxx

dtdx )](1[,

)()()1(

x

zIncreasing

Changing the intensityof illumination changes the position of z-nullcline (dz/dt = 0) defined as:

)(1

xz

laser off laser on laser off

x

z

x

z

x

z

steady-statelow value of z (red)low value of x

new steady-statelower value of z (more red)slightly increased value of xbut less than threshold

The system returns tothe original steady state.No excitation in the centreof illumination.

> 0

laser off laser on laser off

x

z

x

z

x

z

steady-statelow value of z (red)low value of x

new steady-statelower value of z (more red)higher value of xover the threshold

The system returns tothe original steady state.An excitation occurs in the centre of illumination,and a chemical wave is initiated.

>> 0

[1] V. A. Vavilin, A. M. Zhabotinsky, and A. N. Zaikin, Russ. J. Phys. Chem., 1968, 42, 1649. [2] H. Busse and B. Hess, Nature, 1973, 244, 203. [3] V. Gáspár, G. Bazsa, and M. T. Beck, Z. Phys. Chem. (Leipzig), 1983, 264, 43. [4] O. Steinbock, V. Zykov, and S. C. Müller, Nature, 1993, 366, 322. [5] A. Belmonte and J.-M. Flesselles, Phys. Rev. Lett., 1996, 77, 1174. [6] V. Balzani and V. Carassiti, Photochemistry of Coordination Compounds, Academic Press, London, 1970.

References