8. Fundamentals of Charged Surfaces Moving the reagents Quickly and with Little energy Diffusion electric fields Yo + Charged Surface Y*o + + + X=0 G N* exp kT No 1. Cations distributed thermally with respect to potential 2. Cations shield surface and reduce the effective surface potential G N* exp kT No Yo + Y**o Charged Surface Y*o + + + + + + Y***o + X=0 dx * + dx ** dx *** Surface Potentials zF x n e RT no Cation distribution has to account for all species, i Poisson-Boltzman equation Simeon-Denis Poisson 1781-1840 d o 2 dx 2 Dielectric constant of solution Permitivity of free space zi x F * RT i z FC e i i Charge near electrode depends upon potential and is integrated over distance from surface - affects the effective surface potential d o 2 dx 2 z FC e i * i zi x F RT i Solution to the Poisson-Boltzman equation can be simple if the initial surface potential is small: ze o 1 kT o 50mV x o e x Potential decays from the surface potential exponentially with distance d 2 dx 2 z FC i i o * i e zi i F RT z FC * i i i o 2 zi i F 1 zi i F ...... 1 RT 2 RT Largest term d 2 2 dx Let 2 1 xa 2 F 2 zi Ci* i RT o x F 2 zi Ci* i RT o Then: d 2 x 2 2 dx xa General Solution of: Y x Ae x xa d 2 x 2 2 dx xa Be x xa Because Y goes to zero as x goes to infinity B must be zero Y x Ae x xa Ae x Because Y goes to Y0 as x goes to zero (e0 =1) A must be Y0 thus x o e x Potential decays from the surface potential exponentially with distance When =1/x or x=1/ then x o e 1 o (0.367) The DEBYE LENGTH x=1/ What is ? Yo Charged Surface + + + + + + Y=0.36 Yo + + + X=0 X=1/ Petrus Josephus Wilhelmus Debye 1844-1966 Debye Length 2n z e o kT * 2 2 2Conc N A z e o kT 1 2 2 2 1 2 Does not belong 2 moles 6.02 x10 23 1L 100cm . x10 19 C 2 160218 2 ch arg e 3 3 L mole 10 cm m ch arg e 12 2 23 8 . 85419 x 10 C m Nm 138065 . x 10 J 78.49 o unitless 298 K 2 25 C K N m 100cm J 2 =1/cm 1 2 # 19 2 2 160218 . x 10 2 mole cm 23 23 78.49 o 138065 6.022 x10 ions . x 10 298 25 C z(3.29 x10 7 )(C * ) 1/ 2 Units are 1/cm 1 2 2n * z 2 e 2 zF o kT Debye Length 1 2 z(3.29 x10 )(C ) 7 * 1/ 2 Units are 1/cm Table 2: Extent of the Debye length as a function of electrolyte 1/κ ( ) C(M) 1 3 0.1 9.6 0.01 30.4 0.001 96.2 0.0001 304 In the event we can not use a series approximation to solve the Poisson-Boltzman equation we get the following: ze ze 0 exp 2 kT 1 exp 2 kT 1 Check as Compared to tanh x By Bard exp ze ze 0 exp 2 kT 1 exp 2 kT 1 Ludwig Boltzman 1844-1904 Simeon-Denis Poisson 1781-1840 Set up excel sheet ot have them calc effect Of kappa on the decay Example Problem A 10 mV perturbation is applied to an electrode surface bathed in 0.01 M NaCl. What potential does the outer edge of a Ru(bpy)33+ molecule feel? Debye length, x? z(3.29 x10 7 )(C * ) 1/ 2 Units are 1/cm 108 A X 1/ 30 . 4 A 1(3.29 x10 7 )(0.01) 1/ 2 Since the potential applied (10 mV) is less than 50 can use the simplified equation. Radius of Ru x o e x o e x xz 10e 9 30.4 7.43 The potential the Ru(bpy)33+ compound experiences is less than the 10 mV applied. This will affect the rate of the electron transfer event from the electrode to the molecule. Surface Charge Density The surface charge distance is the integration over all the charge lined up at the surface of the electrode a a o dx 0 d 2 d dx 0 2 dx dx The full solution to this equation is: ze o o (8kT o n o ) sinh( ) 2 kT 1 2 1 2 o 117 . (C*) sinh(19.5z o ) C is in mol/L a Yo Charged Surface + + + + + + Y=0.36 Yo + + + X=0 X=1/ Can be modeled as a capacitor: C d differential d For the full equation 1 2 2 z e 0 n ze o cosh C d 2 kT kT 2 2 Cd 228zC o 1 * 2 Differential capacitance Ends with units of uF/cm2 cosh19.5z o At 25oC, water Conc. Is in mol/L y cosh x 12000 10000 8000 6000 4000 2000 0 -15 -10 -5 0 5 10 15 Can be simplified if (o ~ 25 mV), o o o Specific Capacitance is the differential space charge per unit area/potential Cspecific dq d Ad d A C o A Specific Capacitance Independent of potential For small potentials 1 2 2 z e 0 n ze o cosh C 2 kT kT 2 2 o 120 100 Capacitance 80 60 o 40 20 0 -500 -400 -300 -200 -100 0 E-Ezeta Gouy-Chapman Model 100 200 300 400 500 Flat in this region Henrik Jensen , David J. Fermn and Hubert H. Girault* Received 16th February 2001 , Accepted 3rd April 2001 Published on the Web 17th May 2001 Physical Chemistry Chemical Physics DOI: 10.1039/b101512p Paper Photoinduced electron transfer at liquid/liquid interfaces. Part V. Organisation of water-soluble chlorophyll at the water/1,2-dichloroethane interface� Laboratoire d'Electrochimie, D�partement de Chimie, Ecole Polytechnique F�d�rale de Lausanne, CH-1015, Switzerland Real differential capacitance plots appear to roll off instead of Steadily increasing with increased potential Yo + Exponential in the thermally equilibrated or diffuse layer CHelmholtz or Stern Charged Surface Linear drop in potential first in the Helmholtz or Stern specifically adsorbed layer + + + Hermann Ludwig Ferdinand von Helmholtz 1821-1894 + + + + + X=0 x2 Cdiffuse O. Stern Noble prize 1943 Capacitors in series 1 2 2 z e 0 n ze o cosh CDiffuse 2 kT kT 2 2 o C o A Helmholtz or Stern Cseries 1 Cseries Wrong should be x distance of stern layer 1 1 1 1 ...... C1 C2 CN Cseries 1 1 1 ...... C1 C2 CN For large applied potentials and/or for large salt concentrations 1. ions become compressed near the electrode surface to create a “Helmholtz” layer. 2. Need to consider the diffuse layer as beginning at the Helmholtz edge x2 1 C 0 1 1 2 2 z 2 e 2 0 n o ze o cosh 2 kT kT Capacitance Due to Helmholtz layer Capacitance due to diffuse layer 0.71 0.7 0.69 Capacitance 0.68 0.67 0.66 0.65 Deviation Is dependent upon The salt conc. 0.64 0.63 -500 -400 -300 -200 -100 0 E-Ezeta 100 200 300 400 500 The larger the “dip” For the lower The salt conc. Create an excel problem And ask students to determine the smallest Amount of effect of an adsorbed layer Experimental data does not Correspond that well to the Diffuse double layer double capacitor model (Bard and Faulkner 2nd Ed) Physical Chemistry Chemical Physics DOI: 10.1039/b101279g Complex formation between halogens and sulfoxides on metal surfaces Paper * and Andrew A. Gewirth pacitance�potential curve for the Au(111)/25 mM KI in DMSO interface w Department of Chemistry, and Frederick Seitz Materials Research Laboratory, Uni rsity of Illinois at Urbana-Champaign, Urbana, IL, 61801, USA Received 8th February 2001 , Accepted 20th April 2001 Published on the Web 1st June 2001 Siv K. Si e Model needs to be altered to account For the drop with large potentials This curve is pretty similar to predictions except where specific Adsorption effects are noted Graphs of these types were (and are) strong evidence of the Adsorption of ions at the surface of electrodes. Get a refernce or two of deLevie here Charged Surface Yo Introducing the Zeta Potential Imagine a flowing solution along this charged surface. Some of the charge will be carried + away with the flowing solution. + + + + + + + + Yzeta Introducing the Zeta Potential, given the symbo lz Yo Shear Plane Flowing solution Charged Surface + + Sometimes assumed zeta corresponds to Debye Length, but Not necessarily true + + + + + + + z C 1 2 exp 1 C 2 The zeta potential is dependent upon how the electrolyte concentration compresses the double layer. , are constants and sigma is the surface charge density. Shear Plane can be talked about in two contexts Charged Surface Yo Shear Plane + + + + ++ + + + + + + + + + + + + In either case if we “push” the solution along Shear a plane we end up with charge separation which Plane leads to potential + + + Particle in motion Streaming Potentials From the picture on preceding slide, if we shove the solution Away from the charged surface a charge separation develops = potential Y oz P solution resis tan ce m z zeta potential kg vis cos ity m s Sample problem here Reiger- streaming potential apparatus. Can also make measurements on blood capillaries In the same way, we can apply a potential and move ions and solution Anode Vapp Charged Surface Yo Jm + + + + + + + + X=0 + Jo Jm Cathode + Movement of a charged ion in an electric field Electrophoretic mobility f i v zi e i applied electric field f frictional drag 6r v electrophoretic velocity The force from friction is equal to the electric driving force The frictional drag comes about because the migrating ion’s atmosphere is moving in the opposite direction, dragging solvent with it, the drag is related to the ion atmosphere f frictional 6r vis cos ity r ionic radius ion velocity Drag Force f electrical zi e Electric Force Direction of Movement Ion accelerates in electric field until the electric force is equal and opposite to the drag force = terminal velocity At terminal velocity f frictional f electric 6r zi e zi e 6r The mobility is the velocity normalized for the electric field: zi e ui 6r vi zi e zi e uep f 6r Stokes-Einstein equation Frictional drag 6r (Stokes Law) r = hydrodynamic radius Typical values of the electrophoretic mobility are small ions 5x10-8 m2V-1s-1 proteins 0.1-1x10-8 m2V-1s-1 Sir George Gabriel Stokes 1819-1903 Reiger p. 97 Insert a sample calculation When particles are smaller than the Debye length you get The following limit: 2 oz uep 3 Remember: velocity is mobility x electric field Reiger p. 98 What controls the hydrodynamic radius? - the shear plane and ions around it Compare the two equations for electrophoretic mobility 2 oz f oz uep 3 foz zi e 6r zi e uep 6r r zi e f oz 6 Where f is a shape term which is 2/3 for spherical particles Relation of electrophoretic mobility to diffusion Thermal “force” kT D f Frictional drag 6r kT kT D f 6r zi e ui 6r kT kT D uelectrophoretic migration f ze Measuring Mobilities (and therefore Diffusion) from Conductance Cells + - + + + - - - + - + + + - To make measurement need to worry about all the processes Which lead to current measured - Ac Voltage + Solution Charge Motion = resistance + Charging + + RO RO Electron Transfer + - + + + Ct Ct Zf1 Rs Zf2 An aside 1 Z f Rct 1 Cs 2 2 1 1 Cs 2 2 1 2 diffusion Related to ket Electron transfer at electrode surface can be modeled as the Faradaic impedance, Z2 Ct Ct Zf1 Rs Zf2 Solving this circuit leads to Zf1 Zf 2 RT Rs Zf1 Zf 2 1 1 Ct Ct 1 1 RT Rs 1 1 1 1 Z f 1( ) Ct Z f 2( ) Ct Applying a high frequency, w, drops out capacitance and Faradaic Impedance so that RT=Rs What frequency would you have to use To measure the solution resistance between Two 0.5 cm2 in 0.1 M NaCl? Cspecific A d d ( o ) o d d z(329 . x10 )(C ) 7 * 1/2 1 104 . x10 m C Cspecific A Ao 7 Check Calculation To show that It is cm converted to C Cspecific A Ao 2 2 1 m C 78.54 8.854 x1012 C Ao 104 . x107 2 x0.5cm2 x 100cm m J m 2 2 1 m C 7 2 12 C Ao 104 . x10 . x10 2 x0.5cm x 78.54 8854 100cm m J m C 7..2 x10 7 2 C2 C 7 C 7..2 x10 7..2 x107 7..2 x107 F J CV V The predicted capacitance of both electrodes in 0.1 M NaCl would Be 0.72 microfarads For the capacitive term to drop out of the electrical circuit We need: 1 1 Ct 1 1 6 14 . x 10 Ct 7.2 x10 7 The frequency will have to be very large. Solution Resistance Depends upon Cell configuration A length Resistivity of soln. R A Sample calculation in a thin layer cell Resistance also depends upon the shape Of an electrode Disk Electrode R 4a a is the radius Spherical electrode R 4a Hemispherical electrode R 2a Scan rate 1000 V/s at two different size electrodes for Thioglycole at Hg electrode From Baranski, U. Saskatchewan Conductivity is the inverse of Resistance k RA 1 Resistivity and conductivity both depend upon Concentration. To get rid of conc. Term divide k C 1 C RCA molar conductivity A plot of the molar conductivity vs Concentration has a slope Related to the measurement device, and an intercept related to The molar conductivity at infinite dilution o s tan dard molar conductivity This standard molar conductivity depends upon the solution Resistance imparted by the motion of both anions and cations Moving in the measurement cell. t o t o Where t is a transference number which accounts for the Proportion of charge moving Transference Numbers can be Measured by capturing The number of ions Moving. Once last number needs To be introduced: The number of moles of ion Per mole of salt o v v Compute the resistance of a disk electrode Of 0.2 cm radius in a 0.1 M CaCl2 solution v v o 2Ca 1Cl 2 o 2 m 0.00763 mol 1 2 m 0.0119 mol 2 m 0.02716 mol m2 1 1 0.02716 3 mol C mol L 100cm 01 . 3 3 L 10 cm m 1 m2 mol L 100cm 0.02716 . 01 3 3 mol L m 10 cm 3 0.368 m The resistance is computed from 0.368 m R 4.6 01 . m 4a 4 0.2cmx cm Remember – we were trying to get to mobility From a conductance measurement!!!! i ui zi F o Also remember that mobility and diffusion coefficients are related o kT kT oi kToi 7 i J mol D u 2 2.66x10 ze ze zF z eF z 2 C2 D 2.66x107 oi J mol z2 C2 We can use this expression to calculate Diffusion coefficients D 2.66x107 D3 2.66 x107 oi J mol z2 C2 2 m 302.7 x104 2 J mol m J 10 mol 8.92 x10 2 2 ( 3) C C 2 m2 J VC m2 2 Vs s C J C D4 2.66 x107 2 m 442 x104 2 J mol m 10 mol 7 . 34 x 10 s ( 4) 2 C2 Fe(CN)63- diffusion coefficient is 9.92x10-10 m2/s Fe(CN)64- diffusion coefficient is 7.34x10-10 m2/s The more highly charged ion has more solution solutes around It which slows it down. How does this effect the rate of electron transfer? Activation energy * ket el Probability factor kT Z ~ 2m G Z exp kT Collisional factor 1 2 Where m is the reduced mass. Z is typically, at room temperature, 104 cm/s G o G * Free energy change 2 4 in out work required to change bonds And bring molecules together a D donor radii a A acceptor radii op optical dielectric cons tan t s regular dielectric cons tan t e electron ch arg e out e 2 1 1 1 1 1 4o 2a D 2a A rDA op s Formal potential G eE ( w w ) o o p r Work of bringing ions together a A za z pe2 ea D e rDA ( w p wr ) U r e 40 1 a D 1 a A The larger kappa the smaller the activation energy, the closer Ions can approach each other without work When one ion is very large with respect to other (like an electrode) Then the work term can be simplified to: ( w p wr ) Ur Yze