Electrode kinetics in cyanide silver-plating electrolytes at different surface coverages by lead adatoms

Effective values of exchange current i ₀, cathodic and anodic transfer coefficients and , and cathodic and anodic reaction orders with respect to cyanide ions (P _c, P _a) are measured in cyanide silver-plating electrolytes at different surface coverages by lead adatoms . With increasing coverage, i ₀ and increase from 5 × 10^–5 A cm^–2 and 0.24 in pure solutions to 8 × 10^–5 A cm^–2 and 0.3 at = 0.4, with P _c and P _a hardly altering. The cathodic process markedly accelerates at = 0.6, while at 0.5 the kinetics of the cathodic process is unstable. Different effects of lead adatoms on cathodic and anodic gold and silver plating in cyanide solutions are due to lead salts not affecting the metal substrate dissolution mechanism in the latter case.__________Translated from Elektrokhimiya, Vol. 41, No. 4, 2005, pp. 468–474.Original Russian Text Copyright © 2005 by Bek, Shuraeva.     

Properties of aqueous salt solutions of poly(ethylene oxide). Cloud points, θ temperatures

The determination of the properties of aqueous salt solutions of poly(ethylene oxide) has been extended to the cloud point, and temperature measurements have been made at several concentrations for various salts (flourides, iodides, acetates, formates, phosphates, bromides, thiosulfates and perchlorates). The resulting dependency of the critical temperatures (mostly between 290–350 K) on the molar concentration can be expressed as sequences showing the decreasing effect of anion species or cation species in salting out the polymer. The decreasing order of effectiveness of the anions in reducing the temperature is PO ₄ > HPO ₄ > S₂O ₃ > H₂PO ₄ ^– >F^– > HCOO^– > CH₃COO^– > Br^– > I^–. The order for cations is K⁺ Rb⁺ Na⁺ Cs⁺ > Sr⁺⁺ > Ba⁺⁺ Ca⁺⁺ > NH ₄ ⁺ > Li⁺. The changes brought about in temperatures by the salts were found to be the results of the changes taking place in the hydrophilic and hydrophobic interactions among polymer, solvent and additive salts and of the change of water structure by structure making or structure breaking ions, and of the influence of salts on the hydration sheath of the polymer.     

Investigation of the electric moments of AgI particles in aqueous solutions by electric birefringence

Summary Aqueous suspensions of AgI were studied by the electric birefringence method. The rotatory diffusion constant and the relation between two electric moments of the particles (defined by the ratio ) were determined from the dependence of the electric birefringence on the frequency of the applied field (=229s ^–1; =2,37). These parameters were also calculated from the electric birefringence data in rapidly reversed electric pulses. The obtained values are=237s ^–1 and =1,09. The correspondence of the-values is satisfactory. The discrepancy of the -values may be due to the polydispersity of the investigated suspension. The dependence of electric birefringence on the frequency of the applied field, the difference between the initial slopes of the curvesn/E ₌ ² andn/E _~ ² and the type of the birefringence at field reversal show that the orientation of the AgI particles is due to the interaction of two electric moments with the applied field, which are directed along the larger dimension of the particles. One of both electric moments is the induced dipole moment connected with the displacement of the ions in the double electric layer. The other moment shows a slow relaxation between 10 Hz and 1 kHz and may be related to either the permanent or a slow induced dipole moment.

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Zusammenfassung Es wurden wäßrige AgI-Suspensionen mit Hilfe der elektrischen Doppelbrechung untersucht. Die Rotationsdiffusionskonstante und die Beziehung —definiert als Verhältnis - zwischen zwei elektrischen Momenten der Teilchen wurden aus der Abhängigkeit der elektrischen Doppelbrechung von der Frequenz des angelegten Feldes bestimmt (=229s ^–1;=2,37). Diese Parameter wurden auch aus Messungen der elektrischen Doppelbrechung im elektrischen Feld mit rechteckförmigen Impulsen wechseln der Polarität berechnet. Die erhaltenen Werte,=237s ^–1 und =1,09, stimmen im Fall gut, im Fall schlecht überein, was auf die Polydispersität der untersuchten Dispersionen zurückgeführt werden kann. Aus der Abhängigkeit der elektrischen Doppelbrechung von der Frequenz des angelegten Feldes, aus der Differenz zwischen den Anfangssteigungen der Kurvenn/E ₌ ² undn/E _~ ² und aus dem Verhalten der Doppelbrechung bei rechteckförmigen Pulsen wechselnder Polarität geht hervor, daß die Orientierung der AgI-Partikel von der Wechselwirkung zweier elektrischer Momente mit dem angelegten elektris chen Feld herrührt, die beide mit der Richtung der längeren Achse der Teilchen übereinstimmen. Eines der beiden Momente ist das induzierte Dipolmoment und kommt durch eine sehr schnelle Platzverschiebung der Ionen in der elektrischen Doppelschicht zustande. Das andere Moment zeigt eine langsame Relaxation im Bereich 10 Hz bis 1 kHz und kann entweder mit dem permanenten Dipolmoment oder mit einem langsamen induzierten Dipolmoment in Zusammenhang gebracht werden.

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With 4 figures and 1 table     

Kinetic Parameters of Gold Dissolution in Cyanide Solutions: The Effect of Complex Cyanide Ions of Mercury

The kinetics of the gold dissolution in cyanide solutions is studied at constant values of the coverage () of the gold surface by mercury atoms. The constancy of is ensured by maintaining an identical value of the duration (t) of contact of electrode with solution (after renewing its surface by cutting off a thin surface layer of metal) at a potential of –1.3 V, at which the discharge of mercury ions is limited by their diffusion to the electrode. At t = const kinetic dependences of the gold dissolution process correspond to the Tafel equation. Effective values of exchange current i ₀, transfer coefficient , and reaction order by cyanide ions P are determined. With increasing value of their magnitude increases from values 10^–5 A cm^–2, 0.1, and 0.17 that are characteristic of purely cyanide solutions (composition 0.1 M KCN, 0.1 M KOH, and 0.01 M KAu(CN)₂) to i ₀ 2 × 10^–4 A cm^–2, = 0.46, and P 1 at t = 270 s. These results are compared with the data obtained earlier during similar investigations in solutions containing thallium, lead, and bismuth. Common and individual features in the behavior of mercury-containing electrolytes are revealed. It is shown that the possible mechanism of the acceleration of the gold dissolution process in the presence of catalytically active atoms, which had been proposed in these works, may be used also for explaining the action of mercury atoms on this process.     

Effects of adsorbed bismuth on Si(001) surface electronic states

It is shown that depositing Bi on an Si(001) surface fills the free broken-bond surface states, whose concentration decreases linearly as the bismuth coating 8 increases up to _st, = 0.6 monolayer. The bismuth desorption activation energy is constant < _st, (E_d = 2.77 ± 0.1 eV) and decreases for > _st.Taras Shevachenko Kiev National University, ul. Vladimirskaya 64, 252601 Kiev-17, Ukraine. Translated from Teoreticheskaya i Éksperimental'naya Khimiya, Vol. 32, No. 3, pp. 168–171, May–June, 1996. Original article submitted September 19, 1995.     

Synthesis and Crystal Structure of trans-Rb2[Pd(NO2)2Cl2]. Structure Refinement of Na2[Pd(NO2)4]

The reaction products of palladium(II) nitration with sodium nitrite in the presence of rubidium salts are described. The crystal structure of rubidium dinitrodichloropalladoate(II) — trans-Rb₂[Pd(NO₂)₂Cl₂] — has been studied (KUMA automatic diffractometer, MoK radiation, graphite monochromator, /2 scan mode for 2 < 30°, 758 experimental reflections, R = 0.030; R = 0.023 for I>2(I)). Crystal data: a = 15.123(3), b = 7.750(2), c = 7.776(2) , V = 911.4(4) ³, space group Cmca, Z = 4, d _calc = 3.209 g/cm³. The structure consists of [Pd(NO₂)₂Cl₂]^2– complex anions and Rb⁺ cations. The planar square coordination of the Pd atom is completed to distorted octahedral by the chlorine atoms of the neighboring complexes at Pd...Cl distances of 3.18 . Chains of complexes with alternating orientations are formed. The geometrical characteristics of the complex anions, the coordination polyhedra of the cations, and the heavy atom sublattice are analyzed. The crystal structure of Na₂[Pd(NO₂)₄] has been refined, and refinement data are given.     

Evaluation of energy distribution on a heterogeneous surface from heat of adsorption and its application to the ammonia/Na-Y zeolite system

The— function (energy level function) which represents surface heterogeneity was derived from theq— function (experimental heat function) in the case of reversible adsorption. The Langmuir equation was extended and applied to the procedure of calculations. An iterative calculation led to the most probable— function by setting theq— function and adsorption temperature. As an example for actual cases, the— function of Na-Y zeolite was calculated from theq— function obtained by the measurement of heats of adsorption of ammonia at 373 K. The— function thus derived seemed to be consistent with the positional distribution of sodium ions.     

Adsorption Isotherm Accounting for the Electrode Elasticity: Special Solutions

The single-phase adsorption on a solid electrode out of a dilute solution is investigated. As a continuation of the previous paper, on the basis of the complete electrocapillarity equation, an adsorption isotherm equation is derived and supplemented by equations of compatibility of the physical quantities. The equations contain a new parameter, , which is a derivative of the dimensionless surface adsorbate concentration by the relative variation of the electrode surface area. Their solution is obtained in relation to the dimensionless charge density of the electrode surface q for the case of = (). As a result of employing a linear model for q by , the problem of determination of the unknown model functions is reduced to common differential equations that use the capacitance or estance curves as the boundary conditions. In the first case, we suggest to calculate the unknown integration parameter by the method of mathematical optimization, employing coulometric data.     

Kinetics of Gold Electrodeposition from Cyanide Electrolytes at a Monitored Surface Coverage by Thallium Atoms

A procedure for measuring kinetic parameters of gold electrodeposition in the presence of catalytically active thallium(I) ions while monitoring the coverage of the gold surface by thallium adatoms, , is described. The procedure accounts for the duration of contact between a freshly renewed surface of gold and a thallium-containing solution and assumes that the incorporation rate of thallium adatoms is proportional to and the current density of gold electrodeposition. At = const, kinetic dependences correspond to the Tafel equation. Values of and i ₀ increase with . At = 0.3, 0.6 and i ₀ 3 × 10^–4 A cm^–2, which conforms to values calculated from anodic curves obtained in similar conditions.     

Approximate formulas for the characteristics of interelectronic angle densities

The accuracies of approximate formulas are examined for several characteristics of the interelectronic angle density A(₁₂), where ₁₂ (0₁₂) is the angle subtended by the position vectors r₁ and r₂ of two electrons. Numerical results for 102 atoms show that simple approximations have sufficient accuracies for the moments with n=1–4, the central moments _n with n=2, 4, and the kurtosis, when measured by the absolute and relative errors. For heavy atoms, however, the relative errors for the third central moment ₃ and the skewness are large.     

Crystal Structure of NH4NaTiF6and Internal Mobility of the Complex Anions

Single crystals of NH₄NaTiF₆are studied by X-ray diffraction analysis (automated diffractometer, MoK radiation, graphite monochromator, sin/ 1.0 Å^–1, 1566 reflections with I> 3(I), anisotropic least squares method to R= 0.045 and R _w= 0.040). The compound belongs to the NaRbSnF₆structural type. The types of internal motions of the complex ions NH₄ ⁺and TiF₆ ^2–are determined in the temperature range 200–500 K and compared with the motion of ionic groups in (NH₄)₂TiF₆and Na₂TiF₆crystals.     

Interelectronic angle densities of atoms in momentum space

For the 102 atoms from He to Lr in their ground states, the Hartree–Fock interelectronic angle densities,¯A(¯₁₂), in momentum space are reported, where ¯₁₂ is the angle between the momentum vectorsp₁ and p₂ of two electrons. In the first three atoms, He–Be, ¯A(¯₁₂) is found to be uniform independent of ¯₁₂, while in the remaining 99 atoms,¯A(¯₁₂) is larger for a large ¯₁₂ than for a small ¯₁₂. Accordingly, the average interelectronic angles in momentum space are 90° precisely for the three atoms and greater than 90° for the 99 atoms.     

Mechanical properties of oriented fibres of semicrystalline polymers based upon orientation function from optical properties

The computation of the orientational averages is a great problem in the case of semicrystalline polymers. In a previous communication [1] it has been shown that sin=f() sin describes the orientational changes satisfactorily for a certain class of polymers. In this paper some alternative deformation schemes are also discussed. It has been concluded that birefringence provides a useful guideline in the choice of a deformation scheme.     

2-Dimensional atomic arrangements of Te on Pt(111) whose coverage is higher than 0.25+

Presented is an in-situ electrochemical STM study on the structural evolution of Te layer on Pt(111) whose coverage is higher than 0.25. The irreversibly adsorbed oxygenated Te layer was reduced to a rectangular (2×3) adlayer of elemental Te (_Te=0.25). As additional Te was deposited underpotentially onto the Te-covered Pt(111) surface in a TeO₂-saturated 0.05 M H₂SO₄ solution, the surface structure of Te evolved from the rectangular (2×3) (_Te=0.25) to a rectangular c(2×3) (_Te=0.50) via a rectangular c(3×3) (_Te=0.33). The adsorbed elemental Te was mobile enough to compress the superlattice structure to denser ones, so that the resulting Te layer became electrochemically inactive in the potential range below 0.55 V.Dedicated to Professor György Horányi, Hungary, on the occasion of his 70th birthday.     

Lower critical solution temperature (LCST) and theta temperature of aqueous solutions of nonionic surface active agents of various polyoxyethylene chain lengths

Cloud points of aqueous solutions of homogeneous poly(oxyethylene)dodecyl ether derivatives (C₁₂(OE)_n: n=2–8) and the apparent theta temperatureT ^ap were determined from the abrupt changes in optical transmittance and the temperature dependence of the second virial coefficient obtained by light scattering measurements. It was found that the lower critical solution temperature (LCST) shifts to a lower temperature and lower concentration as the number of oxyethylene units in a molecule decreases. Because of this behavior of LCST, the modified Flory-Schultz plot of phase separation was applied to the present nonionic surfactant-water system, and its theta temperature obtained. The dependence ofT ^ap on the number of oxyethylene units suggests that the polyoxyethylene chain has different effects on the solubility of C₁₂(OE)_n in water forn less than or equal to 3 from those forn greater than or equal to 4.     

A calorimetric investigation into copper–arginine and copper–alanine solid state interactions

Complexes of formula CuCl₂ · 2arg and CuCl₂ · 4ala (arg = arginine; ala = alanine) were prepared at room temperature by a solid state route. The metal–amino acid solid state interactions were studied by i.r. spectroscopy and solution calorimetry. For both complexes, participation of the carboxylate group as well as nitrogen in coordination are inferred, based on the i.r. data. For the copper–arginine compound, the calculated thermochemical parameters are: _rH_m = –114.9 ± 1.42 and _fH_m = –1608.3 ± 11.6 kJ mol^–1. For copper–alanine compound, a complete set of thermochemical parameters were calculated: _rH_m = –18.0 ± 0.9; _fH_m = –2490.4 ± 4.3; _DH_m = 597.2 ± 17.7; _MH_m = 771.9 ± 18.7; _gH_m = 627.1 ± 22.3 and D (Cu–L) = 156.8 ± 5.7 kJ mol^–1. Based on _rH_m and dissolution enthalpy values, a stronger intermolecular solid state interaction can be inferred for the arginine complex, than for the alanine one complex, probably due to the formation of intermolecular hydrogen bonds in the former.     

Peroxidase oxidations of hydroquinone and p-cresol in AOT reversed micelles

The enzymatic activities of horseradish peroxidase solubilized in reversed micelles of bis(2-ethylhexyl)sodium sulfosuccinate formed in octane at various _o values ( _o=[H₂O]/[AOT]) were investigated by studying the catalytic oxidation of hydroquinone and p-cresol. These enzymatic reactions obeyed Michaelis-Menten kinetics. The turnover number of the enzymatic reaction of hydroquinone solubilized in the water pool increased with a decrease in _o value. On the other hand, the dependence of the turnover number of the enzymatic reaction of p-cresol solubilized in octane on the _o value was similar to that in the case of hydroquinone, although even at higher _o values the turnover number was smaller than that in water. Furthermore, it was suggested by spectrophotometric and circular dichroism measurements that the conformational change of enzyme induced the change in enzymatic activity.     

Analysis of the Probability of the Mössbauer Effect in Iron(III) β-Diketonates

The probability of the Mössbauer effect f has been evaluated and the Debye temperatures of intermolecular vibrations _M at 295 and 78 K have been determined for ten Fe(III) -diketonates, which are complexes of molecular type. Variation of _M with temperature and molecular mass M has been found; in the latter case, _M decreases as M increases. As a result of this antibatic change in _M and M, the effect of a decreased energy of intermolecular interaction dominates the effect of increased molecular mass, and f decreases in conformity with the prediction provided by the molecular crystal model.     

Solid-Solute Phase Equilibria in Aqueous Solution. XII. Solubility and Thermal Decomposition of Smithsonite

The solubility constant of ZnCO₃, smithsonite, in aqueous NaClO₄ solutions hasbeen investigated as a function of temperature (288.15 T/K 338.15) atconstant ionic strength I = 1.00 mol-kg^–1. In addition, the solubility of zinccarbonate has been determined at 2.00 and 3.00 mol-kg^–1 NaClO₄ (298.15 K).The solubility measurements have been evaluated by applying the Daviesapproximation, the specific ion-interaction theory, and the Pitzer model, respectively.The thermodynamic interpretation leads to an internally consistent set ofthermodynamic data for ZnCO₃ (298.15 K): solubility constant log*K _p50 ⁰ = 7.25 ± 0.10,standard Gibbs energy of formation _i G (ZnCO₃) = (–777.3±0.6)kJ-mol^–1, standard enthalphy of formation _f H (ZnCO₃)= (–820.2±3.0) kJ-mol^–1,and standard entropy S (ZnCO₃) = (77±10)J-mol^–1 K.^–1. Furthermore, the DSCcurve for the thermal decarbonation of zinc carbonate has been recorded in orderto obtain the enthalpy of formation _fH (ZnCO₃) =(–820.2±2.0) from theheat of decomposition. Finally, our results are also consistent within theexperimental error limits with a recent determination of the standard entropy ofsmithsonite, leading to a recommended set of thermodynamic properties of ZnCO₃: