electrosorption of cellosolve at ethyl mercury/kcl solution...

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Indian Journal of Cbemlstry Vol. 16A, May 1978. pp. 391-394 Electrosorption of Cellosolve at Ethyl Mercury/KCl Solution Interface M. v., RAMANAMURTI, B. V. APPARAO & R. K. SINGH Department of Chemistry, Faculty of Science, Banaras Hindu University, Varanasi 221005 Received 4 A pf'il 1977; accepted 26 N ouember 1977 Adsorption of ethyl ceUosolve at the mercury/O·l0 m KCI (aq.) solution interface has been studied through equiUbrium double layer capacity measurements. Langmuir's adsorption isotherm is obeyed with rs=4·91 x 10- 10 mol cmos and ~Gomax = -3·73 kcal mol'<, The adsorption isotherms are found to be congruent with respect to both electrode potential and charge. The dependence of ~Go of adsorption on electrode potential is quadratic. The anodic shift of Epsc ··with increase in concentration of the cello solve indicated orientation with the hydrocarbon chain facini the electrode and functional group in solution. The linear shift of potential 01"zero charge (Epllc) with surface coverage of the adsorbate suggested a single stable orientation of ethyl celio80lve throughout the coverage region. A DSORPTION of organic compounds at the mercury-solution interface is studied chiefly through electrocapillary and differential capa- city measurements, Equilibrium double layer capa- city measurements alone are sufficient to evaluate the surface concentration of the organic molecules. This, however, is strictly valid only when the electrode charge and interfacial tension are in- dependent of adsorbate concentration at extreme cathodic or/and anodic polarizations. This condi- tion is indicated by the capacity curves at various concentrations of the organic component coinciding with that of the base electrolyte at these polariza- tions. This paper presents the results of the adsorption of ethylene glycol mono ethyl ether (ethyl cellosolve) at the mercury/OrHl m KCI (aq.) solution interface through equilibrium double layer capacity measurements. Materials and Methods Differential capacities were measured by Gra- hame's ac bridge method 1 2 using a dropping mercury electrode (d.m.e.) with a drop time of .-g sec. at the potential of zero charge (EpIC) in 0·10 m KCI (aq.) solution and a varia ble signa I genera tor (Ma rconi TF 1370). The capacities were normally measrred at a frequency of 1 kzk with an amplitude of ,...,5 mV across the cell. With pure 0·10 m KCI solution, the capacity data were independent of ac frequency and agreed with Grahame's datas, In order to check the frequency dependence of capacity in the presence of adsorbate, a few measurements were made in the frequency range 0·2-4·0· kHz. The capacities were found to be frequency dependent even below 1 kHz, only in the region of desorption peaks. The frequency dependent capacities were plotted at different frequencies and extrapolated to zero frequency .. Thus, the capacity data report- ed in this paper correspond to equilibrium double layer capacities. A locally designed and construct- ed magnetic drop detacher was used to knock off the drop a t a prefixed time. Time of knocking was fixed a rbitra rily to a bout two-thirds of the natura I life of the drop. The differential capacitance measur- ed was independent of the drop time even a t the desorption peaks indicating atta ir.ment of adsorp- tion equilibrium at d.m.e. The time between two successive knocks of the deta cher wz s noted by a stopwatch measuring 0·05 sec. interval accurately. The bridge was balanced at the instant of the detach- ment of the drop from the capillary tip. The output signal of the bridge was amplified by a multi- stage transistor preamplifier (Marconi type TM 6591A) and then displayed on a Dumont oscillo- graph (Type 274). A large mercury pool electrode and N RCI calomel electrode (NCE) were used as the auxiliary and reference electrodes respectively. The potential between the test electrode and the reference electrode was measured on porta ble poten- tiorneter (Pye-Ca mbridge ; accuracy 1 mY). Differen- tial capacities were measured in the potential range -0·10 to -1·g0 V vs NCE. The measurements were carried out in an air thermostat controlled at 25°±0·lo. Mercury W2S purified following Trasatti's methods, Twice recrystallized (from conductivity water)' KCI (BDH, AR) was used. Ethylcellosolve (Riedel) was trea ted with lithium hydride until the evolu- tion of hydrogen gas ceased and then distilled twice. Solutions a t required molalities of ethyl cellosolve in 0·10 m KCl were deoxygenated with purified and presa tura ted nitrogen before C8 rrying out' the experiments. Results and Discussion Capacity-potential curves - The capacity-potential curves (Fig. 1) for ethyl cellosolve follow the same sha pe typical for simple alipha tic organic compounds. The capacity curves at all concentrations of ethyl cellosolve coincide with that of the base electrolyte at extreme cathodic potentials (~-l·g V vs NeE) indicating complete desorption of ethyl cellosolve. 391:

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  • Indian Journal of CbemlstryVol. 16A, May 1978. pp. 391-394

    Electrosorption of Cellosolve at Ethyl Mercury/KCl Solution InterfaceM. v., RAMANAMURTI, B. V. APPARAO & R. K. SINGH

    Department of Chemistry, Faculty of Science, Banaras Hindu University, Varanasi 221005

    Received 4 A pf'il 1977; accepted 26 N ouember 1977

    Adsorption of ethyl ceUosolve at the mercury/O·l0 m KCI (aq.) solution interface has beenstudied through equiUbrium double layer capacity measurements. Langmuir's adsorptionisotherm is obeyed with rs=4·91 x 10-10 mol cmos and ~Gomax = -3·73 kcal mol'

  • '.r---------------------------------~INDIAN J. CHEM .• VOL. 16A. MAY 1978

    .r---------------------------------~

    42 7i'0!

    0-2>

  • RAMANAMURTI " Ill.: ELECTROSORPTION OF ETHYL CELLOSOLVE

    (0)

    4

    o o 4) 0-0·6D 00 e -0.7o 0 c;: 0 Q:~:

    ~-,.o..0 0

    ~,','~-"2

    -e

    ·0.4-2

    '0.6 c c

    ~~----40------Q~--~~__--o~_6...uZ• ·'.0>

    . '.2

    Fig. 3 - (a) Electrode charge as function of surface excessof ethyl cellosolve at constant potential [Potential indi-cated on each line]. (b) Electrode potential as a functionof surface excess of ethyl cellosolve at constant charge

    [Charge indicated on each line]

    v

    '" A-e-'"0to .. u,

    E 0.06 w

    N~0s- -0

    0 "-is?.. O.O~V"IL!'

    0·01

    0·04 c·oe 0.11 0." 0.1~c ••~_lojll

    'Eig. 4 - Test for Langmuir's adsorption isotherm for ethylcellosolve: (A) E = -1'0, (B) -0'9, (C) _0'8, (D) -0·7,

    (E) -0'6, (F) -0'5 V vs NeE

    o

    0.0%

    of E and increases with decrease in E. Themaximum r.,f values (rmu) obtained at Es, -O·70Vvs NCE (cf. Fig. 2) for various concentrations havebeen employed in plotting C.,fjrmu. vs l/CA (cf.broken line G in Fig. 4). The plot obtained is linear.The value of rs obtained thereby, viz. 4·91X to-10mol em? is independent of E. The maximumof surface coverage (6=rA/rS) attained in thepresent work is 0·70.

    ,

    '7f~.- 3.

    II!>C1I

    - E Vs NeE (\loll.)

    Fig. 5 - Standard free energy of adsorption as a functioDof electrode potential for ethyl cellosolve

    0.1 0.3 0·4 0.50.3 e

    -0.5-2·0

    Fig. 6 - Ep.c as a function of (a) logarithm of bulk concen-tration of ethyl cellosolve and (b) as a function of surface

    coverage of ethyl cellosolve

    The standard free energy of adsorption (AGO)has been calculated from Eq. (4) given by Conwayand Barradass for Langmuir's adsorption isotherm:

    In(SS'S._6_)=_ AGO ..• (4)c, 1-6 RTAt 6=0·3, the values of AGOhave been calculatedat various electrode potentials and the dependenceof 3Zo on E (d. Fig. 5) is found to be quadraticas expected for simple neutral organic substances.The value of K?;~ax (-3·73 kcal mol+) whencomparedt 0 that of ethylene glycol8 (-2·02 kcalmol-I) is a consequence of the relatively weakerintramolecular hydrogen bonding of ethyl cello-solve molecules than that of ethylene glycol withwater molecules.

    Shift of Ep•c with log C.,f and with 6 - The poten-tial of zero charge of mercury in the pure base elec-troyte solution shifts towards less negative potentialswith increasing concentration of ethyl cellosolve(d. Fig. 6a). This indicates that ethyl cellosolveis adsorbed on mercury with the hydrocarbonchain facing the electrode and functional group inthe solution phase. The shift of Ep. with surfacecoverage of ethyl cellosolve (d. Fig. 6b) is linear

    393

  • INDIAN J. CHEll., VOL·t6A; MAy·t978

    suggesting thereby a single stable orientation of Referencesethyl cel1osolve throughout the coverage region'.

    Acknowledgement

    The authors are grateful to the UGC 'and CSIR,New Delhi, for the financial assistance to B. V.Apparao and R. K. Singh respectively.

    :~"

    -

    .: "

    L GRAHAME, D. C., J. Am. chem. Soc., 63 (1941), 207.'2; GRAHAME, D. C., J. Am. chem, Soc .• 71 (1949), 2975.3; TRASATTI, S., J. eleciroanal. Chern.• 28 (1970), 257.4; DUTKIEWlPZ,;E •• GARRISH, J. D. & PARSoNS, R., J: eleo-

    ; troanal. Chem., 16 (1968), 505. .5~ CONw*"\[, ..13.. E. & BARRADAS, R. G., Electrochim. tfcta,:,5

    (1961). 319. . .. .6; TRA~ATTr;. S.,:1- electroanal. Chem., .53. (1941), 335.