ELECTROAMAI.YTICAL
THE
CHEMISTRY
APPLICATION
OF
AP\ID II%TERF_*CI&
DOUBLE
CHRONOCOULOMETRY TO THE Ti(II1) -HYDROXYLAMINE
PETER
JAMES
LINGXI‘NE
Gales and CreZli?t Laboratories
_44ND
=-v
ELECXROCHE-MISTRY
POTENTIIAL-STEP
THE
STUDY OF REACTION”
JOSEPH
of Chemistry.
H.
CATALYTIC
RE-4CTIONS:
CHRISTIE
CaEifovnG
Ixstitzrte
of TechrzoLog>e, Pasaderza,
CnZifomz;z
(U4S.A.)
(Recei-i-edFebruaq
rqth, rg66)
IKKRODUCTI03i
The originally
oxidation and most
of Ti(II1)
by hydrosylamine
in the presence
of oxalic
acid was
polarographically by RI&XX AXD ICORYTAI. These authors obtained a rate constant at ~5” of ~z_z-+ 1-5 l/mole set and an activation energy of 7.9 “r;calfmole. This value of the rate constant was subsequently confirmed polarographka-lly by DELXHAY, &~A~AX AND BERZIKS~. BL~~EKAXDX(ORYT_LL~ alsodetermin ed the rate constant by mixing hydroxylamine and TifIII) solutions and following the rate of disappearance of Ti(III) polarographically_ The rate constant obtained under these conditions was qz.o~o.z l/mole setBLX~EK AKD KORYTA concluded that their results were consistent with the previously-proposed mechanism of Dxvrs, EV_L~KS AND HIGGINSON~I Ti(IV)
+ e+
Ti(II1)
+
-XI& 03zIic
acid
thoroughly
+
Ti(II1)
TNH~OH oxalic
serves
FISCHER,
studied
.?% Ti(IV)
acid %%
as a radicd DRXCK_%
-I- Ho_O +
-NH2
products scavengers_
SXD
FISCHER•
VXQ
hax7e
potentiome~y at low concentrations of hy~oxyl~ne where the catalytic reaction is relatively slow and rate
cocstant SXVEAW~
for the study
of 45_9-1_0_4 _4XD
l/mole
studied this system by chrono(5-10 rnr;) under conditions of second order. They obtained a
sec. have
vwSELILoL~
of this reaction_
(Ii
They
e-x~ploy-ed
obtained
a rate
Linear
sweep
constant
chronoamperometry
of qz_ot_1_7
l/mole
sec.
In the case of a controlled-potential experiment such as polarography. the presence of a catalytic reaction simply means that a larger current is flowing at -any given time and the precision tithwhich this larger current can be measured is not affected. But in the case of a controlled-current experiment such as chronopotentiometry, the presence of a catalytic reaction greatly decreases the rate of potent&I change of the indicator electrode, especially in the vicinity of the transition time, aud * Conl23+iaIl
X0. 333g_
228
P. J_ LINGXXE,
thusrendersthe this reason we
determination ofthetransition timesubstantially expect chronopotentiometry to be a poorer ted
J_ H. CHRISTIE
more
than
difficult_For a controlled-
potential technique for the study of fast catalytic reactions. This is borne-out by the investigation of DEL-WY, &JAm-ax
These
authors found
quite a low
value of z4l/mole
AXD BERZIXS~. set for the rate constant (recal-
culated from their value at 30~ using an activation energy of 7-9 kcal/mole) in a chronopotentiometric study of the Ti(III)-hydroxylamine reaction. They concluded that
they
had obtained an incorrect value
of
the
rate constant because
of the
poor
definition of the chronopotentiometric
transition times. were able to circumvent some
CHRISTE AKD LAUER~ difficultiesby the use of reverse-current chronopotentiometry. Under these conditions, the forward time is a quitewell-definedquantity- Since the shapeoftheTi(II1) oxidationwaveis essentially unaffected by the catalytic reaction, a normal potential inflection is obtained at the transition time
for the reverse
wave_
CHRISTIE
ASD
LXUER
obtained
a value
of
32_0-&2.0 l/mole set for the rate constant (recalculated from their value atz7"S using an activation energy of 7.9 kcal/mole). HERMAN AND BXRD~ consideredtheapplicationofcyclicchronopotentiometry to the studyofthe Ti(III)-hydroxylamine inconsistent Mth a single rate constant complicated than previously =sumed_ justlfied5.
reaction_ Their experimental results were and they suggested that the s_ystemis more This conclusion may not be completely
CKRISTI@ has recently investigated the application of double potential-step chronocoulometrytothestudyofelectrodereactions_ Inthispaperweundertakethe application of the double-step chronocoulometric technique to the study of the Ti(III)-hydroxylamine reaction. RESULTS
XND
DISCUSSION
Our solutions areinitialIy free of Ti(II1) and the concentration of hydroxylamineissufficicntlylarge(roo-zoomF) thattherate ofreactionis well described by a pseudo first-orderrate eIertrode,issuchthatno
constar,t, K('NHaOH). Eo, currentflowsthroughthe
whichissufficientiycathodicthatthereduction
theinitial-potentialoftheindicator cell.ThepotentialissteppedtoE1 of Ti(IV)
is diffusionlirnited. After a
time. t. thepotentialoftheelectrodeissteppedtoEs~vhichissuKicientlyanodicthat the
otidation
of Ti(III) is diffusion l&nit&_
Ignoring the effects of double-layer total faradaic charge ares
charging,
the faradaic
currents
and
the
Ti(III)-HYDRoXYL_sMINE
TRE
where
82 = K( -NHsOH)
,
concentration of Ti(IV). extreme values of fltf_
Fxg. (II),
I. Experimental fit*1_3_ The
D
REXCTIO~
is assumed
TV
Figure
equal
I reproduces
1-t and Q-t traces for extreme current. charge. and time scales
to
Q(z)
E
D, and *CO is the bulk I-t
values of flth_ (I). fl tl= are identical in I and
Forming the ratio of the charge due to the due to the reduction of Ti(IV), we obtain
Q(=) -Q(t)
DTi[m,
experimental
(2figr+,E)erf
oxidation
and
traces
for
o (no hydroxylamine) II.
;
of Ti(II1)
Q-t
to the
charge
f2E-t
I _ 1 -
3
(2)
-
Note that this ratio is independent of the numerical value of D. of the electrode area, and of the bulk concentration of Ti(IV). calculated from eqn. (2)) ‘us. The curve illustrated in Fig. 2 is a plot of @&+I, #Pt_ In the limiting case of no catalytic reaction (KS+). the simple diffusion-limited reaction becomes very fast (k-co). no value of 0.586 is obtained 8. As the catalytic charge G recovered on the reverse step and the ratio goes to zero. We have calculated an extensive table of b”t a5-a function of IQb/Q=j (copies can be obtained from the authors)_ This table was used for the evaluation of /P from the experimental data_ which
A- striking advantage of any integral technique lies a correction-for double-layer charging can be effected_ J. EZecCroanaE.
in the simplicity with In the present case we Chem.,
13 (x967)
2~7--235
P. J __LINGANE,
230
J. H_
CHRISTIE
write
whereQ,and&arethe tively and
esperimentally~observedvalues
41 and
50 represent
the charge
required
ofQ
to charge
att=t
and
the double
21;
layer
respecfor the
forward (cathodic) and backward (anodic) steps, respectively. The asterisks signify that the measured quantities have been corrected for double-layer charging. In the present investigation, qfand qb were deterrninedby repeatingthe experiment in solutionsidenticalwiththosebeinginvestigated but which containedno titanium_ I
I 0.6
I
I
-
I
o-o
o-a
O-0
I
I
I
I.6
2.4
32
4-o
B2y
Fig.
2. Plot
T-!BLE
of IQb/Q,l
us. 82~
talc
from
(2).
1
2.0 mF 35_0°
Ti(IV).
0.20
F oxalic
16.8 II-7
440-O 21=&o
go-0 +z.o
acid,
pH
The results of double of hydrkylamineare
determinations-~-The o-50 -ad 0.60 PC, smaller
than
I-I,
E.
=
-TOO
mV,
EL
=
-60600 mV,
EI =
ooo mV.
o-57 0.5s 0.58 O-576
absence
=
o-57 0.58
7-81 5-5 6 4-03
21.0
1_7%
eqn.
f
0.002
potential-step chronocoulometric tixperirnents in the given-in Table r; each entry is the average of four
Vah~es of _Qf -and @, determined respectively_ The average vz&e
the theqretical
value
of 0.5S6.
for-the sa%e step intervals, are of~~/*Qb/?QII is 01576 +nd is sbme
The reason
for this small
discrepancy
THE
Ti(IIT)-HYDRoXYL_%MINE
TABLE 2-omF
mv,
2
Ti(IV),o.ZoFoxalic EZ = ooo mV
15 o" 412.0 ZIO_O 93-o
acid,pH=
16.5 10.4 6-4
25.oQ -402_0t
25.8 r5_I 7-6 5.2 3-6
207-O
79-o 4I_0 20_0t
84.0 44-O
35.o0 92.0 43-9 20.0
* zb f +
0.021 o-19 0.07I 0033
Average
7.90 8 6 8.q 8.1 8.4 8-35
2 & f + + 2
0-15 0.14 0.065 o-12 0.13 o-092
Average
S-14 -8.6 8.4 S-37
f f f 5
0.081 0.19 0.11 o.oS6
0.32
3-17 1.78 0.65 o-33
o.=j16
0.17
0.220 o-357 o-447
1.70 0.72 036
O-195 o-3=3
201 o-95 042 Average
0_4’Cj
in theaverage.
AVerage
3.17 3-3 344 3-32
1.30 0.69
O-134 0.2I3 o-371 o-457
11.8 6.8 4-o
f Neglected
1.o.0.204 Fhydroxylamine,&
0.262 3_362 0461
16_78-g 59
210.0
TAELE
23=
REACTION
=
-IoomV,E+
=
-6600
0.32 0.3I -F_0.7' f 0.26
22.0
&
22.4
&
21.8 22.0
see text.
3
2.0 mE; Ti(Iv). 0.20 F oxahc -600 mV, EZ = 000 mV
acid, pH
=
1-1, 0.102
F
p
hydroxylamine,
t (mice)
Qr f&l
'Qb/'Qf
fi’t
25.00 4I4-0 220.0 go.0
22.4 13.6
O-203 0.300
I.90 r-03
7-S 5-I
O-430 O-500
0.42
t-67
43-o
0.2I
22.0t
3-7
0547
0.085
4-8 f 4.2 * 4.70 f
.
4-60
21-O
IO-I
6-3 4-4
o-293 0.404 o-489
: j- yeglectedin
I.08
12.5
&
12.2
f
0.24
II-Z- f I'_? f
I-04 O-50 -0.25 -Average the avey+,seetext:
&
0.52 Average
45-o0 37-o_ X9.0 8.6
-& o.org
4-71 zt o-079
Average 35-o" S6_0 42-O
(SEC-l)
o-049
O-I3 0.35 0.040
0.28 0.28 0.24
0.23
28.0 ma I-6 -27-o -& 2.0 29.0 +!z I-I 27-g --f 0.92
ECU=
-100
rnv, EL =
P_ J. LIXGANE,
233
J_ H. CHRISTIE
was varied from - IOO to + zoo mV were performed and results similar to those of Table I were obtained_ \%‘e conclude that the reduction of Ti(IV) and the oxidation of Ti(II1) are diffusionlimited at -600 and ooo mV US. S.C.E., respectively; all subsequent
experiments employed these step potentials. The data obtained in the presence of 0.1 and 0.2 F hydroxylamine edinTables z and3_ Eachentryistheaverageofatleastfourexperirnents. fidence
intervals
listed
correspond
to the
standard
deviation
of the
are present-
mean.
Thecon-
Values
of
qf and qb were determined for the same step interval for the various solutions and only small variations were observed among them_ Therefore, 4~ and @ were taken to be c-50 and 0.60 PC in all solutions. Variation of qY and qb with temperature was not investigated. For any given temperature and hydroxylamine concentration, 8’ should be independent of t. In certain experiments performed with unrecrystallized oxalic acid (which appeared to contain a trace of reducible impurity), B2 was observed to increase dramatically with decreasing values of z at any given temperature and concentration of hydroxylarnine. The constancy of ,9* over a wide range of values of t appears to be a sensitive and useful diagnostic test for impurities and othcirregularities in the system and for the correctness of 40 and yl_ In performing the experiments, it was necessary to decide over what range to vary /?“t_ We have rejected all val les of /?z corresponding to values of the ratio I*Qb/*efl less than 0.2 or greater than o-s_ XVhere available, such values have beers included in Tables 2 and 3 and it is evident that including them in the averages would not
have
altered
the rate
constant
substantially_
,.a -
Fig. 3_ Plot of log RT US. T- 1 for 'he (e).u.I; (0). 0.2 FNH~OH
evaluation
of Rz~
and
of the
_%rrhenius
activation
energy-
The slope of the working curve (Fig. z) has a value of about 6 in the vicinity of p2t = I_ Therefore, an error of about I”/~ in the ratio of i*@/*@[ in this region results in an error of about 6% in the rate constant_ The precision for the determination of r and QzIis not better than I o/o and so xi-e are somewhat surprised, and gratified, by 3 the low standard deviations associated with the experimental determination bf pz.The activation energy was deterrnin ed from the pldt in Fig. 3. Since the stand-
THE Ti(IIIf-HYDROXYLAWIXE
REACTION
233
ard deviationsassociated=vith thevarious values oftherate constant vary by only a factor of three, all of the data pairs were weighted equal157 in the calculation of the least-squares slope and intercept_ The results are 43_4+r_x
As99
=
E,
= 17_2+1_1
where
the
vaIue
of
l/mole set kca_l/mole
confidence KPS
intervals
confirms
the
now
correspond
polarographic
value
to
the
of
B~AZEK
g5:&
confidence
level_
AXD KORYTA~
chronopotentiomet~c value of FIXHER et &?.a_ Theactivationenergy deterrninedinthisstudyislargerbyafactoroftwo thevalueof7.9 kcal/ mole found by BL_+EK AXD KORYT-~1. We were unable
and
This the
than to resolve
this large disagreement by repeating their calculations a-fid therefore we have re-determined t’ne activation energy polarographically. The polarographically and double potential-step chronocoulometrically-d&e-tied rate constants are plotted in Fig_ 3_ The slope of the polarographic line corresponds to an kcal/mole and is in excellent agreement with the value potential-step technique.
activation determined
energy of 17.3 by the double
Double potential-step chronocoulometry compares very favorably with polarography for determining the kinetic parameters of catalytic reactions. This technique can probably be used to measure values of p” of at least 7coo-zoo see-I, well into the polarographic range. /32z can be varied over a far wider range than is possible xvith ‘polarography and this flexibility makes possible the useful diagnostic test for systematic irregularities described above_ Although the experiments were easily performed, obtaining the data from Polaroid prints 1s somewhat tedious, but it is evident that the -experiments could be modified in any of a variety of ways so as to obtain Qr and Qer directly in digital form and thereby increase the ease and simplicity of the experimentl”. ESPERIMEhTTAL
Fisher technical-grade ter and
then
dried
KzTiO(GO&
to constant
weight
- z H20 was twice recrystaliized from waat 60% relative humidity. Solutions were
prepared by weight and were allowed to equihirate 2-1 h before use. Solutions tigated prior to such equilibration appeared to contain two reducible species.
~~nc~odt impurity
xvhich was
AR
H&QO~ - 2 H&
removed
by a single
contained small recrystallization-
inves-
amourzts of some oxidizing The salt was dried for 2 h
at so0 and weighed as the dihydrate.
>99% putity,was recxystalMatheson, Coleman-and Bel! (NHzOH) - HzSOe, lized from an &o/0 ethanol-water solution and d&d for I h at TOES_Stock solutions
P. J. Llh’G_4NE,
231
were standardized by titration withperm_g~ateaccordiTlg~~o &LzZ_~ andthetiterofthesesolutionschangedlessthano.~o~odnring-the experiments-
J_ H. CHmSTIE
&e-method of BRAY courseofthese
MeYczcYy
Ik%llinckrodt
AR
mercurywasemployedintheexperirnentstiththehanging
mercury
drop- The DME experiments Bethlehem Apparatus Cd.,Hellertown, edto
be less than
employ&l triply-distilled mercury from the Pa.; totalnon-volatileimpurities werereport-
0.025 p-p-m_
AU solutions were prepared from triply-distilled water and de-aerated with Matheson “prepurified” nitrogen ( c S p.p_m_ oxygen) -which was further deoxygeuatedby passage through a vanadous &shingtower prior ro entry into the cell. The
electronic circuitry is shown
schematically
in Fig_ 4 and
is analogous
to
LMJER AND OSTERYOUNG~O. Neiay z controls the reverse step and is fired by a xrariable delay timing circuitrf_ The supporting equipment is essentially as previously descnbedl”. The measured rise time of the potentiostat is less than 20 ,usec. The area of the hanging mercury drop was 0.0407 cm2 at zs”_
that of CHFUSTIE.
WEIIKING
7”E”
‘R’ T
POTZNTlOSTAT Aux I
[ I
CURRENT
Relay
MEASURING
AMP.,
2
tiCZA1002 INTEGRATOR
HGZAIOOZ
Fig. -4- Block diagram of the solid-state operational amplifiers The
employing G. electronic appmtus and C. =P. Glare 9c Co_ mercury-tietted
polarographicset-upernployedtheequipm&rtshownin
A.
PhiZbrick relays_
Researches
Fig:dandathree-
electrode cell; the output of the current-measuring amplifier was fed to a Sargent SR recorder aiid the maximum polarographic currents were r_ecorded at - 500, 2 600 and _poo mVvs.S.C.E.Underourconditions,th~ecatalytic~--tcurvewasobservedtobe a->/3_orderparabolaandthecatalyticcurrentwas mercury head: Therate constant was calculated
observedtobeindependentofthe accord>o KOUTECK~~~.
THE
Ti(III)-HYDROXYLAMINE
Thecellwas -f-O.ZO.
REACTION
235
thermostattedatthestatedtempertitures
withaprecisionofabout
2xCKKOWLEDGEIvIEXT Wewishto
thank Army tion
withProfessorF_
acknowledgehelpfuldiscussions
C_ AXSON
and
to
him for providing splendid research facilities under the auspices of the Office of Research (Durham)_ We are especially indebted to G. LAUER for his collaboraon
certain
preliminary
experiments,
for desi,ting
the
experimental
apparatus,
and
for his continued interest during the course of this investigation. The work was supported, in part, by predoctoral fellowships from the U-SPublic Health Service, Division of General Medical Sciences (PJL) and from North
American
Aviation,
Inc_
(JHC)
_
SUMMARY The applied
theoretical
to the
study
relationships of catalytic
Ti(III)-hyclroxylamine tion
for the reactions
reaction_
The
double were
kinetic
potential-step
verified
parameters
by
chronocoulometry
an investigation
obtained
in this
of the
investiga-
are;
where ported
k 398=434&1-r
l/mole
E, = 17_2 + I_1
Ircal/mole
kiss is the rate values
of k=Bare
cons-taut
set
at 2~~ and E,
is the Arrhemus
energy.
in ezcellentagreementwiththevaluereported
previously-reportedvaluefortheArrheniusenergy
Previously-reherebutthe
appearstobeinexplicably
inerror-
REFERENCES L -4 BLA?EIE ~fjD J_ I
+ 3 6 7 8 g IO II 12
13 14 15
COl~eCZiOw CZSC~L Chem. CO7m?ZUn.. I8 (1953) 326. AND T. BERZINS, J_ _-lm. Ckem. Soc_, 76 (1954) 53rg_ P_ DAVIS. M_ G_ Evi~xs AND W. C. E_ HIGGINSON, J_ CJresm_ Sot., (1951) 2563_ 0. FISCHER, O_ DRACICA AND E. FISCHEROVA. Collection Czec7i_ C7zem. Comnzu~z.. 26 (1~61) 1505. J_ H. CHRISTIE XND G_ LATTER. Amzl. Chem., 36 (1964) 2037~ G. LXUE_S. pnvate communicationH. B. HER~LLP; AND A. J_ BARD. LXTL~Z_Cfienz.. 36 (1961) 510. J_ H_ CHRISTIE. J_ EZe~dronnal. Chem.. 13 (1967) 7g_ XV. C. BRAY, M. E. SIU~SON _SND A. A. IMACKENZIE, J_ ,4tn. Chem_-Sor;., 41 (19x9) 1363. J_ H. CHRISTIE, G_ LXUER AND R_ A_ OSTERYOUNG, J_ Etectrcanal_ Chem.. 7 (x964) 60~ G_ LAKER. H. SCHLEIN AND R. A. OSTERYOUNG, Atzal. Chem_, 35 (1963) I7Sg. I?_ J_ LINGA~T. AND J. H. CHRISTIE, J_ Electyoanal. Chew.. IO (x965) 284. J_ KOUTECKP. Collectim Czech. Chem. Comnrtrn.. 18 (1953) 311J_ M. S-~VE~T AXD E. VIAh-EILO, EZed~ochim_ Acta. IO (1965) go=j_ G. L_~UER AND R_ A. OSTERYOUNG, Ayzat. Chem.. in press.
J_ Elactroanal.
Chem.,
I3 (1967)
227-235