JOURNAL
THE
REDUCTION
OF
ELECTROANALYTICAL
WAVES
OF
CHEI\IISTRY
NICKEL
ION
IN
3=3
SOME
SUPPORTING
ELECTROLYTES T. TAK4HASHI Insfifzcfe
of
Industrial
rUI;D
H. SHIRA41
University
Science,
of
Tokyo\(Jupan)
(Revised manuscript received September
Igth,
1960)
INTRODUCTION
Studies on the reduction wave of mckel ion in perchlorate as a supporting electrolyte have shown that it consists of one wave, whose wave height is independent of the concentration of perchlorate. R_ H_ SANBORN~ reported that the wave height in the reduction of nickel ion depends upon the concentration of an electrolyte such as sodium chloride or potassium chloride, and concluded that this result was due to the formation of Ni(1) ion Furthermore, A_ A. VLCEK' considered the reduction wave of nickel in sodium chloride to be accompanied by a kinetic current_ The present paper shows that the reduction waves of nickel ion in potassium nitrate, potassium bromide and potassium sulfate, as well as potassium nitrite, depend on the concentration of the supporting electrolyte,
and
that
except
in the case
of potassium
nitrate,
two
waves
are formed.
APPARATUS
The details of d-c. and a-c. polarographs have already been reported3.4. voltage of IO mV was superimposed on the applied d-c_ voltage, and the
The a-c. standard
L
I Fig_
I_
D.c_
polarograms
of (a),
0.5
I
-QS
I mM 32
I -07
I -CL6
nickel KNOJ;
E (V ion (b),
vs. N.CE_,
in potassium 1-0
AI
KNOJ;
30;)
nilkIte (c),
1.8
at various COncen~ationS (30°) M
]_~EZeciroannl_
IaO,. Chemr,
3 (19611 313-319
:
T.
314
TAKAH4SH1,
H_
SHIRAI
capacity (C,) was 0.3 PF. An agar-agar bridge connected the reference electrode [I iV calomel) and the polarographic cell, from which oxygen was removed by passing hydrogen. The dropping mercury electrode used had the following properties: m = 2.77 mg/sec, t = 3-6 set, (--1.2 V ?IS_N.C.E. in 0.5 M potassium nitrate)_ Potassirim
nitrate
as a sz+portimg
electrolyte
The reduction wave pf nickel has one wave in 0.5 M potassium nitrate, having a half-wave potential at --I-OS V (300)_ Figure I shows the d-c. polarograms of I mM nickelionin potassium nitrate at various concentrations_ The wave height decreases with increasing potassium nitrate concentration, and isindependentofthe addition ofo_o05~/~ gelatine. Figure2 showsthea.c_ polarograms of nickel ion in both the presence and absence of dissolved oxygen_ The two wave polarograrn, registered in the presence of dissolved oxygen, changes to a one wave
E PJ vs. mercury
poo~,
JO-)
Fig. 2. A-c. polarograms of IO mM nickel ion in I &I potassium nitrate in the presence or absence of dissolved nsvgcn ; (a),in the presence of oxygen; (b), in the absence of oxygen.
Fig.
=J_ _Relationsbip
between
the
wave
height of r m&T nitrate.
nickel
ion
J_ EZectroanaZ_
potassium
Chem_.
3 (1961)
313-xzo
REDUCTION
WAVES
when the dissolved oxygen
polarogram
OF
NICk-EL
is removed.
The
3=5
of this wave
disappearance
is presumed to be due to the reduction of Ni(OH)+ or Ni(OH)z formed by reaction with OH- ion,whichisproducedbydissolvedosygen on thesurface oftheelectrode. Figure3
givestherelationshipbetweenthewaveheightandI/hin
nitrate. The
graph
does
kinetic currentinthe Potassium
bromide
not
pass
through
the
r.S Mpotassimn
origin, indicating
the presence
of a
limiting current. as
a szcp~orti~~g
eZectroLyte
The shape of the reduction wave of nickel ion changes withthe concentration of potassium bromide used as a supporting electrolyte_ InFig.4,thed.c.polarogramshowstwo distinctwavesino.SMpotassiumbromide, but the secondwave seems to disappear at a concentration of r.S M, asisshown by (c)_ The half-wave potential of the first wave is -r-o7 V (30°j in 0-5 M potassium bromide. Thesecondwavealsodisappearsifo.oo~o/ogelatineisaddedtothesupporting
L 18 -
- 0.8
Fig-
4. D-c.
polarograms 0.8
M
- 10
of I mM nickel KBr containing
-1.2 E (V
5-
A C. POlarOgrams
of
N.CE.,
vs.
mercury
-1.6
-18
27’)
ion in potassium o.oo~~/~ gelatine;
E (V Fig.
- 1.4 VS.
bromide I (a), in 0.8 (c), in r-8 M KBr.
poop,
_W
I
(b).
300)
IO III&I nickel ion in 0.8 A&potassium bromide: of oxygen; (b). in the absence of oxygen.
(a),
in the
prsence
in
3x6
T_ TAKAHASHI,
KL SHIRAI
electrolyte solution, as can be seen from Fig- g(b)_ Similarly, the second wave was confirmed in the presence of dissolved oxygen, which it disappeared, as can be seen from Fig. 5_ Figure
6 gives
the relationship
in a d-c_ polarogram
of I mM
between nickel
line (b) does not pass the origin, more, the elxistence of a kinetic
the
wave
ion in 0.8
height
of the
A4 potassium
indicating the presence current was also found
appearance of the in the absence of first
wave
bromide,
of a kinetic in the d-c.
and
in which
@ the
current Furtherpolarogram (c) of
nickel ion in 023 M potassium bromide containing o_oo~~/~ gelatine, (as shown in Fig. 6), and in r-8 M potassium bromide (not shown in the Figure). But the line expressing the relationship between the total wave height and r//t passes through the origin
(line (a)), showing
that
the limiting
1 Fig. 6. bromide
Relationship (~7~) : (a).
3
the
presence
7_ D-c_ in o-45
polarograms M &S04;
of I m_ii (b). in o-3
M
of
(V
VS_
diffusion
rate.
277.j
of I m&E nickel xvaves; (b). the o.oo~~/~
ion first
and vh in o-8 ~l:ipotasr;iun~ wave; (c), the first wave in
gelatine.
-14 N.C.Ej
by the
9
N-C-E.,
-1.2 E
Fig(4.
vs.
height second
-113
is controlled
5
E (V
between the wave sum of the first and
current
-16 27”
-1.6
I
nickel ion in potassium sulfate at I(,SO4; (c). in o-3 N J&SO, con~g
various
concentrations: gelatine.
0_005~/~
RJZDUCTION
Potizssit4m sulfa&9 as a szcp$wting
WAVES
OF
3=7
NICKEL
eZectroZyte
Figure 7.shows the d.c. polarogram of I m&f nickel ion in o-45 N (a) or 0.3 A4 (b) potassium sulfate. The shape of the wave changes with the concentration of potassium sulfate, and the addition of o_o05~/~ gelatine makes the second wave disappear, as the polarogram (c) in 0.3 M potassium sulfate shows_ The half-wave potential .is --I.IZ V (30~) in 0.3 M potassium sulfate_ The a-c.. polarogram of nickel ion in the presence of dissolved oxygen is given in Fig. 8, which-shows two waves, the second wave disappearing in the absence of dissolved oxygen.
I
-1.2 E
Fig.. 8.. Ax.
I
-1-4 Yz. mercury
I
I -16
pool.
- 1.8 30”)
polarograms of IO m&T nickel ion in 0.5 M potassium sulfate: (a). in the presence dissolved osygen; (b). in the absence of dissolved oxygen.
of
Fig. g_ Relationship between the wave height of I miW nickel ion andvjz in 0.3 MT potassium sulfate _ (a), sum of the first and second waves; (b), the first wave; (c), the first wave in the presence of 0.005 a/- gelatIne_
The relationship between the wave height of the first wave and pz in the d-c_ polarogram in 0.3 M potassium sulfate is shown in Fig- g, in which the line (d) does not pass through the origin, indicating the presence of a kinetic cm-rent.. Smce.line (c) also does not pass through the origin after the addition of o.oo5°/o gelatine, the yave: height is partly dependen L on kinetic current- But the limiting current containinff:
T_ TAKAHASHI,
3rS the first znd
expressing
second
waves
is controlled
the relationship between
H.
by
the total
SHIRAI
the diffusion rate, because wave
height
andvlc
the
linh
passes through
(a) the
origin_
The d-c. polarogram of nickel ion in o-5 M and I M potassium nitrite gives two waves as shown in (a) and (b) in Fig_ IO, but xtith an increase in the concentration of potassium uitrite, the first wave height seems to increase and the second wave height
decreases, although
only slightly_
The
---o_S5 V (307andthatofthesecondwave--1.09 The latter potentials equals the half-wave
half-wave V
potential
potential ofthefirstwaveis
(30°)ino.5 Mpotassiumnitrite. of Ni(HzO)e"+.
6
-0.6
Fig-
IO-
D-c-
- 0.6
E
polarograms
I
E (v Fig-
II_
Ax_
tv
of I mM niclcel ion in IL1 I
polarograms
of
IO m&1 oxygen;
YS_
N.CE.,
30°)
potassium nitrite:(a),in 0.5 1w KNO.; containing
vs. mercu~-y
o OO~~/~
pod
(b).
in
gelatine.
)
nickel ion in I M pot&urn nitrite: (b). in the absence of oxygen_ J_ Ekctroawal.
(a),
Chem_.
in the
presence
3 (1962)
of
313-320
REDUCTION
The
a-c. polarogramin
I M
potassium
WAVES
OF NICKEL
nitrite containing
3=9 dissolvedoxygenis
given
Fig. II, which shows three waves in the presence of dissolved oxygen, although the third wave disappears after removal of the oxygen. It is not certain that the first wave is controlled by the diffusion rate-because it is difficult to determine the rela-
Fig.
I?_ Relationship
between
the wave height
of I m&1 nickel ion and I/k in 0-5 potassium (279.
nitrite
tionship between the wave height and V?z,as the firstwave approaches the second wave. But the total wave height obtained by combining the firstand second waves passes through the Orion, in~catingthat the total limiting current is controlled by the diffusion rate, as can be seen from Fig. IZ. DISCUSSION
Ofthetwo waves of nickelionin potassium sulfate andpotassium bromide, the first wave accompanies the kinetic current. Therefore, it is considered that the reduction ofnickelionistheelectrodereaction,forcompo~dswhichareinmutua2equllrbrium. Here, the firstwave equals the half-wave potential of Ni(H&)$+, so the firstwave is probably due to the reduction of Ni(HzO)G'+. But the second wave appearing in thepresenceofdissolvedoxygenoccursatapotential---o_zVmorenegativethanthat of the first wave, and it disappears in the absence of dissolved oxygen, so that it is perhaps due to the reduction of Ni(OH)+ or Ni(OI-E)zformed between nickel ion and OH-ion, which is producedby reduction of the dissolved oxygen. The second wave appearinginthe absence of dissolved ox3Tgerroccurs at a potential ~_4to -0-5 V morenegativeth~thatoffhefirstwave,sothatitisprobablynotduetothe reduction of any compound co-ordinated by an OHgroup_ But such a second wave is consideredtobeduetothereduction ofacompoundco-ordinatedby SOa- or Br-ions of the supporting electrolyte, because the second wave height depends upon the concentration of the supporting electrolyte_According to I. M. KOLTHOFF AND J- JLINGANE”, nickel ion exists as Ni(H20)E "+in potassiumnitrate solution_ But the presentstudysho~vedadecreaseinthe~vaveheightofnickelionwithincreased(o.5 n/l--+ J_ EbckxztlaE.
Chcnz.. 3 (1962)
313-320
T. TAKAHASHI,
320
H.
SHIFLTI
I Al->r.S _Mr) potassium nitrate concentration, and a combination of kinetic current into its wave height_ Therefore, it is evident that in potassium nitrate there is not but also a compound coordinated by NO3;-_ These compounds are only Ni(HzO)G+. mutually in a state of equilibrium, the latter compound not being reduced until the applied
d-c_ voltage
reaches
the
potential
of the
final
increase
current. In potassium nitrite, nickel ion exists as two complexes, the complex co-ordinated by NO?-_ The first wave is caused
of the
polarographic
i.e., as Ni(H2O)s”+ and by the reduction of the
latter and the second wave by the reduction of Ni(HsO)s~~. The authors have considered the results of R. H. SANSORN~ regarding the interdependence of wave height and the concentration of tbe supporting electrolyte, as follows. Nickel ion perhaps occurs as Ni(H&)6”+, even in large concentrations of perchlorate, because perchlorate ions do not complex with metallic ions. In sodium chloride solution, two complexes, i.e., Ni(HsO)63+ and a compound co-o&mated with Cl- co-exist, and the former may be more reactive to the reduction than the latter_ Therefore, the concentration of r\ri(.H,O).z ‘+ decreases with increase of Cl- ion, resulting in a lower wave height in large curring in small concentrations.
concentrations
of sodium
chloride
than
that
oc-
The reduction wave of nickel ion in potassium sulfate, bromide or nitrite shows two waves and the first wave is accompanied by a kinetic current, so that Ni(HzO)&and a compound co-ordinated with the anion of the supporting electrolyte are mutually
in a state of equilibrium,
the former being responsible for the first wave and the latter
for the second wave_ In potassium nitrate supporting electrolyte, Ni(HzO)a”” in equilibrium, and it was concluded from the half-wave is responsible for the reduction wave.
and another complex are potential that the latter
REFERENCES 1 R.
H_
-’ -4. A. 3 N.
SAXBORN ~I_CES,
SHIRAI,
3.
a T_ TAKAHASHI 5 I_ X. KOLTHOFF 1952,. p_ &36_
AND E_ F_ ORLEMANN, f_ Anz. ChemEZektrocTzezrz.. 61 (x957) xorq. Ckmz. Sut_ ~a$xz~z. 80 (1959) 609. 1435; AND E- ?+~KI. ~akmte, 3 (x958) 2~5. AND J_ J_ LIE;GAXE, Polarogmpizy.
Sac.. 78 (1956) $35~
2.
Sr (1960)
12+
Interscience
(in
Japanese).
Publishers
Inc.. FJe\vYork,