--_.:
..
..
.-
-1‘. -‘--- .. -: J. Electron~aL’Chkm,.l68(i984)
.:.
:
.-
i63--;IjB.:1
:
:
.’
-.
163
'EIs&-ierSequdiaS.A.,Lausan~e-Pri&&inTheNetherlands _.
_ -:
_:-
--:.
‘_.._
_:
.:
..:
. .’ A
.COMPARATIVE STUDY OF THE-DISSOLUTION OF NICKEL AND COPPER .IN ACIDIFIED ACETONITRILE-H20 .and .CuCl2-NaCl-H20 SOLUTIONS
CuS04-
: Z.Y..LU,~D.M. School
MUIR and
I.M.
RITCHIE.
of Mathematical and qhysical Sciences,
Western
Aus&?
ia
6150
(Au&-al
Murdoch
University,
Murdoch,
ia)
ABSTRACT The electrochemistry of the dissolution of copper and nickel rotating disc 0 solutions was investiCuS04-AN-H 0 and CuCl -NaCl-H electrodes in acidified zed from el zctroch e&-?cal measurements gated. The rate constants calcula 0 and CUSO~-AN-H2Q indicate that the dissolution .of copper ih both CuCl -NaCl-H diffusion a;id nickel in CuCl -NaCl-H 0 soIutions ar g a71 Cu P II) solutions, controlled. However, the-disgolution’of nickel in acidified CuSO -AN-H 0 solutions was shown to be controlled by the formation of a nicke140xide2fi?m_ Rate constants for nickel dissolution were measured by three methods. Good agreement was obtained between the mixed potential predicted from polarization measurements and that observed in the dissolution process.
These results of two comparable from a segregation
contribute to a fundamental understanding of the reactivity leach systems proposed for the processing of calcines derived of dead roasted cha?copyrite/pentlandi te concentrates _
INTRODUCTION There using
is
an
brine
increasing
solutions
interest
or
in
sulfate
the
leaching
saltsinaqueous
because of the high stability of Cu(I) in requirements has
been
for
carried
nickel
Cg-111
acidic
aqueous
out in
is
known about
in
aqueous
the electrolytic recently
acidic
on the
chloride
solutions the
has
~221
who reported
Fe(III)
in acidified
of
also
been or
for that
the
the
two
investigated
of
AN-H20 solutions
is
of
of
the
copper of
of
energy
low
work
C3-83
and
nickel
in
However,
C12-191.
copper
solutions
Extensive
kinetics
Pang
dissolution
and
passivation
dissolution
of
(AN)
[?,21.
kinetics The
work
electrowinning
systems
copper
electrode
solutions.
electrochemistry
AN so?ution-except
Ritchie
these
recovery
and
acetonitrile
1 i ttl
copper
and
et aZ_ C201 and Couche copper
controlled
metal
by
the
by Cu(I1)
diffusion
e
nickel and or
of
the
oxidant_
cou7d
in
brine
be used
roasted
at
35oOc.
The
to
750°C
solutions leach
and
Cu(II)
sulfate
a chalcopyrite/pentlandite
followed
calcine
by segregation.
consisted
of
mainly
roasting copper
~. 0022-0728/34/$03.00
that
by Lu et aZ- C223. it was repobted
.In an,ear?ier paper chloride
~1984ElsevierSeq~oiaS~.
-in
both Cu(I1)
aqueou‘s
acetonitrile
calcine
which
with metal,
salt nickel
and
.
solutions
had
been
coal
-at
metal,
dead 670-
nickel
.I
164 :
oxide- and magnetite _ copper
recovery
with the least
Both 1 each systems: gave similar
and between l-69% nickel
amount of nickel
leached nickel
most nickel leached temperatures favour A fundamental leach
.‘ _: _ _:.
.~
with-the
leached
resul ts:with’88-95%. The large
copper depended onthe
variation
segregation
-in the
conditions.
with 5% coal at 670 ‘C -and-the It is believd'that: higherafter segregation at 870 ‘C. : the formation of Ni metal rather than NiO. .-.
after- segregation
study of the dissolution
systems was therefore
conditions
.recovery.
.-
of the leaching
of copper and nickel
undertaken to ascertain process
in the two
the mechanism-and-optimum
and to compare the electrochemistry
of
copper and nickel corrosion in chloride and sulfate media, in an attempt to achieve more se1 ective 1caching under specified conditions_ This type of study is also of importance to other metallurgical processes. In the dissolution of copper and nickel iti copper(I1) chloride-brine solutions or in copper(I1)
sulfate-aqueous acetonitrile solutions, the cathodic of copper(I1) and the anodic oxidation of copper(O) and nickel(O) are processes. Accordingly, these half reactions were investigated and
reduction important
compared in typical leach solutions. The diffusion another fundamental parameter which was investigated differ
significantly
concerning
in chloride
and sulfate
the mechanism of the dissolution
constructing
coefficient since it
media.
Valuable
reaction
may also
an Evans diagram C231 from the separate
of copper(I1) is likely to
is
information be obtained
polarization
by
curves.
Mixed potentials predicted from the polarization diagrams were compared with those measured during the leaching reaction and the corrosion currents.were compared with rate constants
determined
by kinetic
measurements.
EXPERIMENTAL Solutions
All
chemicals
used in the preparation
water was purified 40 MS2 cm_
by a double deionizing
analytical
grade reagents.
system and had a resistivity
The of about
Acetonitrile was distilled over KMn04 and the middle fraction was
retained (b.pt. 81 ‘C).
was free
were
of
impurities
This fraction within
showed no UV absorbance
the limits
of detection
above 220 nm and
of gas chromatograph.v_
Electrodes The platinum disc electrode
teflon cylinder diamond paste. adsorbed distilled cycling
and polished
(area 0.196 cm’) to a mirror
was mounted in a 1.5 cm diameter
smooth finish
using 10 nm and 1 urn
The electrode was then degreased with chloroform and cleaned of organic matter by immersion in chromic acid and washing with double water. Any surface films were removed by repeated anodic/cathodic
between 1.6 V to -0.90
The nickel wet-and-dry
V in 0.5 M H2S04 (us Hg2S04/Hg)_
electrode (purity : 99.99%) was prepared by abrasion Carborundum paper and washed thoroughly with deionized
with 1200 water and
:-
: ..
_..
‘. :
.~
:. ..
165
.'
.
it was ;etched
:Alter.natively,solution
for -about---1’.min ‘in. a_n equal -
HNGB-and.H2S04. then Gashed thoroughly
-.volume mixture_ of :concentraied .tiater and the test ._ .-~
.
..::_ :
'.
_-
--thk‘ t&+solution,:
_y-
:-
-
I
just
prior
to use..
1..
with -_.
_~
(purity : .99.9%) was prepared’_ by abrasion with 1200 wetCarborundum paper. : It -was.etched. in a.-solution ‘of 50 volume %
The .cGpper el tiiytrode
and-dry nitric
acid,
then rinsed
-‘The counter- electrode
with deionized
water and acetone.
was a platinum wire-with.
a surface
area of about 20
times that bf the working electrode. ,. For the.Cu(II)
chloride
SHE)was used with a saturated aqueous Cu(II)-acetonitrile
a calomel
system:
reference
electrode
(0.245
V US
For the potassium chloride solution salt bridge_ a Hg2S04/Hg reference electrode (O-655 V
system,
US SHE in water) was used with-a saturated potassium sulfate solution salt bridge_ In each solution, the bridge was connected to a Luggin capillary which was placed with its tip about O-5 mm from the centre of the working electrode_ All potentials in this paper are quoted vs the SHE in water. to facilitqte a were made for the liquidcomparison between the two leach systems. Corrections junction
potential
between aqueous acetonitrile
sulfate
solutions
and a
saturated K2S04 bridge using the values determined by Senanayake and Muir E241. Equipment and technique Polarization curves for the reduction of Cu(II)- and the oxidation of copper and nickel
were measured on a PAR Electrochemical
system Model 170.
Viscosities
relative to water were determined using an Ostwald viscometer. The kinetics of nickel dissolution was determined by chronopotentiometry described
by Barth- et aZ. C251.
An exactly
onto a platinum electrode in an electrolyte -I; Na2S04. 120 g 1-l; NiS04_7H20, 175 g 1 pH =: 5.5. The electroplating
was carried
the platinum electrode
rotating
rate,
was determined
as
was plated
with the following composition: NaCl 25 g 1-l; HSBOS,l20 g 1-l;
out at a current at 400 rpm.
mined by atomic absorption analysis acid) was 97 r 1%. The dissolution dissolution
known anWnt of nickel
density
The efficiency
of
50 A m-
of plating
of nickel after dissolution time.in the leach solutions,
with (deter-
in hydrochloric and hence the
by measuring the sudden change in electrode
potential.
RESULTSAND DISCUSSION Reduction
of Cu(I1)
For Cu(I1)
in- Cl-/H20
and S0,12-/AN/H,0 solutions
dissolutiGn .reactions, the diffusion (D) of Cu(I1) is alfundamental parameter of the process_ Itmay be conveniently.determined:at a rotating-disc electrode by measuring the coefficient
diffusion-controlled
: ’
1 imiting current density -(iL).- as -a..function of rotation speed ‘(w) for the-. .., reduction of Cu(I1) to Cu(1) on platinum, and applying the Levich equation T261:
_..-
..
166
I
-. _... -.
--:’
_.
-.
._ ~. :.:.-.
.: -:
.-
._ _. f--:.z)
,wisinrads-l,: Figure
i
chloride there and
is
shoks :th&t
-there
solution,
and
a clear
departure
in
is -a’ Very most from
good
aqueous.
Levich
relationshi-6
for
acetonitrile&lf&te
1 inearity.:in
the:case-
Cu(II-)--j-n
.solutio& of
low
-but
AN .concentratio.ns.
high.acidity.
40(
10
20
1
30
40
b-q-td4
Fig. I. Effect of rotation speed on Cu(I1) diffusion-controlled current density in AN/H 0 and NaC1!H20 solution at 25 ‘C and Cu(I1) = 0.1 M. Key: (RI)3 M Nah , 1 M HCl; (X)6 K AN, 1 M H2 SD4: (814. M AN, 0.05 M H&4, 0.5 PI Na2S04; (A)4 M AN, 1~M H2S04. .. -:
.’ .. 1.. : ..
-. ‘. ..
acetonifrilk
&der~o& 'ao~e~~le&r&i' t&&f&r' reductjon._ iti.th+potential -.r&ige of 0.45 -‘-0’:15- V; and .that. 6eldw- 0115 V; .a-‘further -reduction-takes place: leading to ammonia and ethane’as.~ final’&oducis:.-
In.this:.workf we &nimid&the effect : of AN adsorption -by Itredting~~the el e&ode. at a- positive potential before eachpotentiodynamid were erratic:’
measurement. ~.
Without- such ~pretreahnent; --the’ results
-.:
obtained .,
The effedt-df Cu(I1) ~
Itis~surpri&r&
that in the-~con~&k~ation range O.OOl---6.i .M Cu(II),
‘it
is the concentratioti-of Cu(II) rather than .the-background -soltition-and speciation of_Cu(II) that has the greatest
the value of D even for the’solutions
,_ -.-
,.
effect
on D:
of similar
There is a clear ionic strength -.
decrease
in
when the Cu(I1)
-..‘; ._.
-.
.
.
.:.
Fig_: 2_ Cu(II). diffusion .coeffi&ents -as:6..functidn of 'Cu(I1)&&entr&on -. (in AN/H&l; -NaCl’/HpO,and Hz0 at..25:‘C). .Key::_-_1_ CuSO$-in: Na2S.O at: pH 2, pi =.1.58, .ref-- [301;_. 2:...CuSO;-.in water.-.refC311:- .31 j 3 M NaC4 ; 1 M HCl;:.U-= 4.3;. -4. .--‘6MAN/H20, 1
concentration.increa&s;. Quickenden.and~Jian~~.~~D,, and.Eversole_&~+$, :-[37]_ .(wh&
~&ults_~~&e
also shown in-cig_'-Z); ;,havereporteda $imilar~.tre_nd~ for_ j :
cu(Iij in'>cjueoussulfate solutions. .Therefore,t-hetioDper.con&tration seems~._.to be a'very~.im@rtant~factor::to‘be considered-when-ma-kingcomparisons.betwee_n~, j -diffusion coefficients in d~fierent.:sclutians;~~
’
‘-.
!-.
.:
1
Diffusion coefficients of Cu(II);.Cu(I)and Fe(II1) in -'aqueous~solutions
containing various concentrationsof.Cl-, AN and acid are listed in Tab1 e'l..., A direct comparison of these values is difficult not only because of changes in the concentration of Cu(I1) but also because of changes in the speciationof Cu(I1) in chloride and sulfate systems. In acidified sulfate solutions, there . . 2will be further changes dependent on the pH and relative concentrationsof SO4 2and HSO;. Copper(I1) forms a weak complex with SO4 ) KI = 4-O C32; and a slightly stronger complex with Cl-, K1 = 4.0, K2 = 4.7 C331. According-to the Eh-pC1 diagram for copper, Cu(I1) primarily exists.as CuC12 at high chloride f concentrations.whereas it exists as CuCl at low chloride concentrations C3L
When the diffusion coefficient of Cu(I1) iscompared with those of Cu(1)
TABLE 1 Diffusion coefficients of copper species at 25 'C_ Electroactive DElectrolyte lo-ID/m2 s-l species 0.1 M CuSO4, 4 M AN, 4,4 Cu(I1) 0.05 M H2SO4. 0.5 M 0.1 M CuSO 6 M AN,Na2S04 4.5 Cu(I1) 0.05 M 0.1 M 0.1 M CuSO4, H2S8;,6 M AN,Na2SO4 1 M H2SO 4-4 Cu(I1) 0 05 M ftSO 6MAN 5.82 0.0002-0.003M CuSO Cu(I1) Cu(I1) 0.05 M CuSO 10 M $4 0 05 M -5 Cu(I1) 0.001 M CuSd;, 0 1 M icSo 62Sg4 7.1 5-54 0-l M CuC12, 3 M-NaC1.21 8 HCl Cu(I1) 0.1 M CuC12, 4 M NaCl, 0.02 M HCl 5.52 0.1 M CuCl2,4M NaCl, 1.0 M HCl 0.02 M CuCl 3 M HCl 0.0002-0.009 M CuCl, 4.0 M NaCl 7.3 0.1 M CuCl, 4-O M NaCl, 1 M HCl Cu(I) Fe(II1) 0_OlMFe2(S04)3, 6.0 M AN, .4.2 1.0 M H2S04
Ref.
this work this work this work ~281 CZOI E281
this work this work c351 c31 c281 r351 c211
and Fe(III), it is found to be much lower than that of Cu(1) .butmuch the same 2+ as Fe(II1). This is because the strongly hydrated ions, CU(H~O)~ and Fe(H20)63+, are large compared with the weakly hydrated Cu(AN)$or CUCKOOfrom species. Furthermore, nitrile molecules are reported to displatie.water the outer solvation .shellof Cu(I1) ion and make it less mobile than in aqueous solutions E341. If allowance is made for the pronounced effect of ion-pairing in concentratedCu(I1) solutions, as well as the influence-of ionic
strength
.: ....:--:
...,,.
_:-
.,._
._
-I.:. .;.:. .;-.-, I
.‘: .
‘.
__.i_. -, ‘._“ .. ..-.-’ >. -.‘..:and Cl_y[ANlconcentration;-:etc; -_ . .I1 . .- .
: ._..I
:~
._
-,
.. .
‘.
:I..
.
_..
_.
, ‘.it -will..-. ..-I .z_:. be.pbserved .that the d.iffusion .!of. Cu-i.II)..det‘~rrmned- in this’.work are surprisingly similar-‘.
. . ~do&&iekts
are inuch”greil:ter~~~ftErendes’ in thereported..values RDE-techniques, and .widely .~differing’ ~&n&ntrations_
difftision
coefficient
of. &13~-~
was -slightly
. 169 .’ :
There
for.Cu.( I) .using:it’ and. f?&r: c353 ‘found that the
lower. than that
?f Fe(CN)i3-
measured by’RDE under the same-conditions and reported a value relative to the . . standard value of Fe(CN)63-. ‘_ This work-~shows that the-diffusion coefficient of Cu(IJ) in our chloride system ii about 515 x iO-lo m2 s-l , which’ls__. slightly of 4.4, x 10-l’ m2 s-l in our. sulfate-AN-H20 system. controlled
conditions,
we wouldianticipate
higher than the mean value Thus, under diffusion-
slightly
faster
leaching
using CuCl2
in brine compared with CuS04 in, aqueous acetonitrile, Anodic dissolution of copper and nickel. Quite different~behaviour can.be.expected for the anodic or nickel in chloride and sulfate media. In dilute chloride known
to form CuCl which can cover the copper surface
reaction. nickel
The formation
_
sulfate
On the
other
solutions
of
hand,
such
an insoiuble
nickel
is
C12-197, whilst
layer
be ieadily
copper passivates
of copper
media,
and limit
chloride
known to
reactions
is
topper
unlikely
with
aqueous current den-
passivated
only at-high
is
the anodic in
sities. It is therefore particularly relevant to compare the anodic dissolution of nickel and copper in strong brine soluti_ons in which Cu(1) is qui.te soluble .as cuc12- and CuC132- 3 and in aqueous acetonitrile-sulfate solutions where nickel passivation‘is likely to -influence the leaching process. Figure 3 shows the potentiodynamic polarization curves for a copper and-a nickel
electrode
solution.
in both aqueous AN-sulfate
solution
and aqueous chloride.
It can be seen that in a 6 M aqueous acetonitrile
solution,
both-
_
nickel and~copper passivate at +0.4 V and +0.7 V, respectively. However, the peak current density -obtained with copper was about 50’times higher than that. obtained
with nickel .and wassimilar
at PH 3as well
as at PH.0 with 1 M H2S04.
The passivation of nickel in aqueous-sulfate solution is caused by the formation of a nickel oxide film and has been widely studied Cl3-191_ The passivation of nickel ism.
in sulfate
solutions.containing
Wi.th regard--to
copper,_as
AN would probably
the current
density
have a similar
‘and concentration
mechanof Cu(1)
at the surface. of the electrode increases, the -concentration of free AN in the double-layer decreases and Cu(Jj becomes .unstable, Hence, the formation of- an insoluble
copper(I1)
cu4(oH)6s04, C361.
salt,Rassive
film
is.possible.
CU~(OH)~SO~or Cu(OH)2arethe
However .at .pH -< 2; passivation
CuSO4.on the anode surface ..,
__.*
is
-At.pH 5 3 and Eh > 300 mV,
thermodynamically likely
stable
species
to be caused by saturation
of.
X371_ .-
Fig3. Anodic potentiodynamic polarisation curves for Cu and Ni electrodes in,AN/H20 and NaCl/H20 at 2.5 OC. Full lines 6 M AN; 1 M H$O4; dashed line 3 M NaCl, I M HCl; scan rate 10 mV S-l; stationary condition. In
practical
O-70
V to
This
is
copper about
systems,
0.2
-
0.3
much more
+0.4
important
is
copper of
about
formation Benari of
in
in
of
to
ratio
than
the
peak
density of
the
the
in
solutions
Cu(II):
potential
after
nickel
leach
of
for
nickel
vary
Cu(1)
in
copper
passivation
is
peak
very
low
active
is
that
in
state
a 3 M NaCl,
even
at
1 M HCl
a current
solution
the
density
at a potential of about +0.2 V with -2 A m . In this case.the passivation of
of
4000
a peak
current
2300
copper
is
a CuCl
et at.
film
[381.
density
60 mV per
-
SO
occurs
(Fig.
solution
passivates
of
0.65
passivation,
passivation
AN-H20-sulfate
from solution.
at
3).
especially
processes. 3 shows
an
the
However,
current
Fig.
still
potentials
unlikely.
passivation
leaching
The measured about
the
the
passivation
current
is
V and
By contrast, rode
negative
passivation
Consequently
the
V according
as
But
will
not
is
much
Tafel decade
discussed
again, occur
slope for
under with
higher
than
within the
by Braun
and
practical
Nobe
leaching
C61,
chloride
concentrations
the
1 imiting
current
100
dissolution
mV of of
the
rest
copper
Hyde
density potential,
electwhile
density
caused
by the
i3J
conditions,
high
Ni
A m-‘,
and this
because of was
in both chloride
kind the
peak
Cu(II). found
to
solutions
be
.
_.
_--..
:
-_
i
_,-, :.
__
. _y
..
(
.-
:.
-.
‘:;
.._:y
:
f.
:
;.
:
;
:
-.
-_:, :
17%
.. .; : and AR-Hz’) ._‘sUl;fate.~sol Utions ;. This- did not differ .over a range’ of AN concen‘trati& .fG& .i ‘_ 14 k and does no~tcompare with a-.Tafel slope of 37-4d I% reported ‘for the anodic .. sol&ions. i35j;. Hhie, sulfate
solu‘tions-
dissolution
of copper
the addi.tion
in deaerated
aqueous sulfate
of even 1ow:concentrations
of AN to
changes the mechanism .and ‘Tafel. slope.
In’pure- water the ‘anodic dissolution .ofcopper is a. two-step process with Cu+‘to CL? being rate dettknin~ng C40; 411.. Eut.from these r<s-it would appear.that the copper(I)-acetonitrile complex is in reversible-equilibrium with copper meta. at the electrode surface; and that the slow step is the mass transfer of ‘.the species Cu(AN),,+- into the bulk of the solution. Since the current density (i). is given by the following Levich equation when the bulk concentration is much less than the surface concentration i
0.62FD
=
-u6
2'3
u2
v
w
CCU(AN)n+l,
(2)
where square brackets denote concentrations, and the subscripts refers to the surface, we can then apply the Nernst equation and obtain the'following relationship: E=E”
+ (RT/F)lni
Thus it
is clear
- (RT/F)ln(0.62FD
from equation
(3)
2'3
v
-we
that a Tafel
l/2
w
slope
.-‘j
) of 59 mV will
be obtained
if the reaction is under diffusion control It also follows from ;j;ation (3) that there should be a linear relationship between log i and 1og w at a fixed potential which will have a slope of 1. As shown in Fig. 4, a linear relationsh i p between log i and log w112 was indeed found, but the slopes are about 0.7 _ 0.8 for sulfate solutions containing AN, and about 0.9 for the chlor de solutions. Hence the anodic dissolution lled
of copper
to a large
extent
in both aqueous AN sulfate
current
slow irreversible rate.
density
solutions
is contro-
by the rate of
from the electrode surface. relationship for the anodic anodic
and brine
the diffusion of the copper(I) complex By contrast, there is no linear log i us log w1’2 dissolution of nickel in these two systems and the
is hardly affected
kinetics
with possibly
by the rotation NiO formation
speed.
governing
This implies the reaction
Fig, 4, Effect of rstatinn speed Qn medic current dansifias of copp@r in AN/H$ and NaCl/H 8. Key: 1. 10 M AN, 1 M H2SQ 3 E = Q.QQ V: 2, I'M ANI 1 M H2$Qq? R = tQ.QQQV; 3, 3 M N&l', 4 M HCl, fi = =Q,Q2 V; 4. 4 M NaCl, Q.Q2 M HCl, E = -Q.QE V. Evans diagram, corrosion
current
and.mixed
potential
The corrosion current density-and mixed po;et-&ialcan be obtained using an Evans Diagram.
Such diagrams,
as shown in Figs.
5 and 6 plot
the
cathodic
polarization curves for Cu(II)/Cu(I) on platinum and the anodic polarization curves of copper and nickel in the solutions without Cu(II);
can be seen
It
that for both copper and nickel in chloride solution, and copper in aqueous ANsulfate
solution,
the dissolution
similar
corrosion
current
rates
densities
at
are
Cu(I1)
various
diffusion
rotation
controlled
with
The slight
speeds.
difference observed is attributed to the variation in the diffusion coefficients of Cu(I1)
in the leach solutions as discussed above.
dissolution of nickel in aqueous AN-sulfate current
density
the presence to 50 ‘C, from about
at
the
passivation
of chloride
the
peak current
800 A m-2
M H2S04,
the
When the
density
for
temperature
nickel
is more complex by temperature, is
increased
and the
acidity
and
from 25 ‘C
in 6 M AN and 1 M H2S04 increases
(Fig. 5) to 2400 A mm2 and nickel changes from a passivated
state to an active state. to 1.0
ions.
solutions
peak is affected
On the other hand, the
Similarly, when the acidity
peak.current
density
increases
changes
about
ten
from 0..05 M H$S04
times
(Fig.
5).
o-
l
-0
-__-_
61
Q2
-____
$3
8.6
\
______._
Cl!%
.-06
($7
E (v) Palarisatlen diagram fsr the dlssslution sf copper and nickel with E:?;I:‘l” B M AN/H Cl CuSQ = 8 1 M; Na SQ = S mva ssl; Q;; t$ H$Qq = 1 M (full lines) erQ.Q5 M (dashed l&v&); scdn rate .
1
3
Polarisation Fig. -6. Cu(I1) -in 3 M NatJ,
diagram 1, M HCl;
for CuCY2
the =
dissolution of copper and nickel with 0.1, M; .-scan rate = 5 mV s-l; 25.oC..
:
: ,174
..
..
-..
bf chloride
The addition
ion also accelerates. the break-down’of. _.__ increases_ the’ peak current density.
.~_ ‘a-rid greatly
filth
~.
.. -. ..
‘. :. : of .nfcke7 is a. very ‘-1. -. 5; active nickel has a
is -of interest to note -that. the mixed potential sensitive indicator of the prdcess. .-As shown in’Fig. It
potential
‘of about O-3-0-4
the diffusion current
controlled
density
V and its anodic-curve
region’
(points
A-E, Fig.
the mixed potential
is too low,
&pass.ive-
crosses’ 5).
the cathodic
Curve in
However, if-the.
.will
shift.to
anodic
the-lower
part of
occurs with a. change of the curve (points PI a.nd P2, Fig. 5j and. passivation about 0.35 V in the value of the mixed potential. The mixed potential of nickel dissolution therefore is a function of the When the nickel disc is rotation speed and the addition of chloride ions. stationary. the value increases passivates (Fig. only at rotation increased to 0.1
measured potential is about 0.35 V, but upon rotation, the’to about 0.72 V within a~few seconds as the electrode-surface 7). With the addition of 0.01 M Cl-, the passivation occurred speeds higher than 600 rpm. When the addition of Cl - was M, no passivation occurred and the mixed potential remained
at about 0.36 V even at very high speeds.
Thus, there by polarization
between the mixed potentials predicted measured experimenta 7y (Fig, 7) _ It is noted that the mixed potentials systems are virtually and anodic lals
reactions
appear constant
of copper
independent
of rotation
are diffusion
controlled.
(rr”. points
Table 2 shows the current
is an excel lent agreement curves (Fig. 5) and those
in both leaching
speed,
because
solution
both the cathodic
As a result, the mixed potentA, B and points F, G in Fig. 5).
densities,
mixed potentials
and Tafel
slopes
of copper
and nickel for several chloride and su7fate solutions_ Both measured va7 ues = and values calculated from the Evans diagrams are included. The good agreement of the data for the dissolution of copper in both leaching solution systemi, and the dissolution reactions
of nickel
are Cu(I1)
AN-sulfate solution temperature (50 ‘C)
in chloride
diffusion
solutions,
controlled.
is further
The dissolution
evidence
that these
of nickel
cou7d become Cu(II) diffusion controlled and in strongly acidic solution.
only
in aqueous
at elevated
Kinetics The dissolution
kinetics
of a-copper rotating
aqueous AN solutionscontainingCu(I1) chloride
solutions
containing
Cu(If)
disc
in various
CZOI and Fe(II1) [3J,
acidified
C217, as well
has been described-and
as in
good agre&ent
between the kinetic constants determined by rate measurements and electrochemical methods has been reported. In this work, the rate constants of nickel dissolution predicted from Evans diagrams were confirmed by kineticmeasurements. The dissolution of nickel in the region of its passiration is complicated by the
presence
of an oxide
film and so the kinetic
measurements.were carried
-out only
WO0-10M
;
I 030-I
c--
-
-:
-----
200
0
Cl-
800
1200
1600
Rotation speed ( r.p.m.)
Fig. 7. Mixed potential of a stirred nickel electrode in 6 M AN 1 M H2SO4, 0.1 M CuSO4 at 25 'C, and in the presence of 0.01 M and O-1 M Cl'_
in the Cu(i1) diffusion controlled region. In both CuC12-brine solutions.and CuSO4-AN-sulfatesolutions, the reaction between nickel and Cu(II)_ions proceeds according to.the following reaction : 2 cu2+ t Ni -f 2Cu+ +
Ni2+
(4)
For a diffusion.controlledreac.tion,which obey& first order kinetics. the concentrationof Cu(I1) wijl initi.allydecrease according to equation ii) : _V$. =
K.A C
(where A = area and C = concefjtration)
(5)
from which it-can be shqwn that : = .-
0.6?nD..
v
-.(i5)
c&-kosion curren_~ decsitiesj Tafel.
Comparison & of lcopper
and nickel.
‘at 25 ‘C
(@(II)_=
&lo&s
Tafel slope Electrolyte
El ectrode~
4 M AN, 0.5 M H2S04, O-5 M Na2SC4. 4 M AN, 1 M H2SOq. 6 M AN, O-05 M H2SO4, 0.1 M Na2S04_ 6 M AN. 1 M H2SOa. 4 M NaCl,
0.02
M HCI.
3MNaCl.
1MHCl.
6 M, 0.05
M H2SO4,
mV per decade
CU ( Ni 1 CU Ni { cu Ni { ,“r 1 cu Ni {-cu
6 M AN, f M H2S04b
mixed
y -.,
602
3
602
3
602
3
607
3
60%
Mixed.potential. V. ‘. measured .0.05 -0.62 0.06 -0.65 0.01 -0.60 O-06 -0.70 0.06 0.27 0.05 O-27
60; 3 -100 i 10 60+ 3 75 f 10 6Oi 3
:: { Ni ;r
0.1 M Na S04.b
and-the
Oil-M; 400 -r-pm).:
potentials
{ .-.-_.:-.. ‘~~~~~~~~ density A m-2
predicted 0.04:‘. .- -0.62 0.07 4.65 0.03 -0.60 0.07 -0.70 0.07 0.26 0.05. 0.29
-0.60
-0.60
OT28
or30
220. c 5a
190 < 5?225 < 5a 220 c 5a 250 250 250 250 300 c10a 300 300
3
apassivated bat
50 OC
l/2 This oredicts a 7inear re'lationshio between K and it, , as in Fia. 8, and !vhich was confirmed by chrononotentiometry’and direct chemical analysis of nickel. Activation energies were found to lie between 11-16 KJ mol-' in-both chloride and sulfate solutions which are typical for many such processes. We could not observe any significant differences between sulfate and chloride solution.
CONCLUSIONS The rate of dissolution of copper by copper(I1) in both aqueous acetonitrilesulfate
solutions
solutions,
and in strong
is control
brine
solutions,
led by the diffusion
and of nickel
of copper(i1)
in strong
brine
to the electrode
surface.
The dissolution of nickel in aqueous acetonitrile-sulfatesolutions is mainly determined ity
by the passivation
(1 M H2S04) and elevated
- 0.1
M Cl-,
the passivating
dissolution
in these
dissolution
of nickel
diffusion.
of the electrode temperatures current
two leach
is sufficiently
solutions.
was likewise
surface.
However,:at
high.acid-
(z-50'C), or in the presence high to allow
In the activated
found to be controlled
of 0.01
normal
condition, by the rate
nickel
the of Cu(I1)
Fig. 8. Comparison of rate according to rotation speed. 50 oc; full line 4 M.NaCl,
ion measurement;
For that
the
dissolution of nickel by various techniquesKey: dashed line 6 M AN, 1 M H S04. Oil M CuSO4, -0.02 M HCl, Oil M CuC12, 25 OC. a 0 by polarisatAAS analysis. •Jq by chronopotentiometry; A A by direct
purpose.‘of
CuS04-H20-AN
selectively-leaching
solutions
NaCl , have
absence
of
selectivity
is
present
as discreet
particles.
from
particles previousiy.
coupled
are
unlikely
the
at
No such
copper
of
ability
possible
copper-nickel to
low
copper
acidity to
using
from
ambient
selectively
leach
CuC12-H20-NaCl
Clearly
there
particles
predominate
and
will due
to
nickel,
it
would
temperature, copper solutions
be selective galvanic
without if
appear
and
the
in
nickel
_
metals
leaching corros;on
the
but
such
in the.double roasted calcines studied
C223
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