STUDY OF PROPERTIES OF LUSTROUS NICKEL COATINGS
1733
internal stresses were found by the method described
determined by the method described in [3].
in [7], with a flexible horizontally arranged cathode.
A 35 × 10 × 0.05 mm copper cathode being tested was
preliminarily annealed at a temperature of 700°C for
One of the most important tasks in the field of elec-
trodeposition of metals is to develop an electrolyte and
conditions in which coatings with prescribed properties
can be deposited. The physicomechanical properties of
electrolytic deposits, important quality characteristics of
coatings, predetermine their application areas.
3
0 min [8] and then was cooled in a closed furnace to
room temperature. The substrates were insulated on one
side with a poly(vinyl chloride) lacquer. Deviations of
the cathode from the original position were recorded
using a MIR-2 microscope. The IS was calculated by
the formula
One of properties characterizing the quality and
corrosion resistance of electroplated coatings is their
porosity. It is known that this property depends on
whether IS appears in deposits and on the quality of the
preliminary treatment of the substrate surface, substrate
material, current efficiency, and electrolysis modes.
Finding reasons for pore formation in deposits is one of
the most important issues in electrolytic deposition of
metals and alloys.
2
Ed z
IS = –––– ,
2
3
δl
where E is the elastic modulus of the substrate material;
d, cathode thickness (m); z, cathode end deflection (m);
δ, coating thickness (m); and l, length of the coated part
of the cathode (m).
It can be seen in Fig. 1a that the porosity of coatings
deposited at a temperature of 20°C, pH 1.0, and coating
–
2
Changes in the luster of the nickel coatings were
studied on 50 × 60 × 0.5 mm steel plates with an FB-
thickness of 6 μm at current densities of 1–5 A dm
–
2
increases from 13 to 15 pores cm and then decreases
to 12 pores cm as the current density is raised
to 9 A dm . It was found that the porosity of 6-μm-
–
2
1
A luster meter. As the reference whose luster was
–
2
taken to be 100% served a polished copper plate coated
with a 20-μm-thick layer of lustrous nickel from the
thick coatings deposited at a cathode current density of
5 A dm and pH 1.0 decreases from 15 to 9 pores cm
–
1
–2
–2
electrolyte of composition (g l ): NiSO ·7H O 260–
4
2
3
00, NiCl 6H O 40–60, H BO 30–40, 1,4-butynediol
as the electrolyte temperature is raised from 20 to 60°C
(Fig. 1b). For coatings deposited at a current density
2
2
3
3
(100%) 0.12–0.2, saccharine 1.5–2.0, and phthalimide
–
2
0
5
3
.08–0.12. The electrolysis was performed at pH 4.0–
.0, temperature of 55–65°C, and current density of
of 5 A dm and a temperature of 20°C, the porosity
–
2
decreases from 15 to 9 pores cm as the electrolyte
pH is raised from 1.0 to 4.0. As the pH value is raised
further (to 5.0), the porosity increases to 11 pores cm–2
–
2
–8 Adm .
The strength of coating adherence to the base was
(Fig. 1c).
determined by multiple 90° bending of a coated sample
until its complete fracture in conformity with GOST
9
coating thickness, 20 μm. We examined the outward
appearance of the coatings with an MIM-7 microscope
at ×487.5 magnification. The porosity was determined
by application of filter paper in conformity with
GOST 9.302–88.
As the thickness of a coating deposited at a cathode
–
2
.302–88. The sample size was 25 × 5 × 1 mm, and the
current density of 5 A dm and pH 1.0 increases from 1
to 12 μm, the porosity first sharply decreases and then,
in the range 9–12 μm, varies only slightly. For example,
as the thickness of nickel coatings is raised from 1 to
–2
9 μm, the porosity decreases from 36 to 10 pores cm ,
and when the thickness is raised further to 12 μm, the
–
2
porosity decreases to 8 pores cm .
The phase composition of the nickel coatings was
examined with a DRON-1.5 X-ray diffractometer with
CuKα radiation and a nickel filter. The X-ray diffraction
patterns we obtained were indexed by the Frevel–Rinn
method [9]. The angular correction of the diffractometer
was determined using a reference (quartz). The
scanning rate was 1 deg min . The throwing power of
the electrolyte was studied with a dismountable angled
cathode with an angle of 60° between its sides [10]. The
current efficiency (CE) by nickel and hydrogen was
We studied how the IS in nickel coatings depends
on electrolysis modes (Fig. 2). Measurements were
made at the completion instant of electrolysis. Tensile
stresses were observed. It can be seen in Fig. 2a that,
as the cathode current density is raised from 1 to 5
–
1
–2
A dm , the IS increases from 235 to 245 MPa, and
upon further increase in the current density from 5 to 9
–
2
A dm , decrease from 245 to 225 MPa at an electrolyte
pH 1.0 and temperature of 20°C. As the electrolyte
RUSSIAN JOURNAL OF APPLIED CHEMISTRY Vol. 84 No. 10 2011