twin polishing for al alloys
TRANSCRIPT
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Preparation of high quality Al TEM specimens via a double-jet
electropolishing technique
Necip nl
Istanbul Technical University, Faculty of Chemistry-Metallurgy, Materials Science and Metallurgical Engineering Department, 34469 Maslak,
Istanbul, Turkey
A R T I C L E D A T A A B S T R A C T
Article history:
Received 2 February 2007
Received in revised form
28 March 2007
Accepted 6 April 2007
Obtaining clean, uniformly thin and high-quality TEM specimens entails a great dealof work
that has a number of parameters that have to be considered carefully depending on
specimen preparation technique(s). The parameters, such as voltage, current density,
temperature, time, electrolyte, and electrolyte flow rate, have the most significant
importance in a double-jet electropolishing technique. Useful hints to have the least
failures in preparing TEM specimens and optimum values of the above parameters for pure
Al are given and discussed.
2007 Elsevier Inc. All rights reserved.
Keywords:
Electropolishing
Aluminum
TEM
Specimen
1. Introduction
To understand and correlate the nature of the microstructure
of metals and their alloys directly with their physical,
chemical and mechanical properties, TEM analysis has been
a major tool. TEM analysis requires successfully prepared thin
foils about a few hundred nanometers or less thick from bulk
materials [1,2]; the success of the TEM analysis critically
depends on the quality of the thin foils prepared. Various
techniques, such as electropolishing using pointed cathodes
[3], jet machining [46], low voltage electropolishing using a
special cathode design [7], and jet electropolishing [4,810],
have been developed and used for the thin foil preparationsince 1949. Additionally, a number of experimental techniques
and theoretical knowledge on the preparation of thin films
have been summarized in specialized books, textbooks and
papers [1116]. In 1966, Schoone and Fischione [10] designed a
simple submerged double-jet technique [9] that enables the
polishing of metal disks simultaneously from both sides and
automatically stops the polishing operation when perforation
occurs. Basically, the preparation of the thin foils for TEM
analysis is comprised of three steps, (i) obtaining a sample
piece 12 mm thick, (ii) thinning the sample piece to about
0.2 mm, and (iii) electropolishing the sample to a thin foil
which enables sufficient electron beam penetration [17].
Electropolishing (EP) is a well-known method in an electric
potential passed through the chemical solution utilizing the
specimen as the anode [18,19]. Although this description
seems to be straightforward, to have reproducible optimum
conditions, the EP parameters (i.e., voltage, current density,
temperature, time, and flow rate) and characteristics of the
TEM specimen (thickness, conductivity, and its nature asbrittle or ductile) must be taken into consideration in the thin
foil preparation due to the fact that electropolishing rates and
ideal polishing conditions vary for most metals and alloys
[11,2023]. This paper describes the effects of both EP
parameters and the thickness of the TEM specimens with
regard to preparation of thin foils for TEM analysis.
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2. Experimental Details
The size, shape, and micro- and macrostructure of the hole
and time for hole formation were determined as a function of
the specimen thickness, electropolishing voltage and the
pump flow rate of the electropolisher. These characteristics
served as guides to determine the optimum electropolishingconditions. Pure Al sheet with 99.99999% purity used in this
study was obtained from Alfa Aesar, a Johnson Matthey
Company. Square 11 cm samples were gently cut from the
pure aluminum sheet by a precision diamond saw. Each
sample was mechanically ground on SiC abrasive papers (80,
120, 300, 600, 1000, and 1200) to five different thicknesses, 70,
100, 150, 200, and 250 m. During each grinding step, the
thickness was controlled using a Chicago Brand model digital
micrometer. 15 samples were prepared for each different
thickness. Then,3-mm diameter disks were punched from the
square foils by using a Gatan Disk punch. These samples were
electropolished using a solution consisting of 25 vol.% HNO3
and 75% methanol at different voltages in the range of 660 Vin a TenuPol-5 digitally controlled automatic electropolisher
with program storage capabilities. This instrument was
developed by Struers A/S [24] for twin-jet thinning samples
for transmission electron microscopy (TEM). The pump flow
rate of the electropolisher was adjusted as 15. The tempera-
ture of the electrolyte was held constantly at 202 C by
using Lauda Proline RP 870 model cooling system. The
polishing time was recorded from the digital screen of the
TenuPol-5 for each TEM foil. After polishing, the foil in the
holder was immediately rinsed three times in methanol. Then
the holder was opened gently and the foil was removed with
tweezers and rinsed in three small ethanol cups, gently
rinsing each sample 30 times in each cup. Each rinsing step
was done slowly so as not to damage the thinned area around
the hole. Some ethanol remaining on the tweezers with the
TEM sample was removed by blotting with a filter paper, and
the TEM sample was then put on another clean and dry filter
paper for 1 or 2 min to make it fully dry. These samples were
stored in labeled polyethylene vials to protect them from
mechanical damage and contamination. Each TEM samplewas investigated in detail under a Leica DM6000 M Model
optical microscope and Leica EC3 Model stereomicroscope;
images were recorded to describe the quality of the hole
formation.
3. Results and Discussion
3.1. Affect of Electropolishing Voltage
A stereomicroscopic view of the pure Al specimens, 200 m
thick and 3 mm in diameter, prepared using different
electropolishing voltage values, i.e., 16, 30, 45 and 60 V withthe constant pump flow rate of 15 (arbitrary units as indicated
on the polishing unit), is presented in Fig. 1ad. Increasing the
electropolishing voltage above 12 V resulted in specimens
with smooth and clean surfaces, and holes were successfully
obtained near to the center of the polished circle area. The
peripheral alterations around the polished circle area due to
the increase in voltage from 16 V through 60 V can be seen in
Fig. 1ad. No hole formation occurred at the central areas of
the specimens exposed to excessive voltages such as 45 and
60 V. Fig. 2 shows optical micrographs of the holes produced
and the general effect of increasing the electropolishing
voltage; again the failure to form a hole at 45 V is seen in
Fig. 1 Stereomicroscope views of high purity Al disks, 200 m thick and 3 mm diameter in size, after electropolishing at
different voltages (a) 16 V, (b) 30 V, (c) 45 V, and (d) 60 V. The peripheral alterations around the polished circular areas areshown
with arrows.
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Fig. 2f. After electropolishing at different voltages, elliptical
holes were observed, as seen from Fig. 2ae. It is also evident
that the voltage above 12 V resulted in wider holes (Fig. 2de).
The variation of the time for hole formation and the
calculated hole area of the high purity Al disks as a function of
the electropolishing voltage are shown in Fig. 3. As can be
seen,it is clear that thetime for hole formation decreases with
increasing the applied electropolishing voltage. The time for
hole formation of thespecimens prepared at the voltage range
from 8 to 12 V decreases sharply from 380 s to 106 s. This value
decreased further to 15 and 12 s when the specimens were
prepared at 45 and 60 V, respectively, although for the latter
specimens the holes were not centrally located.
Determination of the suitable and correct electropolishing
parameters is not easy due to the fact that these parameters
have a wide range that makes repeatability difficult. The
voltage adjustment needs to be done properly to achieve the
ideal electropolishing. During this process, the formation of an
anodic viscous layer of electrolyte on the specimen surface is
responsible for thinning. The ideal thinning will create a
smooth surface and polished specimen by removing both the
macroscopic bumps and microscopic irregularities, respec-
tively [12,15]. Although it is not resolvable in Fig. 3, the cal-
culated hole area increases fourfold from 0.0035 mm2 at 8 V to
Fig. 2 Optical micrographs showing the resulting holes after electropolishing at different voltages (a) 8 V, (b) 10 V, (c) 12 V,
(d) 16 V, (e) 30 V, and (f) 45 V.
Fig. 3 The variation of the time for hole formation and the
calculated hole area of the high purity Al disks as a function
of electropolishing voltage.
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0.0141 mm2 at 16 V. Above 16 V, the hole area increases by
nearly a factor of five to 0.06500.0186 mm2 at 30 V. Even
though there is no circular or elliptical shaped hole to be
studied for the specimens prepared at 45 and 60 V, the
calculated hole areas are approximately 1.49 and 5.08 mm2,
respectively. The excessive voltage results in electrolysis of
the aqueous solution which creates bubbles on the specimen
surface; consequently these bubbles mask the surface locallyand cause pitting[25].
3.2. Affect of the Pump Flow Rate
Figs. 4 and 5 show the optical micrographs of the holes of the
pure Al specimens, prepared using five different pump flow
settings, i.e., 5, 15,25, 35,and 45,at a constant electropolishing
voltage, 8 V. Smooth, clean and well-polished surfaces were
observed on the specimens prepared in the range of pump
flow rates from 5 to 35 (Figs. 4a, c, e, and 5a). The effect of the
high flow rates, 35 and 45, on the specimen surface is obvious
in Fig. 5b and Fig. 5d, respectively. In the range of the pump
flow between 5 and 35, the locations of the holes were usually
near to the central area of the TEM disks. The location of the
hole for the specimen prepared with a 45 pump flow rate was
further removed from the central area (Fig. 5c and d); the
higher pump flow rates caused torn elliptical shaped holes
(Fig. 5b and d) and led to the surface distortion seen in Fig. 5c.
Fig. 6 shows the variation of the time for hole formation
and the calculated hole area of the high purity Al disks as a
function of the pump flow setting. The values of the time for
hole formation significantly decrease from approximately610 s for a pump flow setting of 5 to approximately 240 s for
a pump flow setting of 25. When the pump flow was increased
through 45, the time for the hole formation slightly decreases
to about 210 s. The calculated hole area was determined as
0.0086 mm2 on average for the pump flow range from 5 to 25.
When the pump flow setting was increased from 25 to 45, the
calculated hole area significantly increased from 0.0120 mm2
to 0.1763 mm2. Fig. 6 also clearly shows that increasing the
pump flow rate from 5 to 25 resulted in a decrease in the time
for hole formation whereas no significant difference in the
values of the calculated hole areas was observed. An increas-
ing in the time for hole formation with a decrease of pump
flow rate from 25 to 5 indicates a delay in the polishing action
because of the presence of gas bubbles formed by anodic
Fig. 4Optical micrographs showing the holes after electropolishing at different pump settings: (a) and (b) 5, (c) and (d) 15, (e)
and (f) 25.
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dissolution of the metal, which remain in the polishing area
[26]. When the pump flow setting was increased from 25 to 45,
there was no significant change in the values of the time for
hole formation, but the values of the calculated hole areas
increased.
3.3. Affect of the Specimen Thickness
Fig. 7 shows optical micrographs of the holes produced in the
high purity Al disks starting with specimens thinned to five
different thicknesses, i.e., 70, 100, 150, 200 and 250 m, and
prepared using a constant 8 V electropolishing voltage and a
pump flow rate setting of 15. Elliptical-shaped holes were
produced in each, irrespective of starting thickness (Fig. 7ae).
In the present study, the thinnest specimen with a thickness
of 70 m (Fig. 7a) developed a larger hole and more etched
surface than thethicker specimens(Fig. 7be). The variation of
the time for hole formation and the calculated hole area of the
high purity Al disks as a function of the specimen thickness
are given in Fig. 8. The shortest time for hole formation, 84 s,
was observed with the 70 m thick specimens. This time
increased to about 130135 s, when the specimen thickness
increased to 100 and 150 m, respectively, and increased
further up to 440 s for specimen thicknesses from 150 m
through 250m. When the specimenthickness increased from
70 m to 100 m, the hole area decreased from approximately
0.009 mm2 to 0.003 mm2. However, for specimens thicknesses
greater than 100 m no further changes were observed.
4. Conclusion
The quality of the information from TEM analysis study is
directly related to the quality of the thin foils being examined.
Electropolishing is the most common and physically deforma-
tion-free specimen preparation technique available for exam-
ining electrically conductive materials. In the present study
the twin-jet electropolishing parameters for producing high-
quality disks of high purity Al were studied with the purpose
of both showing the effects of the polishing parameters,
achieving well-prepared reproducible TEM disks and adding
to the general knowledge basis for workers in this area of
scientific research. On the basis of the results reported in the
present investigations, the following conclusions can be drawn.
1. At a polishingvoltage range between8 and12 V, specimens
with smooth and clean surfaces and with holes near the
center of the polished area were successfully produced.
Fig. 5 Optical micrographs showing undesirable thin regions after electropolishing at different pump settings: (a) and (b) 35, (c)
and (d) 45.
Fig. 6 The variation of time for hole formation and the
calculated hole area of the high purity Al disks as a function
of the pump flow rate.
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2. It was clearly demonstrated that increasing the applied
electropolishing voltage resulted in decreasing the
required time for the hole formation. However, at higher
voltages, such as 45 and 60 V, the holes were unnecessarily
large and not centrally located in the disks.
3. Smooth, clean and well-polished surfaces were observed
on specimens prepared using the range of pump flow
settings from 5 to 35. Also, it was observed that the required
time for hole formation decreases with an increase of the
pump flow rate.
4. When the electropolishing voltage and the pump flow rateare maintained constant, there is a significant increase in
the specimen thickness; the variation in thesize of the hole
area is negligible due to the endpoint detection sensitivity
of the polishing unit.
5. An increase in the specimen thickness resulted in a signifi-
cant increase in the required time for the hole formation.
Acknowledgements
The author would like to thank Prof. Hseyin imenolu from
Istanbul Technical University for his help during the optical
and stereomicroscope investigations of this study. The author
Fig. 7 Optical micrographs showing the holes in the high purity Al disks thinned to five different thicknesses and prepared
using a constant 8 V electropolishing voltage and a pump setting of 15: (a) 70 m, (b) 100 m, (c) 150 m, (d) 200 m and (e)
250 m.
Fig. 8 The variation of time for hole formation and the hole
area of the high purity Al disks as a function of the sample
thickness.
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is grateful to Bernard J. Kestel for his supports on providing
the literature and sharing his own experience. In addition,
Santhana Eswaramoorthy and Eric Lass from University of
Virginia for their help on providing literature are gratefully
acknowledged. The author also would like to thank Dr. Brian
Gable for his helpful discussion.
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