synthesis and tribological properties of air plasma polymerized soybean oil with n-containing...
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ORIGINAL PAPER
Synthesis and Tribological Properties of Air Plasma PolymerizedSoybean Oil with N-Containing Structures
Xiaoyun Zhao • Jingyi Yang •
Dehua Tao • Xinru Xu
Received: 4 May 2013 / Revised: 12 January 2014 / Accepted: 24 January 2014
� AOCS 2014
Abstract In this study, polymerized oils with different
viscosity grades were synthesized by the polymerization of
soybean oil (SO) in an air plasma environment. The results
of the elemental analysis, infrared spectroscopy, and
pyrolysis gas chromatography revealed that the carbonyl,
organic amine, and nitrogen heterocyclic groups were
incorporated into the molecule of the polymerized oil
(PAIR9); the GPC chromatogram of this oil revealed that
the product consisted of dimers and oligomers with higher
molecular weights. The tribological behaviors of the
polymerized oils were evaluated using a four-ball friction
and wear tester. The maximum non-seizure loads of all the
polymerized oils surpassed that of SO, and the PB value of
PAIR9 reached 1,186 N. Meanwhile, PAIR9 exhibited
much better anti-wear performance when the tested loads
were lower than 350 N. The worn surfaces lubricated by
SO and PAIR9 were analyzed using the X-ray photoelec-
tron spectra (XPS). The results of the XPS analysis proved
that during the frictional process, the polymerized oil could
not only promote the adsorption of the oil on the metal
surface because of the oxygen-containing species (such as
esters and carbonyl groups) with higher polarities but also
promote the interactions with the metallic iron to form
compact and stable tribochemical films containing organic
nitrogen complexes.
Keywords Soybean oil � Plasma polymer � Viscosity �Organic amine � Lubricant � Tribology � XPS �Coordination complexes
Abbreviations
GPC Gel permeation chromatography
XPS X-ray photoelectron spectroscopy
Introduction
The development of environmentally friendly lubricants to
reduce our reliance on petroleum resources and protect the
ecology environment has garnered a global consensus.
Vegetable oils, which are renewable, biodegradable, and
less toxic to the environment as compared to mineral oils,
are important materials in preparing green lubricants.
Fernandez Rico [1] developed a method to enhance the
lubricity of polyalphaolefin by adding sunflower oil. Ratoi
[2] explained the film-forming behavior of fatty acids when
used as oiliness additives. In addition, vegetable oils have
higher dissolving capacities for additives as compared to
mineral oils. Ren [3–5] found that triazine derivatives when
used as additives show excellent lubricating behaviors in
rapeseed oil.
However, vegetable oils persist in having certain
drawbacks that need to be overcome, namely, poor
oxidative stability and poor low-temperature perfor-
mance; this complicates the use of vegetable oils as
biodegradable lubricants. Moreover, the viscosity ranges
of most vegetable oils (except castor oil) are very nar-
row, namely, ISO viscosity grades (VG) of 32 and 46
[6–8]. Several types of lubricant oils, such as gear oils
and hydraulic oils, need higher viscosities. Lathi [9] and
Erhan [10, 11] developed the ring-opening process of
X. Zhao � J. Yang � X. Xu (&)
Research Institute of Petroleum Processing, East China
University of Science and Technology, Meilong Road 130,
Shanghai 200237, People’s Republic of China
e-mail: [email protected]
D. Tao
School of Electromechanical Engineering and Automation,
Shanghai University, Yanchang Road 149, Shanghai 200072,
People’s Republic of China
123
J Am Oil Chem Soc
DOI 10.1007/s11746-014-2424-3
epoxidized soybean oil with alcohols and anhydrides to
improve the oxidative stability. Cermak [12, 13] syn-
thesized estolides from various fatty acids, which yielded
better low-temperature characteristics. By using anthra-
quinone as the catalyst, Guner [14] increased the vis-
cosity of anchovy oil through thermal polymerization.
Biswas [15] evaluated the lubricity of microwave-irra-
diated soybean oil with higher viscosity.
In recent years, the use of plasma polymerization for
fabricating special polymer materials has received
increased attention. Yasuda [16] studied the polymeri-
zation of acetylene using gases and vapors of H2O, N2,
and CO. Dilsiz [17] investigated the effects of plasma
discharge power, different atmospheres, and monomers
having different functional groups on the structures of
plasma polymers. With regard to biomedical applications,
the deposition of polyacrylic acid films using nitrogen
plasma jets at atmospheric pressure has been investigated
[18]. In this paper, air plasma produced in an original
reactor was employed to open the double bonds of SO
for preparing polymerized oils with higher molecular
weights and viscosities. The structure of the oil poly-
merized by air plasma was analyzed using elemental
analyzer, infrared (IR) spectroscopy, pyrolysis gas chro-
matography (Py-GC), and gel permeation chromatogra-
phy (GPC). The tribological behaviors of the
polymerized oils were evaluated on a four-ball friction
and wear tester. The lubricating mechanism of the
polymerized oil was discussed by analyzing the X-ray
photoelectron spectra (XPS) of the worn surface.
Experimental
Materials
In this study, the commercially available SO employed in
the polymerization process was provided by Shanghai
Liangyou Haishi Oils and Fats Industry Company, China.
The fatty acids of SO were primarily composed of unsat-
urated linolenic acids (C18:3, 2.69 %), linoleic acids (C18:2,
46.3 %), and oleic acids (C18:1, 26.6 %), which displayed a
higher degree of unsaturation; they also comprised satu-
rated stearic acids (C18:0, 6.78 %) and palmitic acids (C16:0,
15.0 %). The characteristics of SO were listed in Table 1.
Synthesis of the Polymerized Oils by Air Plasma
The plasma reactor employed to prepare the polymerized
oils used in this study is shown in Fig. 1. The major
components of this equipment were a non-pressurized
vessel containing two parallel graphite electrodes
(150 9 25 9 200 mm); the electrodes were separated
using two quartz glass plates (separation: 6 mm) that acted
as the dielectric medium. The plasma reactor was activated
using a plasma generator (CTP-2000K, Nanjing Suman
Electronics Co., Ltd.) that operated at a frequency of
7.30 kHz and had a deliverable power range from 0 to
500 W.
Approximately 300 mL of SO placed in a storage tank
at a constant temperature (90 �C) was pumped into the
reactor filled with air; the pumping was controlled to
obtain a circular flow at 160 mL/min. In the polymeri-
zation process, the plasma power was maintained at
120 W, and the frequency was adjusted to obtain glow
discharges. The polymerized oil samples were withdrawn
at predetermined times and the viscosities of the samples
were calculated.
Testing the Physicochemical Properties
The viscosities (at 40 and 100 �C) and viscosity index (VI)
were measured and calculated according to ASTM D445
and ASTM D2270, respectively. The iodine values, a
measure of the degree of unsaturation in fatty acids, were
determined according to ISO 3961:1996.
Structural Analysis of Polymerized Oil
Elemental Analysis
The elemental measurement of carbon (C) and hydrogen
(H) for the oil samples were conducted using the vario EL
cube elemental analyzer (Elementar Analysensysteme
GmbH, Germany). The Antek 9000 sulfur and nitrogen
fluorescence analyzer (Petroleum Analyzer Company,
USA) was used to determine the mass fraction of nitrogen
(N) in the polymerized oil, which was diluted by 100 times
using di(2-ethylhexyl)phthalate before the test. The per-
centage composition of oxygen (O) was calculated from
the analysis results of C, H, and N.
Table 1 Characteristics of air plasma polymerized soybean oil at
different reaction times
Sample Reaction
time (h)
Viscosity (cSt) Viscosity
index
Iodine value
(g I2/100 g)40 �C 100 �C
SO 0 33.8 7.84 215 130
PAIR1 1 48.4 10.1 203 125
PAIR3 3 111 16.6 162 104
PAIR5 5 307 40.5 186 79.8
PAIR7 7 645 49.2 130 74.3
PAIR9 9 1,136 68.6 123 69.8
J Am Oil Chem Soc
123
IR Spectroscopy
The polymerized oil of SO was analyzed using a Nicolet
6700 Fourier transform infrared spectrometer (Thermo
Fisher Scientific Inc., USA). The IR spectra were recorded
from 4,000 to 400 cm-1 at a resolution of 0.09 cm-1.
Pyrolysis of Oil Polymerized by Air Plasma
The oil sample was pyrolyzed using a PY-2020iD double-
shot pyrolyzer (Frontier Lab, Japan) coupled to a
GC7089A gas chromatograph (Py-GC). The detection was
carried out using a MS5975C mass selective detector
(Agilent, USA) (MSD, qualitative analyses). In the exper-
iment, the pyrolysis temperature was maintained at 500 �C
and the temperature was maintained constant for 20 s. The
GC oven temperatures were changed as follows: main-
tained at 40 �C for 2 min, increased at a rate of 10 �C/min
up to 310 �C, and finally maintained at 310 �C for 40 min.
Helium was used as the carrier gas as well as to create an
inert atmosphere in the pyrolysis interface.
GPC
The GPC was obtained using a Waters 1515 gel permeation
chromatograph equipped with a column (dimensions
300 9 7.5 mm), a manual injector and a Waters 2414
refractive index detector. The molecular weights were
calculated and calibrated using the polystyrene standards
obtained from the Waters Corp., USA. The polymerized
samples were dissolved in tetrahydrofuran, which was used
as the eluent with a flow rate of 1.00 mL/min at 40 �C and
an injection volume was 100 lL.
Friction and Wear Test
The tribological properties were determined at ambient
temperature on the MS-800 four-ball friction and wear
tester (Xiamen Tenkey Automation Company Limited,
China). GCr15-grade steel ball bearing (diameter:
12.7 mm; hardness: HRC 59–61; chemical composition: C,
0.95–1.05 %; Si, 0.15–0.35 %; Mn, 0.20–0.40 %;
P \ 0.027 %; S \ 0.020 %; Cr, 1.30–1.65 %; Ni \ 0.30
%; Cu \ 0.25 %) was used as the test material; it was
supplied by the Shanghai Steel Ball Plant, China.
Under the test conditions of a rotating speed of
1,450 ± 50 rpm for the duration of 10 s at room temper-
ature, the maximum non-seizure loads (PB value) were
measured according to GB 3142-82 (Chinese National
Standard) similar to ASTM D-2783. The anti-wear tests
were carried out at a rotating speed of 1,450 ± 50 rpm and
different loads of 98, 196, 294, and 392 N for a duration of
30 min. The wear scar diameters (WSD; accuracy:
±0.01 mm) of the three lower test balls were determined
Oil Inlet
Oil OutletGas Inlet
Gas Outlet
Oil Chamber
Oil Chamber
Discharge Gap
Gas Blast Pipe
Electrode Plate
Earth Terminal
High VoltageTransmissionLine Terminal
Fig. 1 The schematic of the plasma reactor
J Am Oil Chem Soc
123
using an optical microscope. In this paper, the average
WSD values of the three lower balls were noted. The
friction coefficients were measured and recorded indirectly
using a friction torque tester. Each test was repeated at least
three times.
Friction Surface Analysis
The original non-wear (NW) and wear surfaces of the steel
balls were analyzed using a PHI-5702 multi-functional
X-ray photoelectron spectroscope (PerkinElmer, USA).
Before conducting the XPS analysis, the upper balls
lubricated by SO and PAIR9 under a load of 294 N for the
duration of 30 min were ultrasonically washed with
petroleum ether. The binding energies and compositions of
C1s, O1s, N1s, and Fe2p on the worn surfaces of the upper
balls were detected by using the Al Ka X-rays as the
excitation source with a pass energy of 29.35 eV. The
binding energy of the contaminated C (C1s: 284.60 eV)
was used as a reference, and the vacuum degree during
testing was maintained lower than 1 9 10-8 Torr.
Results and Discussion
Effect of Reaction Time on the Properties of Oils
Polymerized by Air Plasma
The effect of the reaction time on the characteristics of
polymerized oils was investigated in Table 1, keeping all
other plasma operational parameters constant. The results
revealed the expected effects of the air plasma on the
viscosity and unsaturated degree of SO. The viscosities (at
both 40 and 100 �C) of the polymerized oils increased with
rising reaction time, while the iodine values followed an
opposite trend. All the characteristics of the polymerized
oils were listed in Table 1. Although the VI value of the
polymerized oil (PAIR9), with a reaction time of 9 h,
decreased from 215 to 123, its viscosity at 40 �C increased
from 33.8 to 1136 cSt and that at 100 �C increased from
7.84 to 68.6 cSt. Meanwhile, its iodine value decreased
from 130 to 69.8 g I2/100 g (Table 1). This result indicated
that the opening of the double bonds in SO by the air
plasma caused an increase in the viscosities of polymerized
oils.
The change in the elemental compositions of the poly-
merized oil with the reaction time for polymerization is
shown in Fig. 2. It was noteworthy that the contents of both
C and H decreased with an increase in the reaction time,
while the O and N contents increased with the reaction
time. Furthermore, within the same reaction time, the
increase in the O content of the polymerized oil surpassed
that in the N content. In particular, the O content of PAIR9
increased from 12.65 to 19.07 %, while its N content
reached only 0.52 %. This significant difference between
the elemental increments of the O and N contents can be
attributed to the dissociation energies of O2 and N2. As we
know, N2 possesses a higher dissociation energy (9.8 eV),
but that of O2 is only 5.1 eV [19]. Therefore, in the pre-
sence of air plasma, the O2 molecule can easily participate
in the polymerization process. In other words, it can be
concluded that N2 and O2 in air, which were originally used
in the experiment to function as the reactive gases, par-
ticipated in the plasma polymerization of SO; conse-
quently, nitrogen and oxygen atoms were incorporated into
the molecules of SO during the polymerization process.
0 2 4 6 8 1012.0
13.6
15.2
16.8
18.4
20.0
O atom
Con
tent
s of
oxy
gen
(%)
Reaction time (h)
0 2 4 6 8 1070.0
71.8
73.6
75.4
77.2
79.0
C atom
Con
tent
s of
car
bon
(%)
Reaction time (h)
9.00
9.36
9.72
10.08
10.44
10.80
H atom
Con
tent
s of
hyd
roge
n (%
)
0.00
0.17
0.34
0.51
0.68
0.85
N atom
Con
tent
s of
nitr
ogen
(%
)
Fig. 2 Contents of all elements
of air plasma polymer versus the
reaction time
J Am Oil Chem Soc
123
IR Characterization of Air Plasma Polymerized Oil
The IR spectra of PAIR9 prepared under the air plasma
conditions are compared with those of SO in Fig. 3. It was
shown that the IR spectra of SO exhibited a few peaks at
3,008.8 cm-1 (=C–H stretching vibration), 2,925.6 and
2,854.6 cm-1 (CH2 asymmetric stretching), 1,745.5 cm-1
(C=O triglycerides carbonyl stretching), 1,653.1 cm-1
(C=C stretching vibration), 1,461.0 cm-1 (CH2 bending
vibration), 1,374.5 cm-1 (CH3 symmetrical bending
vibration), and 722.7 cm-1 (CH2 rocking vibrations);
additional peaks were observed at 1,236.7, 1,163.3, and
1,098.8 cm-1 due to the stretching vibrations of the C–O
group in the esters.
However, the two absorption peaks at 1,653.1 (C=C)
and 3,008.8 cm-1 (=C–H) in the IR spectra of PAIR9
exhibited a marked decay, probably because of the opening
of the double bonds in the triacylglycerol molecules.
Meanwhile, the formation of new groups in the polymer-
ized oil, which was induced by the air plasma, was
observed in the IR spectra of PAIR9. The region with the
broad and fairly strong signal at 3,470.7 cm-1 can be
attributed to the N–H stretching vibration. In addition, the
two sharp characteristic peaks at 1,630.8 and 1,552.5 cm-1
can be identified as the N–H bending vibration of the fatty
primary and secondary amines, respectively. The peak at
1,274.1 cm-1 can be assigned to the C–C stretching
vibration of the C–C(=O)–C groups in the aliphatic ketone
molecule. The peak at 862.6 cm-1 can be identified as the
N–H rocking vibration. Therefore, it can be concluded that
the free radicals in the long-chain molecules, which were
formed by the opening of the double bonds under the
plasma conditions, could capture the N2 and O2 molecules
to produce and incorporate ‘‘amine-like’’ and carbonyl
groups into the polymerized oils.
Moreover, in the IR spectra of PAIR9, a small charac-
teristic peak was visible at 972.1 cm-1, which was the
=CH bending vibration of the trans-conjugated system. It
means that under the effect of air plasma, the isolated cis-
double bonds in the hydrocarbon chains of the linolenic
and linoleic acids migrate to the conjugated position and
yield the structure of the conjugated dienes.
Pyrolysis of Air Plasma Polymerized Oil
To additionally clarify the structure of the nitrogen-con-
taining groups, PAIR9 was pyrolyzed by pyrolysis gas
chromatography along with a mass selective detector (Py-
GC/MSD). The nitrogen-containing compounds in the
pyrolysis products of PAIR9 were mainly characterized by
primary and secondary amines, with relative contents
(calculated by normalizing the peak areas) of 4.07 and
2.89 % (Table 2), respectively. These results were almost
consistent with the above explanations regarding the IR
characterization of PAIR9. Meanwhile, minor amounts of
quaternary amines, acid amides and nitrogen heterocyclic
compounds were also observed. Therefore, organic amines
and nitrogen heterocyclic species were identified as the
nitrogen-containing groups.
In addition, 2.64 % cyclic compounds with side chains
were observed in the pyrolysis products of PAIR9
(Table 3). These cyclic compounds were produced by the
Diels–Alder addition between the isolated double bonds
and conjugated dienes.
GPC Analysis
Air plasma polymerized products of SO yielded complex
mixtures that might comprise monomers, dimers, trimers,
and oligomers with higher molecular weights; therefore,
1745
.5
4000 3400 2800 2200 1600 1000 400
722.
7
1098
.811
63.312
36.713
74.5
1461
.0
1653
.1
2854
.629
25.6
3008
.8
SO
Wavenumbers (cm-1)
862.
6
972.
1
1274
.1
1552
.516
30.834
70.7
PAIR 9
Fig. 3 The IR spectra of SO
and PAIR9
J Am Oil Chem Soc
123
GPC was performed on PAIR9 to determine the relative
content of each component and to determine the extent of
plasma polymerization (Fig. 4). Three fractions were sep-
arated from the polymerized product. The molecular
characteristics of these fractions are summarized in
Table 4. Fraction 1, which had a similar molecular weight
and retention time as that of SO, was identified as the
unreacted monomer, which was probably due to the pre-
sence of triglyceride molecules containing fatty acids
without double bonds (palmitic and stearic acids) and with
only one weakly polymerizable double bond (oleic acid).
Apart from the monomer, PAIR9 comprised 17.1 % dimers
(fraction 2) and 44.6 % oligomers (fraction 3), with num-
ber average molecular weights (Mn) of 2,201 and 5,964,
respectively. Obviously, the retention time of the polymer
peak on the GPC chromatogram decreased with increasing
molecular weight of the product. The higher viscosity of
PAIR9 can be attributed to the presence of oligomers with
the broad molecular weight distribution and polydispersity
(Mw/Mn) of 1.54. Therefore, it was concluded that the
presence of air plasma promoted the polymerization pro-
cess of SO.
Tribological Performances
The tribological characteristics of polymerized oils with
different viscosity grades were evaluated using a four-ball
friction and wear tester and the obtained results were com-
pared with those of SO. The PB values of the polymerized
products are shown in Fig. 5. It was interesting to note that all
the products obtained through the treatment of SO by air
plasma exhibited better load-carrying capacities as com-
pared to the untreated SO. Further, the higher the viscosity of
the product, the higher the PB value. Moreover, The PB value
of PAIR9 reached 1,186 N. The difference in the load-car-
rying capacity could be related to the molecular structure and
active elements of the polymerized products under air
plasma conditions. First, the higher viscosity indicated that
the product possessed a longer molecular chain, which could
maintain a sufficiently thick lubricant film on the metal
surface. Moreover, the incorporated O- and N-containing
species were often used as lubricant additives [20, 21] such
that the polymerized oils were able to withstand extreme
pressures and exhibit excellent anti-wear capabilities. It was
known that the polarity of the ester, carbonyl and amines
Table 2 Major peaks of N-containing compounds in pyrolysis mass spectra of PAIR9
GC number Pyrolysis products Formula Relative intensity (% of total)
2/3 NH2 C3H9N 3.25
5 HN
C4H9N 2.73
15 N C6H11N 0.34
33
NO C5H9NO 0.25
52 HN
C4H9N 0.16
55HN
O C7H11NO 0.43
64
O
NH2 O C5H9NO2 0.23
72
H2NOH
O
O C4H5NO3 0.09
73
N NH
N NH2
HN
C3H7N5 0.22
83NH2H2N
C6H14N2 0.59
J Am Oil Chem Soc
123
groups could be arranged in the following order: amine [carbonyl [ ester. Therefore, the presence of the carbonyl
and amine structures with considerably stronger polarities in
the polymerized products could get easily adsorbed on the
metal surface, and react with the metal surface to develop an
additionally durable tribochemical film during the rubbing
process.
The WSD values of the steel balls lubricated with SO,
PAIR7, and PAIR9 as a function of the tested load are shown
in Fig. 6a. It was evident that the WSD values of all these
base stocks increased with increasing tested load; when the
tested load was maintained at a value lower than 350 N, both
PAIR7 and PAIR9 demonstrated much better anti-wear
abilities than that of SO. The WSD values (294 N) of PAIR7
and PAIR9 were only 0.41 and 0.42 mm, respectively, while
that of SO reached 0.57 mm. The O- and N-containing
structures of the polymerized oils played a key role in
improving the anti-wear behavior. However, the anti-wear
abilities of the products deteriorated when the tested load
surpassed 350 N: the WSD values (at 392 N) of PAIR7 and
PAIR9 reached 0.68 and 0.72 mm, respectively, which were
higher than that of SO, namely, 0.60 mm. This can be
attributed to the fact that under the boundary lubrication
conditions, the competitive nature of the adsorption char-
acteristics of the carbonyl and nitrogen-containing groups on
the metal surface might render the boundary lubricating film
unstable and no longer compact.
The friction-reducing properties of these lubricant base
stocks are shown in Fig. 6b. It was observed that the fric-
tion coefficient (f) of SO increased with the applied load,
Table 3 Major peaks of cyclic structures in pyrolysis mass spectra of PAIR9
GC number Pyrolysis products Formula Relative intensity (% of total)
17 O C6H10O 0.22
29 O C7H12O 0.26
42 C8H14 0.21
44 C14H28 0.40
56O
C9H14O 0.20
82 C16H30 0.18
104 HO C10H18O 0.06
106
HO
HO C10H20O2 0.08
100/108/114 C11H20 0.41
110 HO C11H22O 0.23
146 C20H40 0.24
147 C29H48 0.15
J Am Oil Chem Soc
123
while the friction coefficients of both the polymerized oils
followed an opposite trend. At lower loads, both these oils
exhibited higher friction coefficients, which can be attrib-
uted to the higher viscosities of the polymerized oils; this
was not suitable to reduce the energy loss from the lubri-
cation system. However, the friction-reducing perfor-
mances of the polymerized oils were superior to that of SO
at higher loads. In particular, the f294N and f392N of PAIR7
were 0.0682 and 0.0736, respectively. These results indi-
cated that at higher loads, the active elements (O and N) in
the polymer molecules formed an effective tribochemical
adsorption film with low shear strength, thereby resulting
in the lower friction coefficients.
Worn Surface Analysis
To study the lubricating mechanism of the air plasma
polymerized oil comprising carbonyl and N-containing
groups, the XPS analysis of the worn surfaces of the
steel balls lubricated by PAIR9 and SO was carried out
and the obtained results were compared with the original
NW surface of the steel ball. The binding energies of
C1s, O1s, Fe2p, and N1s on the worn surface are shown in
Fig. 7. It was observed that the XPS spectra of C1s and
Fe2p exhibited peaks at the binding energies of 284.8,
707.3, and 710.3 eV, which were attributed to the pre-
sence of C*–C, iron (Fe), and Fe2O3 [22–24], respec-
tively. The above facts indicated during the frictional
process, both SO and PAIR9 adsorbed on the metal
surface to form lubricant films with certain thicknesses.
Meanwhile, the relative concentrations of the C atom on
the worn surface lubricated by SO and PAIR9 increased
from 10.6 to 44.1 % and 86.4 %, respectively, while the
relative concentrations of Fe on the worn surface of SO
and PAIR9 decreased from 39.2 to 28.9 % and 3.20 %
(Table 5), respectively. Obviously, the film formed using
PAIR9 was sufficiently thick to cover the metal surface
for reducing the consequent wear; this advantage can be
attributed to the longer hydrocarbon chain of the PAIR9
molecules.
The O1s spectra of the original NW surface exhibited a
peak at 530.2 eV; this peak was present in the binding
energy range of a metal oxide (529.8–530.2 eV) [25], such
as those of Fe2O3 and Fe3O4. Therefore, this peak can be
attributed to iron oxides. However, it was obvious that the
intensities of O1s peaks on the worn surfaces lubricated by
both SO and PAIR9 decreased. The binding energy
(531.4 eV) of the distinctive peak in the O1s spectra of SO
0.0 6.6 13.2 19.8 26.4 33.0-30
-15
0
15
30
45
SO PAIR9
Res
pons
e
Minutes
Monomer
Fraction 1
Fraction 2
Fraction 3
Fig. 4 GPC chromatogram of SO and PAIR9
Table 4 The molecular weight distribution of SO and PAIR9
Sample Distribution Mna Mw
b Polydispersityc Relative composition (%)
SO Monomer 1,396 1,440 1.03 100
Fraction 1 1,051 1,093 1.04 38.3
PAIR9 Fraction 2 2,201 2,243 1.02 17.1
Fraction 3 5,964 9,158 1.54 44.6
a Number average molecular weightb Weight average molecular weightc Polydispersity: Mw/Mn
SO PAIR1 PAIR3 PAIR5 PAIR7 PAIR90
280
560
840
1120
1400
1186
1049
882.0803.6
774.2
Base stocks
Loa
d-ca
rryi
ng c
apac
ity (
P B v
alue
, N)
646.8
Fig. 5 The load-carrying capacities of air plasma polymers with
different viscosity
J Am Oil Chem Soc
123
75 145 215 285 355 4250.065
0.074
0.083
0.092
0.101
0.110 SO PAIR7 PAIR9
Fric
tion
coef
fici
ent
Load (N)
75 145 215 285 355 4250.20
0.32
0.44
0.56
0.68
0.80
(b)
SO PAIR7 PAIR9
Wea
r sc
ar d
iam
eter
(m
m)
Load (N)
(a)Fig. 6 The wear and friction
properties of SO, PAIR7 and
PAIR9
300 296 292 288 284 2800
600
1200
1800
2400
3000
(c)
(b)
284.8 C1s
Inte
nsity
Binding energy (eV)
(a)
(a)
(b)
(c)
740 732 724 716 708 7001500
2900
4300
5700
7100
8500
(c)
Fe2p
Inte
nsity
Binding energy (eV)
710.3
707.3(a)
(b)
(c)
545 541 537 533 529 5250
1200
2400
3600
4800
6000
O1s
Inte
nsity
Binding energy (eV)
532.3531.4
529.9
414.0 409.8 405.6 401.4 397.2 393.0375
387
399
411
423
435
N1s
Inte
nsity
Binding energy (eV)
399.8
398.5
Fig. 7 XPS spectra of typical elements in tribofilms: a NW, b SO, c PAIR9
J Am Oil Chem Soc
123
did not exist in the range of that of a purely organic oxygen
(532.0–533.9 eV) [26] and was consistent with the O1s
binding energy of metal complexes, such as Fe(1-H-2,4-
pentanedione)3 (531.7 eV) and Fe(1-phenyl-1,3-butanedi-
onate)3 (531.6 eV) [27, 28]; this indicated that the oxygen
in SO and Fe combined together in a coordination bond
similar to the aforementioned two metal complexes.
Therefore, it can be concluded that the breakdown of SO
molecules during the tribochemical process resulted in the
formation of fatty acids, which could interact with the
metallic iron to produce iron carboxylate complexes.
However, iron carboxylate complexes were not observed in
the O1s spectra of PAIR9, and only one peak corresponding
to O*=C–O or O*=C appeared at 532.3 eV. The results
suggested that the O-containing species in PAIR9 mole-
cules exist only on the worn surface in the adsorbed forms.
In addition, the binding energies of N1s on the worn sur-
face of PAIR9 were in two forms with the binding energies of
398.5 and 399.8 eV: the binding energy of 398.5 eV was
assigned to the adsorbed forms of organic amine groups in
the PAIR9 molecules, whereas the binding energy of
399.8 eV was identified to exist because of the presence of
organic nitrogen complex compounds of metallic iron with
N-containing compounds [29, 30]. The relative concentra-
tion of the N atoms on the worn surface lubricated by PAIR9
also reached approximately 1.27 % (Table 5). In other
words, the N-containing species of the air plasma polymer-
ized oil could adsorb onto the metal surface prior to the
O-containing species. Simultaneously, the N atoms with the
lone pair electrons in the organic amine and nitrogen het-
erocyclic structures of PAIR9 possessed a strong coordinate
capacity, and these electrons could combine with the empty
orbital of the metal Fe to form a stable and compact coor-
dinated complex film on the metal surface during the rubbing
process. The insights were consistent with those concluded
by previous studies [31, 32].
Conclusions
The effects of air plasma on the physicochemical prop-
erties and the structure of SO were investigated. It was
proven that the air plasma could not only increase the
molecular weight to yield polymers with higher viscos-
ities by opening the double bonds of SO but also assist
in the incorporation of the carbonyl, organic amine and
nitrogen heterocyclic functional groups with stronger
polarities into the molecules of the obtained polymerized
oil. The tribological tests indicated that the polymerized
oil displayed significantly improved extreme pressure
properties and anti-wear characteristics. The results of
the XPS analysis proved that a majority of the oxygen-
containing groups in the plasma polymer, such as esters
or carbonyl groups, existed in the adsorbed form in the
boundary film. Meanwhile, the nitrogen-containing
structures with the lone pair electrons could combine
with the metal Fe to form complex films containing
organic nitrogen on the metal surface. The synergistic
effect of the carbonyl and nitrogen-containing groups in
the plasma polymer promoted the effective covering of
the inner iron oxide by the chemical adsorbed film,
thereby reducing the wear on the metal surface.
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