Zheng Cao1,2,3,4, Guangwei Lu2, Hongxin Gao2, Zhiyu Xue2, Keming Luo2, Kailun Wang2, Junfeng Cheng2, Qingbao Guan1, Chunlin Liu2,3,4, Ming Luo5. 1. Key Laboratory of High Performance Fibers & Products, Ministry of Education, Donghua University, Shanghai 201620, P. R. China. 2. Jiangsu Key Laboratory of Environmentally Friendly Polymeric Materials, School of Materials Science and Engineering, Jiangsu Collaborative Innovation Center of Photovoltaic Science and Engineering, Changzhou University, Changzhou 213164, Jiangsu, P. R. China. 3. Changzhou University Huaide College, Changzhou 213016, P. R. China. 4. National Experimental Demonstration Center for Materials Science and Engineering (Changzhou University), Changzhou 213164, P. R. China. 5. School of Materials Engineering, Changshu Institute of Technology, Changshu, Jiangsu 215500, P. R. China.
Abstract
In this study, using molybdenum sulfide (MoS2) as laser-sensitive particles and poly(propylene) (PP) as the matrix resin, laser-markable PP/MoS2 composite materials with different MoS2 contents ranging from 0.005 to 0.2% were prepared by melt-blending. A comprehensive analysis of the laser marking performance of PP/MoS2 composites was carried out by controlling the content of laser additives, laser current intensity, and the scanning speed of laser marking. The color difference test shows that the best laser marking performance of the composite can be obtained at the MoS2 content of 0.02 wt %. The surface morphology of the PP/MoS2 composite material was observed after laser marking using a metallographic microscope, an optical microscope, and a scanning electron microscope (SEM). During the laser marking process, the laser energy was absorbed and converted into heat energy to cause high-temperature melting, pyrolysis, and carbonization of PP on the surface of the PP/MoS2 composite material. The black marking from carbonized materials was formed in contrast to the white matrix. Using X-ray diffraction (XRD), Fourier transform infrared (FT-IR) spectroscopy, and Raman spectroscopy, the composite materials before and after laser marking were tested and characterized. The PP/MoS2 composite material was pyrolyzed to form amorphous carbonized materials. The effect of the laser-sensitive MoS2 additive on the mechanical properties of composite materials was investigated. The results show that the PP/MoS2 composite has the best laser marking property when the MoS2 loading content is 0.02 wt %, the laser marking current intensity is 11 A, and the laser marking speed is 800 mm/s, leading to a clear and high-contrast marking pattern.
In this study, using molybdenum sulfide (MoS2) as laser-sensitive particles and poly(propylene) (PP) as the matrix resin, laser-markable PP/MoS2 composite materials with different MoS2 contents ranging from 0.005 to 0.2% were prepared by melt-blending. A comprehensive analysis of the laser marking performance of PP/MoS2 composites was carried out by controlling the content of laser additives, laser current intensity, and the scanning speed of laser marking. The color difference test shows that the best laser marking performance of the composite can be obtained at the MoS2 content of 0.02 wt %. The surface morphology of the PP/MoS2 composite material was observed after laser marking using a metallographic microscope, an optical microscope, and a scanning electron microscope (SEM). During the laser marking process, the laser energy was absorbed and converted into heat energy to cause high-temperature melting, pyrolysis, and carbonization of PP on the surface of the PP/MoS2 composite material. The black marking from carbonized materials was formed in contrast to the white matrix. Using X-ray diffraction (XRD), Fourier transform infrared (FT-IR) spectroscopy, and Raman spectroscopy, the composite materials before and after laser marking were tested and characterized. The PP/MoS2 composite material was pyrolyzed to form amorphous carbonized materials. The effect of the laser-sensitive MoS2 additive on the mechanical properties of composite materials was investigated. The results show that the PP/MoS2 composite has the best laser marking property when the MoS2 loading content is 0.02 wt %, the laser marking current intensity is 11 A, and the laser marking speed is 800 mm/s, leading to a clear and high-contrast marking pattern.
Poly(propylene)
(PP) is a typical thermoplastic. Due to excellent
heat resistance, high chemical stability, resistant ability to most
acid and alkali corrosions, and good processability, PP and its composite
materials have been widely used in automobiles, packaging, membrane
separation and pipelines, and other fields.[1−4] Generally, the surface of PP products
needs to be marked with patterns and texts such as two-dimensional
(2D) codes and serial numbers to indicate the production date, company
logo, the product expiration date, and anticounterfeiting functions.
Usually, ink printing is used to produce these marks on the surface
of the material, but there is the use of toxic and harmful reagents,
the process flow is complicated, and there are serious environmental
pollution problems.[5,6] In recent years, laser marking
technology has emerged as a new type of printing technology that uses
high-energy lasers to mark the surface of materials to form patterns,
text, crystalline and self-assembly structures, and morphology.[6−12] For example, Park et al.[13] reported the
laser-directed supramolecular assembly of sub-5 nm columnar structures
with adjustable orientation control. The high energy of the laser
causes the matrix resin to be heated and carbonized, forming a clear
pattern[14,15] of carbonization and blackening on the surface
of the material. Because laser marking has a fast processing speed
and flexibility, it is highly suitable for marking the surface of
plastic products and can overcome the defects caused by ink printing.
After the product is completed, no additional processing is required,
and a clear, beautiful, and durable pattern appearance can be obtained
by directly performing laser printing.Laser marking is characterized
by noncontact processing. The laser
with a wavelength of 1064 nm is a more commonly used laser in the
industry and is suitable for materials such as metal, ceramics, wood,
and plastic.[16−19] Compared with the easy carbonization and high char residue features
of polycarbonate[20] and polystyrene,[21] it is rather difficult to perform laser marking
with PP itself due to the poor absorption of the near-infrared laser
energy of the 1064 nm wavelength. Usually, the method of adding laser
marking additives can effectively improve the laser marking performance
of PP. General laser marking additives used in industrial production
include inorganic laser marking additives, which are mostly metal
oxide powders,[22] such as ferroferric oxide
(Fe3O4),[23] bismuth oxide (Bi2O3),[24,25] bismuth oxychloride
(BiClO),[26] antimony trioxide (Sb2O3),[27] graphene,[28,29] montmorillonite,[30] carbon nanotube,[31] and other inorganic fillers. After laser irradiation,
the composite material undergoes color changes on its surface by absorbing
the laser energy. At present, there are only a few organic laser additives
reported, which are mainly halogen-containing organic compounds, color
masterbatches, and organic dyes,[32] causing
serious environmental pollution. The other type of laser additive
is inorganic/organic composite laser marking particles. Most of the
composite additives are formed by coating a layer of easily carbonized
polymers, such as antimony-doped tin oxide@polyimide (ATO@PI),[33] polystyrene-grafted antimony trioxide (PS@Sb2O3),[34] stannic oxide/polycarbonate
(SnO2/PC) microcapsules,[35] and
graphene/polystyrene, on the inorganic particles.[36] The core of the inorganic particles can effectively absorb
laser energy, which makes it easy to carbonize the polymer of the
shell layer, enhances the laser absorption of the matrix resin, and
improves the definition of laser marking. In addition, the use of
polymer-encapsulated modified inorganic particles, due to the existence
of the organic polymer shell, can make the core–shell structure
particles more compatible with the matrix resin material so that they
can obtain better mechanical properties.[37−39] Looking for
new inorganic laser-sensitive particles with the near-infrared laser
response performance and introducing them into PP to prepare PP/inorganic
composite materials with both laser-markable performance and excellent
mechanical properties have also been research hotspots recently.Single-layer MoS2 is a typical layered metal disulfide
and has been reported as a new type of near-infrared absorber.[40] The MoS2 absorber in the near-infrared
region has higher absorbance than both graphene and gold nanorods.[41] Due to the advantages of wider absorption bands,
better stability, excellent photoelectric performance, and a unique
two-dimensional structure, MoS2 has been widely used in
near-infrared photothermal therapy, electronics, catalysis,[42,43] and antibacterial applications.[44−46] In our study, the introduction
of MoS2 into PP resin to prepare composite materials and
the laser marking performance have not been reported yet. In this
design, using MoS2 as a laser marking additive and PP as
the matrix resin, PP/MoS2 composite materials were prepared
by melt-blending with different contents of MoS2. Considering
that the addition of MoS2 laser marking additives affects
the mechanical properties of PP, the optimum ratio of PP/MoS2 is also determined. The near-infrared laser response performance
of the composite material was studied by controlling the content of
laser additives, laser current intensity, and laser scanning speed.
The color difference tests, a metallographic microscope, an optical
microscope, a SEM, X-ray diffraction (XRD), FT-IR and Raman spectroscopies,
and mechanical performance measurements were used to characterize
the surface morphology, marking performance and mechanism, and mechanical
properties of PP/MoS2 composites. This research is of great
importance for the realization of high-functionality and high-performance
applications of PP-based materials and meets the high-quality marking
needs of characters, patterns, and QR codes on the surface of PP products
in the fields of automobiles, medical equipment, and precision instruments.
Results and Discussion
Laser-Markable Performance
of Pure PP
PP was directly pressed into sheet samples for
laser marking without
adding MoS2. Figure shows the response performance of pure PP before and after
laser marking. The laser current intensities of 8, 9, 10, 11, and
12 A were chosen to mark the pure PP sheets. Note that the marking
pattern of a cartoon bird was selected for this experiment. From Figure , it can be found
that at a very low laser current intensity of 8 A, there are hardly
any changes between the unmarked and marked PP samples. As the laser
current intensity is increased to 11 A, black particles and a blurred
marking pattern appear on the PP surface. More black particles appear
at a higher laser current intensity of 12 A. When the marking current
intensity is low, the color contrast between the marking and the substrate
is low. When the color of the printed pattern differs greatly from
the color of the substrate, the surface of the material seems carbonized,
the laser current intensity required is also large, and more energy
is consumed. Therefore, pure PP cannot display a clear pattern under
a small laser current intensity, and it is necessary to add suitable
laser marking additives to improve the markability of the PP material.
Figure 1
Visual
appearance of PP before and after marking at different laser
marking current intensities ((a) 0 A, (b) 8 A, (c) 9 A, (d) 10 A,
(e) 11 A, (f) 12 A; scale bar of 1 cm).
Visual
appearance of PP before and after marking at different laser
marking current intensities ((a) 0 A, (b) 8 A, (c) 9 A, (d) 10 A,
(e) 11 A, (f) 12 A; scale bar of 1 cm).
Effect of the Laser Marking Process and MoS2 on the Laser Marking Property of PP/MoS2 Composites
Effect of MoS2 Content on the
Laser Marking Property
MoS2 with different contents
(0.005, 0.01, 0.015, 0.02, and 0.2%) was added to the PP matrix by
the melt-blending method to prepare the PP/MoS2 composite
material for laser marking. The purpose of this research is to obtain
the PP/MoS2 composites with excellent laser marking performance
and mechanical properties. The MoS2 loading content is
expected to be as low as possible because the addition of black MoS2 powder particles with a content higher than 0.2% influences
the color of the matrix and probably decreases the mechanical property
of PP. Therefore, in our case, the MoS2 loading contents
of 0.005–0.2% were chosen for the experiments. Figure shows the visual appearance
of the laser marking of pure PP and PP composites containing different
contents of MoS2 at the same laser current intensity of
11 A and the same scanning speed of 800 mm/s. Compared with the fuzzy
pattern produced on the pure PP surface, the PP composite material
with MoS2 added shows sensitivity to laser absorption,
and the laser marking pattern becomes much clearer. At a very low
MoS2 content of 0.005%, a clear marking pattern of a cartoon
bird is displayed. As the content of MoS2 increases, the
pattern contrast remains unchanged. As the content increases to a
higher content of 0.2%, the pattern contrast decreases and it is difficult
to recognize the pattern. The main reason for this is that MoS2 is black powder particles, and the addition of the black
pigment makes the color of the matrix black. It is difficult to make
precise comparisons by visual observation alone; therefore, a colorimeter
is used for the quantitative analysis below.
Figure 2
Visual appearance of
(a) pure PP, (b) 0.005% PP/MoS2, (c) 0.01% PP/MoS2, (d) 0.015% PP/MoS2, (e)
0.02% PP/MoS2, and (f) 0.2% PP/MoS2 composite
materials after laser marking at the laser current intensity of 11
A and a marking speed of 800 mm/s (scale bar of 1 cm).
Visual appearance of
(a) pure PP, (b) 0.005% PP/MoS2, (c) 0.01% PP/MoS2, (d) 0.015% PP/MoS2, (e)
0.02% PP/MoS2, and (f) 0.2% PP/MoS2 composite
materials after laser marking at the laser current intensity of 11
A and a marking speed of 800 mm/s (scale bar of 1 cm).Figure shows
the
laser marking color difference values of PP/MoS2 composites
with different MoS2 loading contents at 800 mm/s and 11
A for quantitative analysis of the laser marking property of composites.
As shown in Figure , the color difference values (ΔE) measured
of the laser marking patterns on composites with MoS2 loadings
of 0.005, 0.01, 0.015, 0.02, and 0.2% are 12.82, 12.47, 11.87, 13.47,
and 2.72, respectively. This result is in agreement with the observation
mentioned above. This means that the laser marking property depends
on the proportion of MoS2. When the MoS2 loading
content is 0.2%, the color of the matrix material becomes much darker
due to the excessively high MoS2 content, resulting in
a decrease in the contrast of the marking and a lower color difference.
When the concentration is 0.02%, the laser marking color difference
value reaches the maximum value of 13.47, and the highest color contrast
between the marking area and the matrix material can be obtained,
leading to the best laser marking performance.
Figure 3
Laser marking color difference
values of PP/MoS2 composites
with different MoS2 loading contents at 800 mm/s and 11
A.
Laser marking color difference
values of PP/MoS2 composites
with different MoS2 loading contents at 800 mm/s and 11
A.
Effect
of the Laser Current Intensity on
the Laser Marking Property
The laser marking current intensity
is the most important parameter in the laser marking process. A suitable
laser marking current intensity can save energy consumption while
ensuring a favorable laser marking effect. Figure shows the visual appearance of 0.02% PP/MoS2 composite materials after laser marking at different laser
current intensities of 8, 9, 10, 11, and 12 A and the marking speed
of 800 mm/s. It can be seen from Figure that as the laser current intensity of the
laser marking increases from 8 to 11 A, the laser marking pattern
becomes much clearer and the contrast is higher obviously. After the
laser marking current intensity is greater than 11 A, the pattern
definition decreases. Similarly, the color difference analysis for
the detailed comparison was carried out in the following discussion.
Figure 4
Visual
appearance of 0.02% PP/MoS2 composite materials
after laser marking at different laser current intensities of (a)
8 A, (b) 9 A, (c) 10 A, (d) 11 A, and (e) 12 A and the marking speed
of 800 mm/s (scale bar of 1 cm).
Visual
appearance of 0.02% PP/MoS2 composite materials
after laser marking at different laser current intensities of (a)
8 A, (b) 9 A, (c) 10 A, (d) 11 A, and (e) 12 A and the marking speed
of 800 mm/s (scale bar of 1 cm).Figure shows a
histogram of laser marking color difference values of 0.02% PP/MoS2 composite materials at a scanning speed of 800 mm/s and different
current intensities. From Figure , the color difference values of laser marking with
current intensities of 8, 9, 10, 11, and 12 A are 2.01, 0.96, 12.27,
13.47, and 3.01, respectively. When the laser marking current intensity
is 11 A, the color difference value is the largest, and the best laser
marking performance is obtained. As the laser marking current intensity
increases to 12 A, MoS2 can absorb more laser energy and
produce strong photothermal conversion, resulting in the local temperature
rise and overheating, which makes the PP chains surrounding the MoS2 particles decompose and bubble on the composite surface.
In addition, the color difference value begins to decrease because
the surface of the material begins to bubble and the color becomes
lighter. To summarize the above result, it can be seen that when the
laser current intensity is 11 A, the laser marking color difference
value reaches the maximum value of 13.47. The carbonization degree
of the material surface becomes higher, and the best laser marking
performance is obtained due to the increase of the laser intensity.
Figure 5
Laser
marking color difference values of 0.02% PP/MoS2 composites
at different laser current intensities (8, 9, 10, 11,
and 12 A) and 800 mm/s.
Laser
marking color difference values of 0.02% PP/MoS2 composites
at different laser current intensities (8, 9, 10, 11,
and 12 A) and 800 mm/s.
Effect
of Different Marking Speeds on the
Laser Marking Property
Figure shows the visual appearance of the laser markings
of 0.02% PP/MoS2 composites at different marking speeds
(200, 400, 600, 800, 1000 mm/s) under the same current intensity of
11 A. From Figure , there are no obvious differences observed among the composites,
and all of the composites show very clear patterns.
Figure 6
Visual appearance of
0.02% PP/MoS2 composites after
laser marking at the scanning speeds of (a) 200 mm/s, (b) 400 mm/s,
(c) 600 mm/s, (d) 800 mm/s, and (e) 1000 mm/s and the laser current
intensity of 11 A (scale bar of 1 cm).
Visual appearance of
0.02% PP/MoS2 composites after
laser marking at the scanning speeds of (a) 200 mm/s, (b) 400 mm/s,
(c) 600 mm/s, (d) 800 mm/s, and (e) 1000 mm/s and the laser current
intensity of 11 A (scale bar of 1 cm).Figure shows laser
marking color difference values of the 0.02% PP/MoS2 composite
material at different line speeds (200, 400, 600, 800, 1000 mm/s)
at 11 A. As shown in Figure , it can be seen that the laser scanning speed has little
effect on the color difference values of the 0.02% PP/MoS2 composite. Under the same current intensity of 11 A and at the scanning
speeds of 200, 400, 600, 800, and 1000 mm/s, the color difference
values of composites are 11.15, 11.02, 12.3, 13.47, and 12.47, respectively.
When the laser marking speed is 800 mm/s, the composite shows better
laser marking performance, but the color difference values of other
marking speeds are also very high. The scanning speed higher than
1000 mm/s was also investigated (see Figure S4 in the Supporting Information) because from an industrial point
of view, extending the upper limit of the laser marking speed with
a relatively good definition would be helpful. From Figure S4, it can be seen that at high scanning speeds of
1200 and 1500 mm/s, the color difference values are slightly decreased,
compared with the values at lower scanning speeds. This is because
if the laser marking scanning speed is too high, the distance between
the laser spots becomes too large and the definition of laser-induced
marking is relatively low. Only when the laser spot size and distance
are moderate, carbonization is more uniform and the optimum laser
marking can be obtained. In addition, a high laser scanning speed
leads to high energy consumption and also affects the service life
of the laser. In our work, a scanning speed higher than 1000 mm/s
was not considered for the following experiments and data analysis.
From the perspective of laser marking performance and energy-saving,
the optimum conditions for laser marking composites include a 0.02%
loading content of MoS2, a laser current intensity of 11
A, and a laser marking speed of 800 mm/s, leading to the maximum color
value of 13.47.
Figure 7
Laser marking color difference values of the 0.02% PP/MoS2 composite material at different line speeds (200, 400, 600,
800,
1000 mm/s) at 11 A.
Laser marking color difference values of the 0.02% PP/MoS2 composite material at different line speeds (200, 400, 600,
800,
1000 mm/s) at 11 A.
Metallographic
Microscopic Images of PP/MoS2 Composites
Although
a metallographic microscope
is also an optical microscope, there are some differences in the observed
information. The magnification of the metallographic microscope observation
is usually higher than that of the ordinary optical microscope. The
working principle of the metallographic microscope is that it uses
the reflection of light on the surface of the material and mainly
observes the degree of laser ablation on the surface, which enables
us to clearly see the phenomenon and visualize the appearance of the
material surface. The working principle of the optical microscope
is that it mainly uses the transmission of light. Through the light
passing through the film material, the degree of carbonization on
the surface of the material can be clearly seen. When the surface
of the material is more carbonized, the light transmittance of the
material is relatively poor, and black carbonized dots usually appear
and can be observed. The results using both microscopes have been
revealed and discussed in this study.Figure shows the metallographic microscopic images
of PP and PP/MoS2 with different MoS2 loading
contents before and after laser marking. From Figure a–e, the unmarked PP and PP/MoS2 composite materials show a rather flat and smooth surface
with the increase of the MoS2 content without laser marking.
After laser marking (see Figure g–l) at the laser current intensity of 11 A
and the scanning speed of 800 mm/s, the surface of PP remains unchanged
and flat due to its poor absorption of laser energy. On the contrary,
the PP/MoS2 composite show an increasing laser sensitivity
with the increase of the MoS2 loading content. At a lower
MoS2 content of 0.005%, the laser pattern is not clear
and the surface only shows a small number of spots, indicating the
slight carbonization on the composite surface. With the increase of
the MoS2 content from 0.01 to 0.02%, the composite can
absorb more laser light energy and undergo a severe photothermal reaction,
leading to a rough surface and a clear laser marking pattern. However,
at a very high MoS2 content of 0.2%, the composite absorbs
too much laser energy, and the carbonization degree of the composite
is increased, causing the surface to bubble. It is impossible to form
a clear and high-contrast laser marking on the composite surface.
Similarly, the influence of the laser current intensities of 8, 9,
10, 11, and 12 A on the laser marking performance of the composites
was also investigated. The result shows that with the increase of
the laser current intensity, the composite becomes more sensitive
to laser energy, and carbonization can easily occur, leading to high-contrast
and clear laser markings on the surface. However, a high laser current
intensity leads to severe photothermal conversion and formation of
foams on the surface, which has a negative influence on the laser
marking performance. In summary, the optimum conditions of the 0.02%
PP/MoS2 composite material at the laser current intensity
of 11 A and the marking speed of 800 mm/s can lead to the formation
of a clear laser marking.
Figure 8
Metallographic microscopic images of (a) PP
and PP/MoS2 with different loading contents of (b) 0.005%,
(c) 0.01%, (d) 0.015%,
(e) 0.02%, and (f) 0.2% (scale bar: 100 μm) before laser marking
and (g) PP and PP/MoS2 with different loading contents
of (h) 0.005%, (i) 0.01%, (j) 0.015%, (k) 0.02%, and (l) 0.2% (magnification
200) after laser marking.
Metallographic microscopic images of (a) PP
and PP/MoS2 with different loading contents of (b) 0.005%,
(c) 0.01%, (d) 0.015%,
(e) 0.02%, and (f) 0.2% (scale bar: 100 μm) before laser marking
and (g) PP and PP/MoS2 with different loading contents
of (h) 0.005%, (i) 0.01%, (j) 0.015%, (k) 0.02%, and (l) 0.2% (magnification
200) after laser marking.
Microscopic Images of PP/MoS2 Composites
Figure shows the
microscopic images of PP and PP/MoS2 composites under different
conditions including the loading content, laser current intensity,
and the marking speed.
Figure 9
Microscopic images of PP (a), (b) 0.01% PP/MoS2, (c)
0.015% PP/MoS2, (d) 0.02% PP/MoS2, and (e) 0.2%
PP/MoS2 composite materials after laser marking at the
laser current intensity of 11 A and the marking speed of 800 mm/s;
images of 0.02% PP/MoS2 composite materials after laser
marking at different laser current intensities of (f) 8 A, (g) 9 A,
(h) 10 A, (i) 11 A, and (j) 12 A and the marking speed of 800 mm/s;
images of 0.02% PP/MoS2 composites after laser marking
at the scanning speed of (k) 200 mm/s, (l) 400 mm/s, (m) 600 mm/s,
(n) 800 mm/s, and (o) 1000 mm/s and the laser current intensity of
11 A (scale bar of 100 μm).
Microscopic images of PP (a), (b) 0.01% PP/MoS2, (c)
0.015% PP/MoS2, (d) 0.02% PP/MoS2, and (e) 0.2%
PP/MoS2 composite materials after laser marking at the
laser current intensity of 11 A and the marking speed of 800 mm/s;
images of 0.02% PP/MoS2 composite materials after laser
marking at different laser current intensities of (f) 8 A, (g) 9 A,
(h) 10 A, (i) 11 A, and (j) 12 A and the marking speed of 800 mm/s;
images of 0.02% PP/MoS2 composites after laser marking
at the scanning speed of (k) 200 mm/s, (l) 400 mm/s, (m) 600 mm/s,
(n) 800 mm/s, and (o) 1000 mm/s and the laser current intensity of
11 A (scale bar of 100 μm).The uniformity of MoS2 dispersion in PP was first investigated
by analyzing the results of optical microscopy and laser pattern analysis
after laser marking. Since the size of MoS2 is about 1.5
μm and MoS2 itself is black flake particles, the
dispersion and aggregation of inorganic MoS2 in the composite
film are observed through the transmitted light of an optical microscope.
If larger aggregates are formed, black spots with a large size can
generally be observed. Figure S3 shows
the optical microscope photos of the 0.2% PP/MoS2 composite
before laser marking. It can be seen from Figure S3 that the 0.2% PP/MoS2 composite material did
not show large black spots caused by obvious aggregates before laser
marking, indicating that MoS2 was uniformly dispersed in
the PP matrix resin. After laser irradiation, from Figure b–e it can be clearly
observed that the PP/MoS2 composite material shows an ordered
dot array in the marked area, especially, the PP/MoS2 composite
material itself forms ordered black carbon dots through line-by-line
scanning and then forms a pattern. Comparing the marked area with
the unmarked area, it can also be seen that MoS2 is evenly
dispersed in PP. Conversely, if the dispersion of MoS2 in
PP is poor and aggregation occurs, the resulting pattern should be
uneven, and there will be differences in various places. Taking into
account that the amount of MoS2 added is relatively small
and the pattern definition and contrast after laser marking are relatively
high, it can be concluded that the dispersion of MoS2 in
PP is quite good; therefore, uniform carbonization and a blackening
pattern can be formed. From Figure a–e, it can be clearly seen that compared with
pure PP, the composites show a clear laser marking, and the carbonization
degree increases with the increase of the MoS2 content.
At a very high MoS2 content of 0.2%, because too much MoS2 content is added, the composite surface is too dark, the
contrast is not obvious, and it is impossible to display clear laser
markings. It is suitable for the carbonization of the composite with
0.02% MoS2 to form a relatively clear laser mark, which
is consistent with the result drawn from the color difference tests.
In summary, the 0.02% PP/MoS2 composite material at a laser
marking speed of 800 mm/s becomes more uniformly carbonized at a laser
current intensity of 11 A, and it is easier to form a clearer laser
mark. From Figure f–j, with the increase of the laser current intensities, the
PP/MoS2 composites become more sensitive to laser energy
and adsorb more laser energy, which leads to the increased degree
of carbonization and a clearer laser marking. However, the higher
energy seriously damages the surface and influences the mechanical
properties of composites. From Figure k–o, it can be seen that there is no large difference
in the laser marking performance for composites at different marking
speeds from 200 to 1000 mm/s. Normally, a high marking speed is beneficial
to improve the efficiency of laser processing. In conclusion, at the
laser marking speed of 800 mm/s, the 0.02% PP/MoS2 composite material
has more uniform carbonization at the laser current intensity of 11
A, and it is easier to form a relatively clear laser marking.
SEM Images of PP/MoS2 Composites
Figure displays
the SEM image of pure PP and PP/MoS2 composites with different
MoS2 loading contents of 0.005, 0.01, 0.015, 0.02, and
0.2% after laser marking at the laser current intensity of 11 A and
the marking speed of 800 mm/s. As shown in Figure , the marked PP shows a flat and smooth
surface. After the addition of laser-sensitive MoS2 into
PP, the obtained laser marked surface is rough and covered with carbon
particles. At a lower content of 0.005%, the marked composite has
a relatively smooth surface and there are a few particles and aggregation,
indicating the slight changes including photothermal conversion, melting,
and carbonization caused by laser irradiation. With the gradual increase
of the MoS2 content, the responsiveness of the PP/MoS2 composites to the laser gets better and better, and an uneven
and rough surface is observed. When the content of MoS2 increases to 0.02%, the laser ablation area expands and PP melts.
This laser marked area is uniform, and the overall carbonization degree
is quite high, which also indicates the good laser marking performance
of composites. As shown in Figure e, the platelike particles that appear on the surface
of composites with MoS2 are carbonized PP, indicating the
melting, cooling, and solidification of PP induced by the severe photothermal
reaction. At a high MoS2 loading of 0.2%, the platelike
particles disappeared (see Figure f). In relation to the results obtained by the microscope,
this phenomenon can be explained by the high MoS2 loading
being able to absorb more laser energy and the temperature suddenly
increasing dramatically, leading to pyrolysis and foaming on the PP
surface. On the contrary, the extent of the carbonization reaction
that occurs is not as much as when the loading content is lower. This
is difficult to be observed by a SEM and is a possible reason why
the carbonized PP disappeared in the 0.2% PP/MoS2 composite.
In addition, when the content of MoS2 is 0.2%, the uniform
carbonization degree of the surface of the composite material and
the contrast of laser marking on the surface of the material are both
reduced, resulting in a decrease in the laser marking property of
the material. In combination with the visual and microscopic observations,
it can be concluded that with the increase of the MoS2 content,
the PP/MoS2 composite material increases its responsiveness
to the near-infrared laser and undergoes a severe photothermal reaction,
which causes the surface of the composite material to be uneven and
rough.
Figure 10
SEM image of (a) pure PP, (b) 0.005% PP/MoS2, (c) 0.01%
PP/MoS2, (d) 0.015% PP/MoS2, (e) 0.02% PP/MoS2, and (f) 0.2% PP/MoS2 composite materials after
laser marking at the laser current intensity of 11 A and the marking
speed of 800 mm/s (magnification 1000) (the red dotted box indicates
the laser marked area).
SEM image of (a) pure PP, (b) 0.005% PP/MoS2, (c) 0.01%
PP/MoS2, (d) 0.015% PP/MoS2, (e) 0.02% PP/MoS2, and (f) 0.2% PP/MoS2 composite materials after
laser marking at the laser current intensity of 11 A and the marking
speed of 800 mm/s (magnification 1000) (the red dotted box indicates
the laser marked area).
Water
Contact Angle on the Composite Surface
Figure shows
the changes in the water contact angle of the surface of PP and the
PP/MoS2 composite material containing different MoS2 loading contents before and after laser marking. It can be
seen from Figure a–f that before laser marking, the water contact angle of
the pure PP surface is about 71°. With the addition of MoS2, the roughness of the prepared composite material is slightly
increased, the water contact angle increases in the range of 72–80°,
and the overall change is not big. This is because the material has
not been laser marked on the surface, there have been no drastic photothermal
conversion and surface roughness changes, and MoS2 is incorporated
in the PP matrix, which does not have much impact on the water contact
angle; therefore, the water contact angle changes slightly. The water
contact angle test results in Figure g–l show that after laser marking, since pure
PP has a poor response to the near-infrared laser, the changes in
the hydrophilic and hydrophobic properties of the PP surface before
and after laser marking are small. With the increase of the MoS2 content, the PP/MoS2 composite material becomes
more and more responsive to the laser. The carbonized materials are
formed on the surface of the sample sheets. Compared with pure PP
laser marking, the surface roughness of the PP/MoS2 composite
becomes higher, resulting in a larger contact angle. When the MoS2 content is 0.2%, the water contact angle of the composite
material after laser marking is 98°, which is about 20°
larger than that of the unmarked surface. During the laser marking
process in air, the PP chains are easily carbonized and oxidized due
to the severe photothermal reaction induced by MoS2. The
surface chemical composition of PP/MoS2 is changed due
to the increased number of oxygen groups, which most probably improves
the hydrophilic property of the PP composites. However, from Figure , it can be found
that the water contact angles of PP/MoS2 with different
loading contents of 0.005, 0.01, 0.015, 0.02, and 0.2% after laser
marking were increased, compared with those of the unmarked samples.
This indicated that the roughness change plays a greater role in the
contact angle change than the surface chemical composition change.
By observing the change of the water contact angle before and after
the laser marking of the PP/MoS2 composite material, it
can be concluded that due to the high temperature of the laser marking,
the surface is carbonized, forming uneven carbonized particles and
porous structures, and the surface roughness increases. The contact
angle of the material after marking is relatively increased. This
result is consistent with the above SEM and visual observation data.
Figure 11
Water
contact angles on the surface of PP (a) and PP/MoS2 with
different loading contents of (b) 0.005%, (c) 0.01%, (d) 0.015%,
(e) 0.02%, and (f) 0.2% before laser marking and PP (g) and PP/MoS2 with different loading contents of (h) 0.005%, (i) 0.01%,
(j) 0.015%, (k) 0.02%, and (l) 0.2% after laser marking.
Water
contact angles on the surface of PP (a) and PP/MoS2 with
different loading contents of (b) 0.005%, (c) 0.01%, (d) 0.015%,
(e) 0.02%, and (f) 0.2% before laser marking and PP (g) and PP/MoS2 with different loading contents of (h) 0.005%, (i) 0.01%,
(j) 0.015%, (k) 0.02%, and (l) 0.2% after laser marking.
XRD Patterns and Raman Spectra of PP/MoS2 Composites
To better clarify the mechanism of laser
marking on the surface of composite materials, XRD and Raman spectroscopy
were used to study the structural changes of pure PP and composite
materials before and after laser marking. Figure shows the XRD patterns and Raman spectra
of pure PP and composite materials before and after laser marking.
It can be seen from Figure a that there are hardly any changes observed in the spectra
of PP and PP/MoS2 composites before and after marking,
which indicates that after laser marking, the crystal structures of
PP and MoS2 did not change, that is, the laser-induced
marking only changes the surface properties of the PP material without
influencing the crystal structures. Figure S1 in the Supporting Information indicates that the XRD pattern of
pure MoS2 appears at 15°. Since MoS2 dispersed
in PP has a very low loading content, the XRD pattern of the composite
material does not show the characteristic peak of MoS2.
The carbonization of the PP/MoS2 composite material is
due to the role of pure MoS2 in the matrix material, and
there is no change in the crystal structure inside the material during
the marking process. Figure S2 in the Supporting
Information shows that the Raman spectrum of MoS2 has two
characteristic peaks at around 408 and 376 cm–1.
As shown in Figure b, compared with the unmarked PP and composite samples, the Raman
spectra of the laser marked PP and the PP/MoS2 composite
show a broad band appearing from 1000 to 2000 cm–1, which corresponds to the characteristic band of the amorphous carbon.
This is because after laser marking, the surface of the PP/MoS2 composite is carbonized and the amorphous material is formed.
Compared with the marked PP, the marked PP/MoS2 composite
shows a higher broad band in the range of 1000–2000 cm–1. The composite material with MoS2 has
a good response to the near-infrared laser and undergoes a severe
photothermal reaction, and the content of amorphous carbonized material
on the surface increases; therefore, the intensity of the broad band
increases. This proves that the composite material can absorb the
laser energy and undergo photothermal conversion, causing surface
pyrolysis and carbonization to form amorphous carbonized materials.
Figure 12
XRD
patterns (a) and Raman spectra (b) of PP and 0.2% PP/MoS2 composite
materials before and after laser marking at 11 A.
XRD
patterns (a) and Raman spectra (b) of PP and 0.2% PP/MoS2 composite
materials before and after laser marking at 11 A.
Mechanical Properties of PP and PP/MoS2 Composites
Figure shows the elongation at break and the tensile strength
of PP, 0.005% PP/MoS2, 0.01% PP/MoS2, 0.015%
PP/MoS2, 0.02% PP/MoS2, and 0.2% PP/MoS2 composite materials after laser marking. From Figure a, it can be seen that with
the gradual increase of the laser current intensity from 8 to 12 A,
the elongation at break of the PP/MoS2 composite material
gradually decreases, that is, the mechanical properties of the PP/MoS2 composite material gradually decrease. This is because the
increase of the current intensity damages the laser marked matrix
material. From SEM observations, there are many carbonized particles
and bumps after the laser marking, and the stress concentration during
the stretching process causes the material to break.
Figure 13
Elongation at break
(a) and the tensile strength (b) of PP, 0.005%
PP/MoS2, 0.01% PP/MoS2, 0.015% PP/MoS2, 0.02% PP/MoS2, and 0.2% PP/MoS2 composite
materials after laser marking at the laser current intensity of 11
A and the scanning speed of 800 mm/s.
Elongation at break
(a) and the tensile strength (b) of PP, 0.005%
PP/MoS2, 0.01% PP/MoS2, 0.015% PP/MoS2, 0.02% PP/MoS2, and 0.2% PP/MoS2 composite
materials after laser marking at the laser current intensity of 11
A and the scanning speed of 800 mm/s.On observing Figure a, it can be seen that the mechanical properties of the laser
marked PP/MoS2 composites gradually become lower than those
of pure PP. Considering the laser marking performance, the 0.02% PP/MoS2 composite can be selected for the tensile strength properties.
From Figure b, it
can be found that the tensile strength of pure PP is about 26.86 MPa.
Since the carbonized particles after laser marking can cause stress
concentration, the tensile strength decreases gradually with the MoS2 content, resulting in poor mechanical properties at high
MoS2 contents. Compared with pure PP and other composites,
the 0.02% PP/MoS2 composite material can maintain a good
laser marking property and mechanical performance at the laser current
intensity of 11 A and the marking speed of 800 mm/s.
Conclusions
In this work, from multiple perspectives
such as the laser marking
performance, mechanical properties, and energy consumption during
the laser marking process, the optimum formula and conditions are
determined for the PP/MoS2 composite material.The
laser marking additive MoS2 has stable properties
and good absorption for the near-infrared laser, which makes the PP
material undergo pyrolysis and carbonization to form a relatively
clear laser marking. Through visual and microscopic observations,
scanning electron microscopy, Raman spectroscopy, XRD, color difference
measurements, and mechanical property tests, the PP/MoS2 composite material has the best laser marking performance at the
MoS2 loading content of 0.02%, the laser current intensity
of 11 A, and the laser marking speed of 800 mm/s. The addition of
the small amount of MoS2 has a slight influence on the
tensile strength of the composite materials. During laser marking,
the additive MoS2 can absorb the laser energy and undergo
a photothermal reaction and the PP chains around MoS2 can
be pyrolyzed and carbonized, leading to the formation of the black
carbonized materials on the surface of the composites. This topic
is of great significance to the realization of the high-functionality
and high-performance application of PP-based materials and meets the
laser marking needs of characters, patterns, and 2D codes on the surface
of PP products in the fields of automobiles, medical equipment, and
precision instruments.
Materials and Methods
Chemicals and Materials
PP (1600E)
was purchased from Sinopec Shanghai Petrochemical Co., Ltd (Shanghai,
China). MoS2 (1.5 μm, XF184–1) was commercially
available at Nanjing Xianfeng Nano Co., Ltd (Nanjing, China).
Preparation of the PP/MoS2 Composite
Materials
PP granules and MoS2 powders with different
contents, including 0.005, 0.01, 0.015, 0.02, and 0.2%, are fully
mixed and then added into an internal mixer (Su-70, Changzhou Suyan
Technology Co., Ltd., Changzhou, China) for internal mixing, and the
temperature is set at 180 °C. The temperature of the upper and
lower templates of the flat curing machine (YF-8017, Yangzhou Yuanfeng
Experimental Machinery Factory, Yangzhou, China) is set at 180 °C.
After the materials are molded into sheets, they are laser marked
by the laser marking machine. The composite samples are denoted as
PP/MoS2. For example, 0.02% PP/MoS2 indicates
the incorporation of 0.02% MoS2 in PP.
Laser Marking Process
The laser labeling
of PP/MoS2 composites was performed by a Nd: YAG (KDD-50, Suzhou Kaitai
Laser Technology Co., Ltd., China) pulsed laser beam at 1064 nm. Laser
marking process parameters include the laser focal length of 219 mm,
the laser spot of 100 μm, and the laser pulse repetition frequency
of 4000 Hz. In addition, the laser scanning speeds are set to be 200,
400, 600, 800, and 1000 mms. The laser current intensities of 8, 9,
10, 11, and 12 A are adopted in the laser marking process.
Instruments and Characterization
Color
Difference Tests
A spectrophotometer
(7000A, X-Rite) was calibrated with a black-and-white standard sample,
and then the color difference of the test samples was detected. The
unmarked area was referred to as the standard, and the laser marked
area (15 mm × 15 mm) on the surface of the substrate was the
comparison sample. The corresponding values of ΔE, ΔL, Δa, Δb were recorded and analyzed. Among the color difference
values, Δa represents yellowness, Δb represents blueness, ΔL represents
brightness (black and white), and ΔE represents
the color difference value. The calculation formula of the color difference
value is: ΔE = [(ΔL)2 + (Δa)2 + (Δb)2]1/2.
SEM
Tests
A scanning electron microscope
(JSM-1T100, JEOL Ltd.) was used to observe PP and PP/MoS2 samples before and after laser marking. The observation sample was
sprayed with gold and the surface morphology of the material was observed
and recorded.
XRD Measurements
The PP and PP/MoS2 samples with the size of 15 mm ×
15 mm before and after
laser marking were scanned using an X-ray diffractometer with Cu Kα
radiation (λ = 1.54 Å) (Rigaku, D/max 2500) to characterize
the crystal structure characteristics of PP composites after laser
marking.
Raman Analysis
The samples of PP
and PP/MoS2 before and after laser labeling were analyzed
using Raman spectroscopy (DXR2-5967, Thermo Fisher Scientific).
FT-IR Tests
An FT-IR spectrometer
(Nicolet IS50R, Thermo Fisher Scientific) was used to analyze the
samples such as PP and PP/MoS2 sheets, and the reflection
mode was selected for the detection. The wavenumber range was 400–4000
cm–1.
Water Contact Angle Measurements
The surface water contact angles of PP and PP/MoS2 before
and after laser irradiation were measured using a dynamic contact
angle measuring instrument (JC2009D1 goniometer, Shanghai Zhongchen
Digital Technology Equipment Co., Ltd.).
Metallographic
Microscopic Observation
The PP and PP/MoS2 samples
before and after laser marking
were placed under a metallographic microscope (4XC-VS, Dexon Testing
Equipment Co., Ltd.) to observe and record the surface morphology
of the materials.
Mechanical Property Tests
The standard
dumbbell-shaped tensile test samples of PP and PP/MoS2 were
prepared from the sheets using a dumbbell cutting die cutter. The
sheet dumbbell-shaped samples have a central part of 20 mm length,
4 mm width, and 2 mm thickness. The tensile test was carried out using
a universal testing machine (WDT-30, Shenzhen Kaiqiangli Experimental
Instrument Co., Ltd.). The tensile speed is 20 mm/min, and the measuring
span is 20 mm.
Authors: Taewoo Jeon; Hyeong Min Jin; Seung Hyun Lee; Ju Min Lee; Hyung Il Park; Mi Kyung Kim; Keon Jae Lee; Byungha Shin; Sang Ouk Kim Journal: ACS Nano Date: 2016-07-19 Impact factor: 15.881
Authors: Luka Pirker; Anja Pogačnik Krajnc; Jan Malec; Vladimir Radulović; Anton Gradišek; Andreja Jelen; Maja Remškar; Igor B Mekjavić; Janez Kovač; Miran Mozetič; Luka Snoj Journal: J Memb Sci Date: 2020-10-01 Impact factor: 8.742