Open Access

Synthesis and Tribological Properties of WSe2Nanorods

Nanoscale Research Letters20083:481

Received: 10 July 2008

Accepted: 2 October 2008

Published: 25 October 2008


The WSe2nanorods were synthesized via solid-state reaction method and characterized by X-ray diffractometer, TEM, and HRTEM. The results indicated the WSe2compounds had rod-like structures with diameters of 10–50 nm and lengths of 100–400 nm, and the growth process of WSe2nanorods was discussed on the basis of the experimental facts. The tribological properties of WSe2nanorods as additives in HVI500 base oil were investigated by UMT-2 multispecimen tribotester. Under the determinate conditions, the friction coefficient of the base oil containing WSe2nanorods was lower than that of the base oil, and decreased with increasing mass fraction of WSe2nanorods when it was <7 wt.%. Moreover, the base oil with the additives was rather suited to high load and high rotating speed. A combination of rolling friction, sliding friction, and stable tribofilm on the rubbing surface could explain the good friction and wear properties of WSe2nanorods as additives.


WSe2nanorodsGrowth mechanismLubrication additiveTribological propertiesRotating speed


The transition-metal dichalcogenides (including disulfide and diselenium) showed a wide variety of interesting physical properties, such as semiconducting, metallic, superconducting, and magnetic behavior [17]. WSe2 was an interesting member of the transition-metal dichalcogenides family. It was a semiconductor with a band gap in the range of 1.2–2 eV, which was useful for photovoltaic and optoelectronic applications [810]. WSe2 possessed a layered structure with the metal atoms (W) bonded covalently between the layers of chalcogen atoms (Se), and the remarkable feature of the WSe2 was highly antiphotocorrosive due to the observation of layered structure, which made it as a strong candidate in the development of high efficiency photoelectrochemical solar cells [11].

In the past few decades, the disulfides, such as MoS2 and WS2, had been extensively studied as lubrication additive on reducing friction and wear of rubbing pairs [12, 13]. The friction-and-wear mechanism had been discussed in great detail [1419]. However, little work focused on the preparation of WSe2 nanorods, which was similar to the WS2 nanorods, especially the tribological properties of WSe2 as lubrication additive.

In this study, we reported a simple and benign method to prepare WSe2nanorods using W and Se (mole ratio 1:3) at 800 °C in an argon atmosphere. Moreover, the tribological properties of WSe2nanorods as additives in the HVI500 base oil were also investigated.


Preparation of WSe2Nanorods

All chemicals used in the experiment were from state reagent without any further purification. In a typical procedure, high-purity tungsten, selenium powders (mole ratio W:Se = 1:3), and agate balls with diameter of 8 mm were mixed in an agate jar and mechanically milled with QM-ISP2 apparatus for 50 h at 450 rpm. After ball milling, the mixture was pressed into cylindrical pellets with omnipotence tester (CSS44100, ChangChun, China). The pellets were put into a conventional tube furnace, and heated up 800 °C for 1 h followed the argon flow at the rate of about 20 sccm before cooling to the room temperature.

Structural characterization was performed by X-ray diffractometer (XRD) on D/max-2500 copper rotating-anode XRD with Cu Kα radiation (λ = 1.5406 Å) at 40 kV, 200 mA. The morphology and structure of samples was determined using TEM (JEM-2100HR, Japan) at 200 keV. The composition was characterized by energy dispersive X-ray spectroscopy (EDX, S-570, and Japan).

Tribological Properties of WSe2Nanorods as Lubrication Additive

Different mass fractions of WSe2nanorods were dispersed in the HVI500 base oil with ultrasonic vibration (1800 W power, 2000 Hz frequency) for 5 h without any active reagent, and then a series of suspended oil samples were obtained. The tribological properties of the base oil containing WSe2nanorods and the base oil were investigated using a ball-on-disk mode of UMT multispecimen tribotester at ambient condition. The morphology of the wear scar was examined using a Metallurgical microscope (MBA21000, Japan).

Results and Discussions

Characterization of WSe2Nanorods

The XRD pattern of WSe2 nanorods is illustrated in Fig. 1a. All peaks were indexed to the hexagonal WSe2 (JCPDS No. 38-1388), which indicated the high purity of the obtained WSe2 nanorods. Figure 1b shows the shifted (002) peak caused by the crystal defects and strains [20]. Moreover, all peaks were not obviously widened from XRD pattern. The EDS results gave a W:Se ratio about 1:2, so the sample was confirmed to be WSe2.
Figure 1

XRD pattern of the WSe2nanorods

Figure 2 shows the TEM patterns of WSe2 nanorods. Figure 2a indicated that the diameters of WSe2 nanorods were from 10 to 50 nm, and the lengths were hundreds of nanometers. At the same time, Fig. 2a also reveals that the nanorods have a sharp top and unsmooth trunk, which is different from the WS2 nanorods obtained by self-transformation process [21]. Further observation showed the top of the short nanorods joined at different angles as shown in Fig. 2a (area f, e). The special structure might be due to the unsaturated dangling bonds of the top, which combined with each other under a high temperature. Figure 2b displays a single WSe2 nanorod with diameter of 6 nm. The HRTEM image shows the d-spacing between two adjacent layers was 6.54 Å corresponding to the (002) plane. Moreover, different folding stages of samples were observed at regions marked A, B, and C (Fig. 2c), the WSe2 nanorods were formed at last.
Figure 2

a TEM image of WSe2nanorods.b HRTEM image of single WSe2nanorod.c TEM image of WSe2layers at different folding stages

The reported growth mechanism in literatures [22, 23], especially the solid-state reaction of MoS2 nanostructure, gave us much inspiration toward understanding the formation of WSe2 nanorods. Under the high temperature conditions, Se quickly evaporated and simultaneously reacted with W. This rapid reaction might lead to supersaturation and fast nucleation. Thus, numerous nuclei of WSe2 were initially formed in the vapor phase. When the initial clusters grew to the critical size, they began to form crystal flakes. Because of the instability of unsaturated dangling bonds, crystalline sheets began folding, and the dangling bonds of self-terminated planes stabilized into spherical or cylindrical crystal shapes. Thin-folded flakes could directly roll up and adopt the rod-like structure (Fig. 2c).

Effect of WSe2Nanorods on Tribological Properties

Figure 3 shows the friction coefficient as a function of time with 2 N load and 150 rpm rotating speed. The average friction coefficient of 7 wt.% WSe2 nanorods (Fig. 3b) was close to 0.063, whereas it was 0.116 for the HVI500 base oil (Fig. 3a). That meant the addition of WSe2 nanorods to the base oil resulted in nearly 50% reduction for the friction coefficient of the base oil. The wear scar of plate after rubbing is shown in Fig. 4a (the base oil) and Fig. 4b (the base oil containing WSe2 nanorods). It could easily be found from Fig. 4a that wear scar has evidently rough, thick, and deep furrows and the width of about 0.18 mm. Compared to the wear scar of the base oil, the wear scar was flat and smooth, and the width was only 0.06 mm as in Fig. 4b. For other materials, such as MoS2 micrometer spheres [24], the lowest friction coefficient was only 0.08, and the wear scars of MoSe2 and WS2[25] have evidently thick and deep furrows different from that of the WSe2 nanorods we synthesized.
Figure 3

Variation of friction coefficients for the HVI500 base oil and the HVI500 base oil containing 7 wt.% WSe2nnaorods

Figure 4

The wear scar of plate:a HVI500 base oil,b HVI500 base oil containing WSe2nanorods

Figure 5a shows the friction coefficient as a function of concentration of the WSe2nanorods from 2 to 7 wt.% at 200 N load and 300 rpm rotating speed. For any mass fraction <7 wt.%, the friction coefficient of the base oil containing WSe2nanorods was lower than that of the base oil, and decreased with increasing mass fraction of the additives. Figure 5b shows the impact of rotating speed and load for the base oil containing 7 wt.% WSe2nanorods. Obviously, under low rotating speed, the friction coefficient at low load was lower than that at high load. But under high rotating speed, the friction coefficient at high load decreased. In other words, the base oil containing the additives was rather suitable for high loads and high rotating speeds.
Figure 5

Variation of friction coefficient as a function of rotating speed fora the HVI500 base oil and the HVI500 base oil containing 2, 5, 7 wt.% WSe2nanorods at 200 N,b the HVI500 base oil containing 7 wt.% WSe2nanorods for 30 min

From the above results, WSe2nanorods as lubrication additive could improve tribological properties of the base oil. A rolling friction mechanism could explain the excellent tribological properties of nanoparticles as lubrication additive. In this study, the effect WSe2nanorods as lubrication additive could be attribute to the molecule bearing mechanism of rolling friction and sliding friction of the WSe2nanorods between the rubbing surfaces. In addition, rotating speed was very important in the experimental process. Under low rotating speed, the stability of liquid lubricant reduced, the load almost acted on protruding part of rubbing surfaces. When the load was increased, the lubricant film became unstable and easily splintered, the friction coefficient became high, as shown in Fig. 5b. But with the increase of rotating speed, the oil film became more and more stable, which could not only bear the load of the steel balls but also prevented any direct contact between the two rubbing surfaces. Moreover, when the shape of nonmaterial was destroyed at high load and high rotating speed, exfoliation of nonmaterial layer filled the rough contact surface and formed a stable thin film with base oil, which could decrease friction and wear happening on the rubbing surfaces.


WSe2nanorods of 10–50 nm in diameters and 100–400 nm in lengths were prepared successfully by solid-state reaction of the tungsten and selenium powders. The HVI500 base oil with addition of WSe2nanorods showed the best friction-and-wear properties. Tribological experiments indicated that the effect of WSe2nanorods as lubrication additive could be attribute to the molecule-bearing mechanism of rolling friction and the sliding friction of the WSe2nanorods between the rubbing surfaces. Moreover, a stable film on the rubbing surface could not only bear the load of the steel ball but also prevent any direct contact between the two rubbing surfaces.



This study is supported by the National Natural Science Foundation of China (Grant Nos. 60778040, 10804036, 60878039), the Science and Technology Bureau of Key Program for Ministry of Education (Item No. 207025), and the Development of the Science and Technology Planning Project of Jilin province (Item No. 20070514).

Authors’ Affiliations

The Institute of Condensed State Physics, Jilin Normal University


  1. Boscher ND, Carmalt CJ, Parkin IP: J. Mater. Chem.. 2006, 16: 122. COI number [1:CAS:528:DC%2BD2MXhtlShtrzJ] COI number [1:CAS:528:DC%2BD2MXhtlShtrzJ] 10.1039/b514440jView ArticleGoogle Scholar
  2. Boscher ND, Carmalt CJ, Parkin IP: Eur. J. Inorg. Chem.. 2006, 10: 1255. 10.1002/ejic.200500857View ArticleGoogle Scholar
  3. Tsuneta T, Toshima T, Inagaki K, Shibayama T, Tanda S, Uji S, Ahlskog M, Hakonen P, Paalanen M: Curr. Appl. Phys.. 2003, 3: 473. 10.1016/j.cap.2003.07.002View ArticleGoogle Scholar
  4. Salman Z, Wang D, Chow KH, Hossain MD, Kreitzman SR, Keeler TA, Levy CDP, MacFarlane WA, Miller RI, Morris GD, Parolin TJ, Saadaoui H, Smadella M, Kiefl RF: Phys. Rev. Lett.. 2007, 98: 167001. COI number [1:STN:280:DC%2BD2s3ptVyqsw%3D%3D] COI number [1:STN:280:DC%2BD2s3ptVyqsw%3D%3D] 10.1103/PhysRevLett.98.167001View ArticleGoogle Scholar
  5. Soto F, Berger H, Cabo L, Carballeira C, Mosqueira J, Pavuna D, Toimil P, Vidal F: Physica C. 2007, 460: 789. 10.1016/j.physc.2007.04.032View ArticleGoogle Scholar
  6. Zhou Z, Jin R, Eres G, Mandrus D, Barzykin V, Schlottmann P, Hor Y-S, Xiao Z, Mitchell JF: Phys. Rev. B. 2007, 76: 104511. 10.1103/PhysRevB.76.104511View ArticleGoogle Scholar
  7. Hu SY, Lee YC, Shen JL, Chen KW, Tiong KK, Huang YS: Solid State Commun.. 2006, 139: 176. COI number [1:CAS:528:DC%2BD28XmvFykt70%3D] COI number [1:CAS:528:DC%2BD28XmvFykt70%3D] 10.1016/j.ssc.2006.05.027View ArticleGoogle Scholar
  8. Tiefenbacher KS, Eyert V, Pettenkofer C, Jaegermann W: Thin Solid Films. 2000, 380: 221. 10.1016/S0040-6090(00)01510-8View ArticleGoogle Scholar
  9. Reshak AH, Auluck S: Physica B. 2007, 393: 88. COI number [1:CAS:528:DC%2BD2sXjvFeisrg%3D] COI number [1:CAS:528:DC%2BD2sXjvFeisrg%3D] 10.1016/j.physb.2006.12.065View ArticleGoogle Scholar
  10. Reshak AH, Auluck S: Phys. Rev. B. 2003, 68: 195107. 10.1103/PhysRevB.68.195107View ArticleGoogle Scholar
  11. Jebaraj Devadasan J, Sanjeeviraja C, Jayachandran M: Mater. Chem. Phys.. 2002, 77: 397. 10.1016/S0254-0584(02)00095-0View ArticleGoogle Scholar
  12. Feldman Y, Frey GL, Homyonfer M, Tenne R: J. Am. Chem. Soc.. 1996, 118: 5632. 10.1021/ja9602408View ArticleGoogle Scholar
  13. Rapoport L, Leshchinsky V, Lvovsky M, Lapsker I, Volovik Yu, Tenne R: Tribol. Int.. 2002, 35: 47. COI number [1:CAS:528:DC%2BD38XktVOhtA%3D%3D] COI number [1:CAS:528:DC%2BD38XktVOhtA%3D%3D] 10.1016/S0301-679X(01)00094-9View ArticleGoogle Scholar
  14. Rapport L, Bilik Y, Feldman Y, Homyonfer M, Cohen SR, Tenne R: Nature. 1997, 387: 791. 10.1038/42910View ArticleGoogle Scholar
  15. Rapoport L, Nepomnyashchy O, Lapsker I, Verdyan A, Moshkovich A, Feldman Y, Tenne R: Wear. 2005, 259: 703. COI number [1:CAS:528:DC%2BD2MXltFygtL4%3D] COI number [1:CAS:528:DC%2BD2MXltFygtL4%3D] 10.1016/j.wear.2005.01.009View ArticleGoogle Scholar
  16. Rapoport L, Nepomnyashchy O, Lapsker I, Verdyan A, Soifer Y, Popovitz-Biro R, Tenne R: Tribol. Lett.. 2005, 19: 143. COI number [1:CAS:528:DC%2BD2MXlsFartro%3D] COI number [1:CAS:528:DC%2BD2MXlsFartro%3D] 10.1007/s11249-005-5095-2View ArticleGoogle Scholar
  17. Tenne R, Margulis L, Genut M, Hodes G: Nature. 1992, 60: 444. 10.1038/360444a0View ArticleGoogle Scholar
  18. Chhowalla M, Amaratunga GAJ: Nature. 2000, 407: 164. COI number [1:CAS:528:DC%2BD3cXmsl2nsbc%3D] COI number [1:CAS:528:DC%2BD3cXmsl2nsbc%3D] 10.1038/35025020View ArticleGoogle Scholar
  19. Sawyer WG, Thierry A, Blanchet TA: Wear. 1999, 225: 581. 10.1016/S0043-1648(99)00020-4View ArticleGoogle Scholar
  20. Joly-Pottuza L, Dassenoya F, Belina M, Vachera B, Martin JM, Fleischer N: Tribol. Lett.. 2005, 18: 477. 10.1007/s11249-005-3607-8View ArticleGoogle Scholar
  21. Zhang LL, Xu J, Wu HM, Yang YZ: Mater. Sci. Eng. A. 2007, 454: 487. 10.1016/j.msea.2006.11.072View ArticleGoogle Scholar
  22. Li XL, Ge JP, et al.: Chem. Eur. J.. 2004, 10: 6163. COI number [1:CAS:528:DC%2BD2cXhtVOisLzN] COI number [1:CAS:528:DC%2BD2cXhtVOisLzN] 10.1002/chem.200400451View ArticleGoogle Scholar
  23. Li XL, Li YD: Chem. Eur. J.. 2003, 9: 2726. COI number [1:CAS:528:DC%2BD3sXltVSiur0%3D] COI number [1:CAS:528:DC%2BD3sXltVSiur0%3D] 10.1002/chem.200204635View ArticleGoogle Scholar
  24. Zhou XD, Wu DM, et al.: Tribol. Int.. 2007, 40: 863. COI number [1:CAS:528:DC%2BD28XhtlShs7jE] COI number [1:CAS:528:DC%2BD28XhtlShs7jE] 10.1016/j.triboint.2006.09.002View ArticleGoogle Scholar
  25. Kubart T, Polcar T, et al.: Surf. Coat. Technol.. 2005, 193: 230. COI number [1:CAS:528:DC%2BD2MXhtleksbs%3D] COI number [1:CAS:528:DC%2BD2MXhtleksbs%3D] 10.1016/j.surfcoat.2004.08.146View ArticleGoogle Scholar


© to the authors 2008