Materials Chemistry and Physics 134 (2012) 670e676 Contents lists available at SciVerse ScienceDirect Materials Chemistry and Physics journal homepage: www.elsevier.com/locate/matchemphys Effects of electroless nickel plating on 441 stainless steel as SOFC interconnect Wei-Ja Shong a, *, Chien-Kuo Liu a, Peng Yang a, b a b Physics Division, Institute of Nuclear Energy Research, 1000 Wenhua Rd, Chiaan Village, Lungtan, Taoyuan 32546, Taiwan, ROC Department of Engineering Science and Ocean Engineering, National Taiwan University, Taipei 10617, Taiwan, ROC a r t i c l e i n f o a b s t r a c t Article history: Received 25 October 2011 Received in revised form 30 January 2012 Accepted 13 March 2012 Metal nickel was electrolessly deposited in thickness of approximately 6, 8, and 10 mm on ferritic stainless steel 441. Oxidation behaviour of plated samples was investigated after isothermal ageing at 750 C for 400 h in an air atmosphere. Microstructure examination showed that nickel oxide formed on the surface, (Fe, Ni)3O4 spinel layer at the subsurface, and chromite at the oxide scale/steel interface. No chromium species was readily detected on the outer surface. Area specific resistance measurement indicated 2.0, 3.3, and 6.3 mU cm2 for 6, 8, and 10 mm plating layers, respectively, all lower than that of the uncoated case, 28 mU cm2. Results suggested nickel plating of thickness 8 mm would be sufficient for effectively preventing Cr out-diffusion while maintaining a low electric resistivity. Ó 2012 Elsevier B.V. All rights reserved. Keywords: Coatings Oxidation Microstructure Electrical conductivity 1. Introduction Solid oxide fuel cells (SOFCs) are devices transferring chemical energy in fuel directly into electricity through electrochemical reactions operated in high temperature environments [1]. With a planar type SOFC stack design, interconnect is placed between unit cells to serve for electricity conduction and oxidant-fuel gas separation. As the operating temperature descends to the intermediate range (600e800 C), metallic interconnect, especially that made of chromium-forming ferritic stainless steel, is widely employed for its low-cost and easy-machining attributes [2,3]. However, the chromium element contained in steel for preventing oxidation can cause Cr poisoning on cells and degrade cell performance [4e6]. Moreover, chromium oxide scale growth with high electric resistance also reduces energy efficiency. Due to these disadvantages, metallic interconnect surface coated with various materials and applying techniques has become one of common measures to improve SOFC stack durability. It was reported that sputtered nickel layers of 8e10 mm on ferritic stainless steel Crofer22APU could limit chromium evaporation rate to less than one percent of the uncoated level [7]. Nickel coating with atmospheric plasma spraying on SS430 could significantly reduce the oxidation rate to 1/50 of the uncoated case [8]. In light of the promising characteristics, applying nickel in other * Corresponding author. Tel.: þ886 3 4711400x2954; fax: þ886 3 4711408. E-mail address: wjshong@iner.gov.tw (W.-J. Shong). 0254-0584/$ e see front matter Ó 2012 Elsevier B.V. All rights reserved. doi:10.1016/j.matchemphys.2012.03.049 inexpensive and convenient ways could be explored. Among a wide range of coating techniques, industrially available electroless nickel plating offers distinct advantages. Electroless nickel plating can produce uniform deposits, even on complex surfaces. The Ni film, being more compact, provides a better protection layer to the steel substrate than electroplated nickel does. Nickel oxide (NiO) shows electric resistivity of w1/15 that of chromium oxide (Cr2O3) at 800e900 C [9], but the oxidation rate is 10e100 times higher than that of Cr2O3 [10]. For a nickel film of thickness less than 10 mm, full oxidation completes in 300 h at 800 C [10], and NiO-induced elevation in electric resistance then ceases. However, the mismatch of thermal expansion coefficients between NiO (14e17 106 C1) and a-type steel substrate (11e12 106 C1) may cause oxide scale spallation. In this study, metal nickel was electrolessly plated on SS441 steel substrates with approximately 6, 8, and 10 mm in thickness. Samples were aged in an air atmosphere at 750 C for 400 h. Area specific resistance (ASR) and microstructure with phase and element analyses were examined. Samples with 8 mm Ni plating and extra (La0.67Sr0.33)MnO3 (LSM) coating were aged at 800 C up to 5000 h for long-term effect observation. Correlations between ASR evolution and oxide scale growth were discussed. 2. Experimental Stainless steel grade SS441 was obtained from Nippon Steel Corporation. Chemical composition analyzed by inductively coupled plasma atomic emission spectrometer (ICP-AES) is shown W.-J. Shong et al. / Materials Chemistry and Physics 134 (2012) 670e676 Table 1 Chemical composition for selected elements of as-received SS441 (wt%).a Mn Cr Nb Ti Al Ni 0.26 17.30 0.36 0.11 0.005 0.11 a Analyzed with inductively coupled plasma atomic emission spectrometer. in Table 1. A steel sheet of 2.5 mm thick was cut into 1 1 cm2 specimens and abraded with #1200 grit emery paper. Prior to electroless nickel plating, specimen surfaces were degreased and activated. The activation step was to slightly etch and roughen the surface for better deposit attachment. Each step was followed by water rinsing to remove chemicals. The specimens were then immersed in a proprietary solution. Plating thickness grew at an estimated rate of 4 mm/15 min to reach around 6, 8, and 10 mm in thickness. Finished objects were water rinsed and completely dried. 671 Ni-plated and uncoated samples were aged together in a furnace at 750 C for up to 400 h. Within the furnace space, a stagnant air atmosphere was present without particular humidity control. ASR values were monitored using a multichannel four-wire probing system over the ageing period. The microstructures were examined using a scanning electron microscope (SEM, Hitachi S-4800, Tokyo, Japan), equipped with an energy dispersive X-ray spectroscopy (EDS) to determine the elemental compositions. The crystalline phases and structures of the oxide layer were analyzed by a Bruker D8 Discover X-ray diffractometer (XRD) (Karlsruhe, Germany) equipped with Cu-Ka radiation. The operation current and voltage were 40 mA and 40 kV, respectively. The scanning range was 2q ¼ 15 e85 and scanning speed 4 min1. Another long-term ageing process was conducted to examine the effect of 8 mm Ni films at 800 C for 5000 h. An additional LSM Fig. 1. SEM cross-sectional views and EDS line scans of original electrolessly nickel plated SS441 with thickness of (a) 6 mm; (b) 8 mm; (c) 10 mm. 672 W.-J. Shong et al. / Materials Chemistry and Physics 134 (2012) 670e676 Fig. 2. Surface morphology of SS441 after ageing at 750 C in an air atmosphere for 200 h: (a) uncoated; (b) 6 mm; (c) 8 mm; (d) 10 mm Ni coating. coating layer was applied on top of the 8 mm Ni film for further oxidation and Cr out-diffusion prevention [11]. The amorphous LSM coating layer was deposited using a pulsed DC magnetron sputter coater at 1.5 kW of power [12]. Sputter coating was performed in an argon atmosphere at a pressure of 7.5 mTorr and a flow rate of 130 sccm. The thickness of the LSM layer was approximately 4 mm. A Ni/LSM double-layered specimen and an LSM single-layered reference specimen were aged together at 800 C. A constant air flow from the ambient environment was introduced into the furnace at a rate of 2 l min1. The humidity of the ambient air was w3%. No specific humidity control was taken on the air flow. ASR values were measured using the same fourwire probing system during the ageing process. 3. Results and discussion Fig. 1 shows SEM cross-sectional images corresponding to the original electrolessly nickel plated SS441 with thicknesses of 6, 8, and 10 mm, respectively. Metal nickel was deposited with uniform thickness and well adhered to the steel substrate. The EDS scan lines show abrupt changes of element concentration distributions at the interface. This suggests that no inter-diffusion occurred between the Ni layer and the steel substrate. An XRD analysis on the surface of the 8 mm Ni as-plated sample revealed that the nickel layer was amorphous (see Fig. 3). After being aged at 750 C for 200 h, the uncoated sample showed pyramid-shaped grains on the surface (Fig. 2). In contrast, Fig. 3. XRD patterns for SS441 uncoated, and with 6 mm, 8 mm, and 10 mm Ni coatings. (After ageing at 750 C in an air atmosphere for 200 h). W.-J. Shong et al. / Materials Chemistry and Physics 134 (2012) 670e676 673 Fig. 4. Surface morphology of SS441 after ageing at 750 C in an air atmosphere for 400 h: (a) uncoated; (b) 6 mm; (c) 8 mm; (d) 10 mm Ni coating. the Ni-plated surfaces exhibited a denser crystalline structure. XRD analyses indicated (Mn, Cr)3O4 spinel crystallites on the uncoated sample, and NiO and (Ni, Fe)3O4 spinel for the Ni-plated ones (Fig. 3). The thermally grown nickel oxides were all of similar sizes at this stage. Surface morphologies of the 750 C, 400-h aged samples are shown in Fig. 4. For the uncoated sample, pyramid-shaped crystallites were not apparently observed. Instead, irregularly-shaped grains and a more homogeneous spinel layer below were present. Ni-plated surfaces exhibited crystalline structures. The crystal size varied with the Ni plating thickness, thicker plating yielding larger grains. XRD analyses (Fig. 5) revealed similar results as in the 200-h ageing period. (Mn, Cr)3O4 spinel appeared on the uncoated sample while NiO and (Ni, Fe)3O4 spinel formed on the Ni-plated surfaces. Cross sectional views are shown in Fig. 6. Sample areas under the silver electrodes used for ASR measurement were specifically examined [13]. The scale formed on the uncoated surface was mainly composed of chromium oxide. It was observed that Cr diffused farther into the attached Ag electrode region. The chromium content in the Ag electrode was higher than in the bulk steel zone next to the oxide scale/steel interface. In a testing environment at 750 C, the phase of silver chromite (AgCrO2) could form and contribute to electric resistance [14]. At SOFC operating temperatures above 625 C, silver chromium oxide evaporates and contaminates the cathode of cells [15]. For nickel plated samples, the oxide scale thickness was proportional to the original plating Fig. 5. XRD patterns for SS441 uncoated, and with 6 mm, 8 mm, and 10 mm Ni coatings. (after ageing at 750 C in an air atmosphere for 400 h). 674 W.-J. Shong et al. / Materials Chemistry and Physics 134 (2012) 670e676 thickness. Nickel oxide formed at the outer surface, followed by a NieFe spinel layer. Chromium oxide remained in the back of the scale structure at the oxide scale/steel interface. The EDS scan line indicated that Cr species was blocked and did not diffuse to the surface. It is noticed that Ni diffused into the bulk steel substrate significantly, at a level compatible with or higher than the Cr concentration in the sub-interface zone. The rich nickel content was likely to induce the formation of austenite. The effect of this new phase requires further investigation. The concentration distributions of chromium and nickel elements reveal exclusive trends in the steel substrate. Ni species seemed to exert an expelling effect on Cr species. This is attributed to the excellent FeeNi inter-solubility, which can enhance the oxide scale adherence. Despite the existence of microcavities at the oxide scale/steel interface, scale spallation was not observed on the Ni-plated surface. Neither was spallation found on uncoated SS441 samples, not as occurred on SS430 [16,17]. The concern for scale spallation needs to be clarified in more realistic SOFC operation environments. Testing conditions may include thermal cycling, humidified oxidant and dual (reducing and oxidizing) atmospheres. The ASR evolution of the Ni-plated samples is shown in Fig. 7 for the 400-h isothermal ageing at 750 C in an air atmosphere. The ASR value escalated with plating thickness, but not in linear proportion to the oxide scale thickness measured in Fig. 6. This is due to the complex oxide scale structure which comprises chromite, NieFe spinel and nickel oxide with various intrinsic resistance. All samples exhibited no significant ASR variation over the ageing period. The 6 mm Ni-plated specimen showed a mild rising slope of w16% over the 200e400 h ageing interval. This was probably due to the steady growth of chromium oxide. The 8 mm Fig. 6. SEM cross-sectional views and EDS line scans of SS441 after ageing at 750 C in an air atmosphere for 400 h: (a) uncoated; (b) 6 mm; (c) 8 mm; (d) 10 mm Ni coating. W.-J. Shong et al. / Materials Chemistry and Physics 134 (2012) 670e676 Fig. 7. The ASR evolution with ageing time at 750 C in an air atmosphere for SS441 electrolessly plated with 6 mm, 8 mm, and 10 mm Ni layers. (Data were not recorded between 50 and 100 h) and 10 mm Ni-plated specimens displayed slight decrease (1.2%) and increase (þ3.1%) trends respectively in the last 200-h ageing course. The nearly flat ASR trends of the 8 and 10 mm Ni-plated specimens suggest that nickel oxide of sufficient thickness can effectively retard chromia growth. From Fig. 6, both 8 and 10 mm Niplated specimens contained thinner chromium oxide layers than the 6 mm one did. The increasing trend of the 10 mm Ni-plated specimen is mainly attributed to the gradual growth of (Ni, Fe)3O4 layer. The resistivity of (Ni, Fe)3O4 is approximately two 675 orders of magnitude less than that of Cr2O3 at 800 C [18]. The development of the relatively low-resistant (Ni, Fe)3O4 layer with an impaired Cr2O3 growth rate resulted in the small positive slope of the ASR trend for the 10 mm Ni-plated specimen. The descending ASR behaviour of the 8 mm Ni-plated sample is supposedly due to the continuous inward diffusion of nickel element from the initially grown nickel oxide scale. Comparing the EDS scan lines of Fe and Ni elements for the 8 and 10 mm Ni-plated cross sections in Fig. 6 reveals some differences. According to the Fe distribution in the 8 mm case, it is suspected that the (Ni, Fe)3O4 phase, though detected from the XRD analyses (see Fig. 5), did not develop as well as in the 10 mm case. Thus the resistance contribution from (Ni, Fe)3O4 for the 8 mm Ni-plated sample still remained minor before 400 h. At the end of the 400-h ageing period, ASR values reached 2.0, 3.3 and 6.3 mU cm2 for the 6, 8, and 10 mm Ni-plated specimens, respectively. As a comparison, the ASR of the uncoated SS441 sample rose up to 28 mU cm2, mostly due to the formation of highly resistant chromium oxide scale. For the three nickel plating thicknesses, the 6 mm Ni film could block chromium out-diffusion and showed the lowest ASR value after the 400-h ageing. However, the increasing ASR trend suggested chromium oxide was still growing at a moderate rate. A thicker nickel film (8 or 10 mm) could yield an enhanced chromia suppression ability, but with a more elevated ASR level. To prevent chromium out-diffusion and oxide growth while maintaining good electric conductivity, 8 mm appears to be an adequate nickel plating thickness. The 5000-h 800 C ageing results of the 8 mm Ni/LSM doublelayered sample and the LSM single-layered reference sample are shown in Fig. 8. The ASR of the Ni/LSM coated sample started with a higher initial level due to the thicker coating. The resistance evolved with a slower rising trend and turned lower than that of the LSM coated sample after w1000 h of ageing. No spallation was found on the Ni/LSM coated surface. The results suggest a promising application of electroless nickel plating. 4. Conclusions 1. Nickel layers of 6, 8, and 10 mm in thickness have been electrolessly plated on stainless steel SS441. The Ni-plated and uncoated samples were aged at 750 C for 400 h in an air atmosphere. 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