Electronic Supplementary Material Determination of nimesulide in human serum using a glassy carbon electrode modified with SiC nanoparticles Raouf Ghavami*, Aso Navaee Department of Chemistry, Faculty of Science, University of Kurdistan, P. O. Box 416, *Corresponding author, Tel.: +98 871 6624133; fax: +98 871 6624133. Sanandaj, Iran; E-mail addresses:rghavami2000@yahoo.con; rghavami@uok.ac.ir Properties of SiC nanoparticles Silicon carbide is a wide band gap semiconductor with a range of excellent physical, chemical, mechanical and electronic properties [1]. Due to various technological applications, nanoparticles of silicon carbide have attracted the interest of scientists and engineers [2]. Silicon carbide nanoparticles are promising raw materials for high temperature engineering ceramic devices and polymers [3-5]. SiC-NPs are expected to have the ability to exhibit photoluminescence (PL) at shorter wavelengths than silicon nanoparticles, making them a promising material for optoelectronic devices [6]. The application of SiC slurry for the electrolyte matrix of phosphoric acid fuel cell and metal oxide gas sensors have been reported [7,8]. SiC–C composite film has been used for sensing of dopamine and ascorbic acid [9]. Furthermore, SiC electrode has been used as an ordinary oxidation-reduction indicator electrode in potentiometric titrations [10]. In addition, GC electrode modified with SiC nanoparticles has been used for electrocatalytic and flow injection analysis of insulin [11]. The stability and optical properties of SiC quantum dots, luminescence behavior of amorphous silicon-carbide film and electrochemical properties of SiC nanoparticles have been investigated [12-14]. Electrochemical behavior of nimesulide on the SiC-NPs/GC electrode The relationship between the peak current and the potential scan rate of nimesulide in the 0.1 M PBS was studied and CVs of 8.0 μM nimesulide in different potential scan rates from the range of 0.01-0.17 V.s-1 was recorded (Fig. S1). The experimental results indicate a good linear dependence of the catalytic reduction peak current with the square root of scan rate (v1/2) by regression coefficient R2=0.9921 (Fig. S1, inset A). This result also indicated the reaction involves mass transport and depends on concentration of nimesulide, which was ideal case for quantitative applications. -10 -8 A Ip (mA) -6 -8 -4 -2 y = -16.433x + 0.8387 R2 = 0.9921 -6 I (mA) 0 0.1 0.2 0.3 V1/2 0.4 -13.8 Ln Ip (mA) -4 -2 0.5 B -13.2 y = -20.296x - 14.713 R2 = 0.9942 -12.6 -0.04 0 -0.06 -0.08 -0.10 E-Eo' -0.2 -0.4 -0.6 -0.8 -1.0 -1.2 -1.4 -1.6 E (V) vs . Ag/AgCl Fig. S1. CVs of 8 µM nimesulide in different scan rate (0.01-0.17 V·s-1) and plot of Ip versus square root of scan rate (inset A) and LnIp versus Ep-Eº (inset B). -1.0 -8.E-07 Ip = -5 x 10-7t-1/2 - 5 x 10-7 I (A) R2 = 0.9929 -0.8 I (mA) -7.E-07 0.25 0.29 t -0.6 0.33 -1/2 -1/2 (s) -0.4 0 100 200 t (s) Fig. S2. Chronoamperogram of 2.47 × 10 -3 µmol.cm-3 nimesulide and plot of current versus inverse square root of time in 0.1 M pH 2.0 PBS. According to the peak current equation for a totally irreversible diffusion process [15]: 1 I p (3.01 10 5 )nAC (n D ) 2 (2) That αnα was determined by the following equation [15]: Ep E p 2 1.857 RT 47.7 mV n F n (3) where α is the electron-transfer coefficient, nα is the number of electrons involved in the rate determining step and Ep/2 is the potential corresponding to Ip/2. The value for αnα was found to be 0.548 (T = 298 K) for the reduction of nitro group at the surface of the modified electrode. Also, A (effective area, cm2) was determined by recording CVs of a standard concentration of K4[Fe(CN)6] in different scan rate and according to the Randles-Sevcik equation [16]: 2 3 1 2 I p (2.69 10 )n AC D 5 1 2 (4) where C* and D are the bulk concentration (47 × 10-3 µmol.cm-3) and diffusion coefficient (7.5 × 10-6 cm2.s-1) of K4[Fe(CN)6], respectively. Plot of Ip vs. v1/2 gives a straight line that from the slope of this line, the value of A can be estimated which equals to 0.144 cm2. Then inserting the obtained values of αnα and A in equation 1 the value of D can be estimated equal to 6.08 × 10-5 cm2.s-1. Moreover, by plotting of LnIp vs. Ep-Eº in different scan rate (Fig. S1, inset B) (Eº can be determined by the extrapolating of Ep vs. v, the value is equal to -0.39 V vs. Ag/AgCl), gives a straight line LnIp = -14.713 – 20.296 (Ep-Eº), R2 = 0.9942; that from slop and intercept based on following equation [17]: I p 0.227nFAC K s exp[ n F ( E p E )] RT (5) the value of αnα and Ks (standard heterogeneous rate constant of the electrochemical reaction) can be determined equal to 0.535 and 4.4×10-3 cm.s-1 respectively. Simultaneous chronoamperometric detection of 2.47×10-3 mol.cm-3 of nimesulide in 0.1 M PBS, pH 2.0, using modified electrode based on Cottrell equation [16]: 1 I (t ) nFAC * D 2 1 1 2 2 (6) t (C*=2.47 × 10-3 μmol.cm-3 is concentration of nimesulide in bulk solution, and A=0.144 cm2 is the effective area of modified electrode calculated from equation 4) and plot of I(t) vs. t−1/2 for each chronoamperograms were give a straight lines (Fig. S2); the slopes of those lines can be used to estimate the diffusion coefficient (D) of nimesulide. The value of D was found equal to 4.97×10−5 cm2.s-1, that this value has a little difference to the value of D received from equation 1 (6.08 × 10-5 cm2.s-1), so the mean value of diffusion coefficient for nimesulide from equations 2 and 6 can be 5.52 × 10-5 cm2.s-1. References 1. Zhao, H., Shi, L., Li, Z., Tang, C (2009) Silicon carbide nanowires synthesized with phenolic resin and silicon powders. Physica E 41:753-756. doi: 10.1016/j.physe.2008.12.005 2. Luo, X.L., Morrin, A., Killard, A.J., Smyth, M.R (2006) Application of nanoparticles in electrochemical sensors and biosensor. Electroanalysis 18:319- 326. doi: 10.1002/elan.200503415 3. Greil, P., Petzow, G., Tanaka, H (1987) Sintering and HIPping of silicon nitridesilicon carbide composite materials. Ceram Int 13:19-25. doi: 10.1016/0272-8842(87)90034-4 4. Chen, J.W., Xue, L.A (1990) Development of Superplastic Structural Ceramics. J Am Ceram Soc 73:2585-2609. doi: 10.1111/j.1151-2916.1990.tb06734.x 5. Kasemann, R., Schmidt, H (1994) Coatings for mechanical and chemical protection based on organic-inorganic sol-gel composites. New J Chem 18:1117-1123. 6. Boucle, J., Kassiba, A., Emery, J., Kityk, I.V., Makowska-Janusik, M., Sanetra, J., HerlinBoime, N., Mayne, M (2002) Local electrooptic effect ot the SiC largesized nanocrystallites incorporated in polymer matrices. Phys Lett A 302:196- 202. doi: 10.1016/S03759601(02)00965-9 7. Dheenadayalan, S., Song, R.H., Shin, D.R (2002) Characterization and performance analysis of silicon carbide electrolyte matrix of phosphoric acid fuel cell prepared by ball-milling method. J Power Sources 107:98-102. doi: 10.1016/S0378-7753(01)00991-0 8. Wiche, G., Berns, A., Steffes, H., Obermeier, E (2005) Thermal analysis of silicon carbide based micro hotplates for metal oxide gas sensors. Sens Actuators A 123-124:12-17. doi: 10.1016/j.sna.2005.03.028 9. Singh, S., Buchanan, R.C (2007) SiC-C fiber electrode for biological sensing. Mater Sci Eng C 27:551-557. doi:10.1016/j.msec.2006.05.053 10. Hume, D.N., Kolthoff, I.M (1941) The silicon carbide electrode. J Am Chem Soc 63:28052806. doi: 10.1021/ja01855a089 11. Salimi, A., Mohamadi, L., Hallaj, R., Soltanian, S (2009) Electrooxidation of insulin at silicon carbide nanoparticles modified glassy carbon electrode. Electrochem Commun 11:1116-1119. doi: 10.1016/j.elecom.2009.03.024 12. Roboredo, F.A., Pizzagalli, L., Galli, G (2005) Computational Engineering of the Stability and Optical Gaps of SiC Quantum Dots. Nano Lett 4:801-804. doi: 10.1021/nl049876k 13. Chen, D., Xu, J., Qian, B., Chen, S., Mei, J., Li, W., Xu, L., Chen, K (2008) Luminescence behavior from amorphous silicon-carbide film-based optical microcavities. Mater Chem Phys 111:279-282. doi: 10.1016/j.matchemphys.2008.04.008 14. Chang, H., Tsung, T.T., Chen, L.C., Jwo, C.S., Tsung, J.W., Lu, Y.C (2005) The electrochemical properties of SiC nanoparticle suspension. J Mater Eng Performance, 14, 158-162. doi: 10.1361/10599490523256 15. Nicholson RS, Shain J (1964) Theory of stationary electrode polarography: single scan and cyclic methods applied to reversible, irreversible, and kinetic systems. Anal. Chem 36:706723. doi:10.1021/ac60210a007 16. Bard AJ, Faulkner LR (2001) In: Electrochemical methods, Fundamentals and applications, 2nd ed., John Wiley & Sons. 17. González-Velasco J (1994) The linear sweep voltametric method: An application to the study of reversible and doi:10.1002/elan.1140060902 irreversible processes. Electroanalysis 6:711-724.