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Abstract: In this work, we considered first order differential equation (FODE) for nuclide build-up during
irradiation of Gold (Au) with neutron. The approximate solutions to FODE are obtained using the Adomian
Decomposition Method (ADM). Results have been found to be accurate and effective when compared with
analytical solutions. Numerical computation was carried out using force.3 software.
Keywords: Adomian, Build-up, Differential equation, Gold, Neutron
Keywords: Adomian, Build-up, Differential equation, Gold, Neutron
[1] Abdusalam, H.A and Alabdulatif, M (2006). Exact and numerical solutions of the telegraph model of dispersive variability. Applied
Numerical Mathematics. Far East. J. of Dynamic System 8(1):65.
[2] Adomian, G (1994).Solving frontier problem of Physics. The decomposition method (Boston, M.A: Kluwer Academic).
[3] Antoaneta, E, Ana, P, Carmo, F and Alina, B (2011). EDXRF and INAA analysis of soils in the vicinity of a metallurgical plant.
Rom.Journ Phys. 56(7-8): 993-1000.
[4] Ellis, D.V (1987).Well logging for Earth scientists. 1st Ed. Elsevier: 523.
[5] Ellis, D.V and Singer, J.M (2008). Well logging for Earth Scientists. 2nd Ed. Springer: 629.
[6] Essiett, A.A, Uwah, E.J and Uwak, S.O (2011). Elemental analysis of soil around Ikot Abasi, aluminum smelter plant, Nigeria by
Instrumental Activation Analysis (INAA). Archives of Applied Science Research 3(1): 25-32.
[7] Evans, D.J and Raslan K.R (2004). The Adomian decomposition method for solving delay differential equation. International
Journal of Computer Mathematics 0(0):1-6.
[8] Hassan, A.M (2008). Modern trends in neutron activation analysis. Application to some African Environmental samples. Proceedings
of the 3rd Environmental Physics Conference, 19-23, 2008, Aswan, Egypt. 27-40.
[9] Ioan,S, Constantin, C, mihai, T, Sorana, D.B and Lorentz, J (2008). Analysis of soil heavy metal pollution in central Transylvania.
Int. J. Mol. Sci. 9: 434-453.
[10] Kogo, B.E, Gajere, E.N, Ogunmola, J.K and Ogbole, J.O (2009). Neutron activation analysis of soil samples from different parts of
Abuja metropolis. Middle-East Journal of Scientific research 494): 254-262.
Numerical Mathematics. Far East. J. of Dynamic System 8(1):65.
[2] Adomian, G (1994).Solving frontier problem of Physics. The decomposition method (Boston, M.A: Kluwer Academic).
[3] Antoaneta, E, Ana, P, Carmo, F and Alina, B (2011). EDXRF and INAA analysis of soils in the vicinity of a metallurgical plant.
Rom.Journ Phys. 56(7-8): 993-1000.
[4] Ellis, D.V (1987).Well logging for Earth scientists. 1st Ed. Elsevier: 523.
[5] Ellis, D.V and Singer, J.M (2008). Well logging for Earth Scientists. 2nd Ed. Springer: 629.
[6] Essiett, A.A, Uwah, E.J and Uwak, S.O (2011). Elemental analysis of soil around Ikot Abasi, aluminum smelter plant, Nigeria by
Instrumental Activation Analysis (INAA). Archives of Applied Science Research 3(1): 25-32.
[7] Evans, D.J and Raslan K.R (2004). The Adomian decomposition method for solving delay differential equation. International
Journal of Computer Mathematics 0(0):1-6.
[8] Hassan, A.M (2008). Modern trends in neutron activation analysis. Application to some African Environmental samples. Proceedings
of the 3rd Environmental Physics Conference, 19-23, 2008, Aswan, Egypt. 27-40.
[9] Ioan,S, Constantin, C, mihai, T, Sorana, D.B and Lorentz, J (2008). Analysis of soil heavy metal pollution in central Transylvania.
Int. J. Mol. Sci. 9: 434-453.
[10] Kogo, B.E, Gajere, E.N, Ogunmola, J.K and Ogbole, J.O (2009). Neutron activation analysis of soil samples from different parts of
Abuja metropolis. Middle-East Journal of Scientific research 494): 254-262.
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| Paper Type | : | Research Paper |
| Title | : | Studies on Tensile Properties of Some Plant Fibers |
| Country | : | India |
| Authors | : | Gajendra Nath Sarma, Manoranjan Talukdar |
| : | 10.9790/4861-0261013 ![]() |
|
| Downloads : Times |
Abstract: The linear density of the raw and degummed plant fibers such as ginger (zingiber officinale),
turmeric (curcuma longa) and java galangal (alpinia galangal) fibers has been determined by the use of a
Vibromat M. The stress-elongation curves for the fibers were drawn by using a Tensile Tester with electric
strain gauges 'Fefegraph' for each of the specimen fiber; at temperature 250 C and 65% R.H.
Various tensile parameters have been calculated from the stress-elongation curve obtained by using
the Tensile tester with electric strain gauges 'Fefegraph'; and the linear density by a 'Vibromat M'. It is
observed that the tenacity is linearly related with the linear density. From various investigations it has been
concluded that all the plant fibers in present investigation are hygroscopic in nature and the hygroscopicity
does not change due to irradiation and degumming.
Keywords: zingiber officinale, curcuma longa, alpinia galangal, vibromat M, fefegraph, hygroscopicity.
Keywords: zingiber officinale, curcuma longa, alpinia galangal, vibromat M, fefegraph, hygroscopicity.
[1] Thakur R, Sarkar C R and Sarmah R, Indaian J of Fiber and Textile Research, Vol. 24, Dec. 1999, p. 277.
[2] Textile Fibers, Pandya R H, edited by Deve M S, p. 26.
[3] Bora M N, Talukdar C and Talukdar M, Indian J of Fiber and Textile Research, Vol. 24, Sept. 1999, pp. 172-176.
[4] Solid State Physics, Dekker A J, McMillan India Limited, 2000, p. 150.
[5] Chattopadhyay D P, Samanta A K, Nanda R and Thakur S, Indian J Fiber and Textile Reseach, Vol. 24, March 1999, p. 76.
[6] Physics of dielectric materials, Tareev B, Mir Publishers, Moscow, p. 114.
[7] Handbook of Cotton weaving, Vol. I, edited by Onocov E, Mir Publishers, Moscow, 1981, pp. 9-33.
[8] Cheronkov E, Laboratory practice in the study of textile materials, edited by Koblyakov A, Mir Publishers, Moscow, 1989, pp. 130- 157.
[9] Principle of Textile testing, Booth J E, Bulterworth and Co. Ltd. , London, 1958. pp. 382-387.
[10] An Introduction to Polymer Physics, Perepechko I.I. Mir Publishers, Moscow, p.83.
[2] Textile Fibers, Pandya R H, edited by Deve M S, p. 26.
[3] Bora M N, Talukdar C and Talukdar M, Indian J of Fiber and Textile Research, Vol. 24, Sept. 1999, pp. 172-176.
[4] Solid State Physics, Dekker A J, McMillan India Limited, 2000, p. 150.
[5] Chattopadhyay D P, Samanta A K, Nanda R and Thakur S, Indian J Fiber and Textile Reseach, Vol. 24, March 1999, p. 76.
[6] Physics of dielectric materials, Tareev B, Mir Publishers, Moscow, p. 114.
[7] Handbook of Cotton weaving, Vol. I, edited by Onocov E, Mir Publishers, Moscow, 1981, pp. 9-33.
[8] Cheronkov E, Laboratory practice in the study of textile materials, edited by Koblyakov A, Mir Publishers, Moscow, 1989, pp. 130- 157.
[9] Principle of Textile testing, Booth J E, Bulterworth and Co. Ltd. , London, 1958. pp. 382-387.
[10] An Introduction to Polymer Physics, Perepechko I.I. Mir Publishers, Moscow, p.83.
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Abstract: Cu2ZnSnS4 (CZTS) thin films were fabricated by sulfurization of thermally evaporated metallic
precursors on glass substrates. While the Zinc and Tin thicknesses were kept constant at 300 and 200nm
respectively, three Copper layer thicknesses of 100, 150 and 200 nm were used to obtain the metallic
precursors. The precursor films were sulfurized for 3 hours at 550 0C with an initial ramping rate of 10 0C/min.
X-ray diffraction studies reveal polycrystalline films exhibiting Kesterite structures with preferential orientation
along [112] direction. The films with lowest Cu layer thickness exhibited binary metal alloy contents, which
disappears with higher Cu precursor layer thickness. The surface morphology and elemental composition of
CZTS thin films was determined from scanning electron microscopy and energy dispersive spectroscopy
analysis respectively. The grain size become large with increasing Cu/(Zn + Sn) ratio, exhibiting an
enhancement of the grain growth under Cu – rich condition. There is a nominal increase in the optical band gap
from 1.49 to 1.51 eV with increase in Cu content. The samples resistivities are in the range of 0.8 to 1.5Ωcm
Keywords: CZTS, Sulfurization, Thermal evaporation. XRD, SEM.
Keywords: CZTS, Sulfurization, Thermal evaporation. XRD, SEM.
[1] N. Kamoun, H. Bouzouita and B. Rezig Fabrication and characterization of Cu2ZnSnS4 thin films deposited by spray pyrolysis
technique, Thin Solid Films, 51(15), 2007, 5949–5952
[2] K. Ito, and T. Nakazawa, Electrical and Optical-Properties of Stannite-Type Quaternary Semiconductor Thin-Films, Japanese
Journal of Applied Physics, 27(11), 1988, 2094-2097.
[3] J. Emsley, The Elements, 3rd ed., (Oxford: Oxford University Press, 1998).
[4] B.A. Schubert, B. Marsen, S. Cinque, T. Unold, R. Klenk, S. Schorr and H.W. Schock., Cu2ZnSnS4 thin film solar cells by fast coevaporation, Progress in Photovoltaic Research and Application, 19, 2011, 93–96.
[5] H. Katagiri, K. Jimbo, W. Shwe Maw, K. Oishi, M Yamazaki, H. Araki and A. Takeuchi, Development of CZTS based thin film
solar cells, Thin Solid Films, 517 (7), 2009, 2455–2460..
[6] J. J. Scragg, D.M. Berg and P.J. Dale, A 3.2% efficient Kesterite device from electrodeposited stacked layers, Journal of
Electroanalytical Chemistry, 646 ( 1–2), 2010, 52–59.
[7] J. S. Seol, S.Y. Lee, J. C. Lee, H.D. Nam and K. H. Kim, Electrical and optical properties of Cu2ZnSnS4 thin films prepared by rf
sputtering process, Solar Energy Materials and Solar Cells, 75(1-2),. 2003, 155–162.
[8] T. Tanaka, T. Nagatomo, D. Kawasaki, M. Nishio, Q. Guo, A. Wakahara, A. Yoshida and H. Ogawa, Preparation of Cu2ZnSnS4 thin films by hybrid sputtering, Journal of Physics and Chemistry of Solids, 66(11), 2005, 1978–1981.
[9] F. Liu, Y. Li, K. Zhang, B. Wang, C. Yan, Y. Lai, Z. Zhang, J. Lie and Y. Lu, In situ growth of Cu2ZnSnS4 thin films by reactive
magnetron co-sputtering, Solar Energy Materials and Solar Cells, 94(12), 2010, 2431–2434.
[10] Q. Guo, H. W. Hillhouse and, R. Agrawal, Synthesis of Cu2ZnSnS4 nano crystal ink and its use for solar cells, Journal of the
American Chemical Society, 131(33), 2009, 11672–11673.
technique, Thin Solid Films, 51(15), 2007, 5949–5952
[2] K. Ito, and T. Nakazawa, Electrical and Optical-Properties of Stannite-Type Quaternary Semiconductor Thin-Films, Japanese
Journal of Applied Physics, 27(11), 1988, 2094-2097.
[3] J. Emsley, The Elements, 3rd ed., (Oxford: Oxford University Press, 1998).
[4] B.A. Schubert, B. Marsen, S. Cinque, T. Unold, R. Klenk, S. Schorr and H.W. Schock., Cu2ZnSnS4 thin film solar cells by fast coevaporation, Progress in Photovoltaic Research and Application, 19, 2011, 93–96.
[5] H. Katagiri, K. Jimbo, W. Shwe Maw, K. Oishi, M Yamazaki, H. Araki and A. Takeuchi, Development of CZTS based thin film
solar cells, Thin Solid Films, 517 (7), 2009, 2455–2460..
[6] J. J. Scragg, D.M. Berg and P.J. Dale, A 3.2% efficient Kesterite device from electrodeposited stacked layers, Journal of
Electroanalytical Chemistry, 646 ( 1–2), 2010, 52–59.
[7] J. S. Seol, S.Y. Lee, J. C. Lee, H.D. Nam and K. H. Kim, Electrical and optical properties of Cu2ZnSnS4 thin films prepared by rf
sputtering process, Solar Energy Materials and Solar Cells, 75(1-2),. 2003, 155–162.
[8] T. Tanaka, T. Nagatomo, D. Kawasaki, M. Nishio, Q. Guo, A. Wakahara, A. Yoshida and H. Ogawa, Preparation of Cu2ZnSnS4 thin films by hybrid sputtering, Journal of Physics and Chemistry of Solids, 66(11), 2005, 1978–1981.
[9] F. Liu, Y. Li, K. Zhang, B. Wang, C. Yan, Y. Lai, Z. Zhang, J. Lie and Y. Lu, In situ growth of Cu2ZnSnS4 thin films by reactive
magnetron co-sputtering, Solar Energy Materials and Solar Cells, 94(12), 2010, 2431–2434.
[10] Q. Guo, H. W. Hillhouse and, R. Agrawal, Synthesis of Cu2ZnSnS4 nano crystal ink and its use for solar cells, Journal of the
American Chemical Society, 131(33), 2009, 11672–11673.
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Abstract: Technological applications of High Temperature Superconductors (HTSC) are limited by "Flux
Creep", an undesired magnetic vortices movement, creating a pseudo-resistance that depresses both critical
current density and critical field. For practical applications (like energy storage systems, current limiters,
magnetic bearings, etc.), it is desired to have high values of Critical Current Density (JC) even at higher applied
field. Flux Pinning is an established mechanism of enhancing JC in HTSC by Swift Heavy Ion irradiation. This
paper explains as to how JC can be enhanced in HTSC and thereby make HTSC technologically more useful.
Some recent works and our initiatives in this direction are also discussed.
Keywords: Superconductivity, High temperature, Transport properties, Critical Currents, Flux Pinning
Keywords: Superconductivity, High temperature, Transport properties, Critical Currents, Flux Pinning
[1] D. K. Avasthi and G K Mehta, Swift Heavy Ions for Materials Engineering and Nanostructuring, Springer, 2011.
[2] T. J. Haugan et al. Nature, 430, 867, 2004
[3] K. Sanghamitra et al, Supercond. Sci. Technol., 15, 324, 2002
[4] K. R. Mavani et al, Solid State Communications, 142, 462, 2007
[5] M. R. Singh et al., Nucl. Instru. and Meth., B 269, 1117 2011
[6] P. Mele et al., Physica C , 426, 1108, 2005
[7] R. Biswal et al, Supercond. Sci. Technol. 21, 085016, 2008
[8] S. H. Wee et al, J. of the American Ceramic Society, 95, 4, 1174, 2012
[9] M. Haruta et al, Physica C, 412, 511, 2004
[10] R. E. Thomson et al, Appl. Phys. Lett., 63, 614, 1993
[2] T. J. Haugan et al. Nature, 430, 867, 2004
[3] K. Sanghamitra et al, Supercond. Sci. Technol., 15, 324, 2002
[4] K. R. Mavani et al, Solid State Communications, 142, 462, 2007
[5] M. R. Singh et al., Nucl. Instru. and Meth., B 269, 1117 2011
[6] P. Mele et al., Physica C , 426, 1108, 2005
[7] R. Biswal et al, Supercond. Sci. Technol. 21, 085016, 2008
[8] S. H. Wee et al, J. of the American Ceramic Society, 95, 4, 1174, 2012
[9] M. Haruta et al, Physica C, 412, 511, 2004
[10] R. E. Thomson et al, Appl. Phys. Lett., 63, 614, 1993
