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, the Haar wavelets method [ 3 ], Legendre wavelets method [ 4 ], Rationalized haar wavelet [ 5 ], Hermite cubic splines [ 6 ], Coifman wavelet scaling functions [ 7 ], CAS wavelets [ 8 ], Bernoulli wavelets [ 9 ], wavelet preconditioned techniques [ 25 , 26 , 27 , 28 ]. Some of the papers are found for solving Abel′s integral equations using the wavelet based methods, such as Legendre wavelets [ 10 ] and Chebyshev wavelets [ 11 ]. Abel′s integral equations have applications in various fields of science and engineering. Such as microscopy, seismology

References 1. Sahoo SK, Sahoo HB, Priyadarshini D, Soundarya G, Rani KU. Antiulcer Activity of Ethanolic Extract of Salvadora indica ( W .) Leaves on Albino Rats. J Clin Diagnostic Res 2016; 10(9): 7-10. 2. Zakaria ZA, Balan T, Suppaiah V, Ahmad S, Jamaludin F. Mechanism(s) of action involved in the gastroprotective activity of Muntingia calabura. J Ethnopharmacol 2014; 151(3): 1184-1193. 3. Balan T, Mohd. Sani MH, Suppaiah V, Mohtarrudin N, Suhaili Z, Ahmad Z, et al. Antiulcer activity of Muntingia calabura leaves involves the modulation of endogenous nitric

{ }}\cos E){\kern 1pt} dE. \end{array}$$ (25) Completing the functions of the momenta given above (23) , it is convenient to introduce two more state functions w = U 1 / L ,      z = U 3 / L . $$\begin{array}{} \displaystyle w=U_1/L,\qquad z=U_3/L. \end{array}$$ (26) The previous results may be summarized in the following theorem: Theorem 3. By composing the three symplectic transformations ( q 1 , q 2 , q 3 , q 4 Q 1 , Q 2 , Q 3 , Q 4 ) Projective Euler → ( ρ , ϕ , θ , ψ P , Φ , Θ , Ψ ) ↓ ↓ P A ( ℓ , u 1 , g , u 3 L , U 1 , G , U 3 ) Delaunay ← ( ρ , u 1 , u 2 , u 3 P

: 11834836. 7. Ali M, McKibbin M, Booth A, Parry DA, Jain P, Riazuddin SA, et al. Null mutations in LTBP2 cause primary congenital glaucoma. Am J Hum Genet. 2009 May;84(5):664-71. doi: 10.1016/j. ajhg.2009.03.017. Epub 2009 Apr 9. PubMed PMID: 19361779; PubMed Central PMCID: PMC2680998. 8. Chavarria-Soley G, Sticht H, Aklillu E, Ingelman-Sundberg M, Pasutto F, Reis A, et al. Mutations in CYP1B1 cause primary congenital glaucoma by reduction of either activity orabundance of the enzyme. Hum Mutat. 2008 Sep;29(9):1147-53. doi: 10.1002/humu.20786. PubMed PMID: 18470941. 9

differences were observed between groups. Table 1 Anthropometric data. Variables Groups Mean Age (years) Mass (kg) Height (m) BMI (kg/m 2 ) Mean 32 80.81 1.81 24.77 Paraplegic active SD 6.06 17.19 0.07 4.24 CI 26.4- 64,91- 1.74- 20.85- 37.6 96.71 1.86 28.69 Mean 37.73 77.43 1.74 25.58 Paraplegic inactive SD 9.09 15.12 0.07 4.64 CI 32.7- 69.06- 1.7-1.78 23.01- 42.77 85.81 28.16 Mean 34 63.4 1.74 20.95 Tetraplegic active SD 8.31 9.61 0.03 2.89 CI 23.69- 51.47- 1.7-1.78 17.35- 44.31 75.33 24.54 Mean 37.25 76.98 1.78 24.11 Tetraplegic inactive SD 9.94 10.46 0.05 2.82 CI 30

International. 2003 , 11, 389–396. [4] Kortan D, Adamek Z, Polakova S. Winter predation by otter, Lutra lutra on carp pond systems in South Bohemia (Czech Republic). Folia Zool. 2007 , 56, 4, 416–428. [5] English Nature. Retrieved 2010 , 03-15. [6] Conroy J, Chanin P. The status of the Eurasian otter ( Lutra lutra ) in Europe – a review. Proceedings of the first otter toxicology conference, Eds., Conroy, J. W. H., Yoxon, P. and Gutleb, A. C.) 2000 , 7-29. [7] Ruiz-Olmo J, Loy A, Cianfrani C, Yoxon P, Yoxon G, de Silva PK, Roos A., Bisther M, Hajkova P, Zemanova B, 2008

joint probability density in phase space associated with continuous-time random walk. Physica A. 391, no. 15, 3858–3864. 10.1016/j.physa.2012.03.013 Kwok Sau Fa. Wang K.G. 2012 Integro-differential equation for joint probability density in phase space associated with continuous-time random walk Physica A. 391 15 3858 3864 10.1016/j.physa.2012.03.013 [10] Santos, L.T., Dorini, F.A., Cunha, M.C.C. (2010). The probability density function to the random linear transport equation. Appl. Math. Comput. 216, no. 5, 1524–1530. 10.1016/j.amc.2010.03.001 Santos L.T. Dorini F

. Figure 2 Apparent frequencies of a signal with a 0.3 Hz actual frequency component, sampled at 0.2, 0.3, 0.4 and 0.5 Hz are depicted. It is clear that due to aliasing the apparent frequency differs from the actual frequency in all cases. Irrespective of choice of estimation method for the impedance spectra, be it frequency sweep, multi-sine or other, longer estimation times yield better estimates; the more periods of the stimulation and sensing voltage/current, the higher signal-to-noise ratio (SNR). For slowly varying signals, e.g. body composition estimates, this

. A. Aguillon M.A. Rosell F. P. J. Carrera B. J Electrical Impedance Tomography: An Electronic Design, with Adaptive Voltage Measurements and A Phantom Circuit for Research in The Epilepsy Field Proceedings - 19th Internl Conf. - IEEE/EMBS Oct. 30 - Nov. 2 1997 867 868 USA 19 Henderson R. P., Webster J. G. An impedance camera for spatially specific measurements of the thorax. IEEE Transactions on Biomedical Engineering. 1978;Bme-25(3):250-254. 10.1109/TBME.1978.326329 Henderson R. P. Webster J. G An impedance camera for spatially specific measurements of the thorax

those obtained with the MT4080. Table 2 Capacitance C HL measured with the 4294A impedance analyzer and calculated body capacitance to ground C g for the four subjects and two feet heights above to ground: 10 cm (u) and direct outsole contact (d). Subject C HLu (pF) C gu (pF) C HLd (pF) C gd (pF) 1 22.5 95.4 18.2 153.0 2 23.5 85.1 17.8 159.7 3 24.8 72.9 20.5 119.2 4 25.5 66.8 20.2 123.2 Table 3 Capacitance C HL measured with the MT4080 LCR meter and calculated body capacitance to ground C g for the four subjects and two feet heights above ground: 10 cm (u