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Fig. 1.
Spectra were collected in the 400-4000 cm−1 range with a 2 cm−1 resolution.
Table 1.
They decrease from pH 1 to pH 5, increase at pH 9, and decrease again at pH 11.
References [1] J.

Fig. 1.
Table 1.
References [1] M.J.
Med. 1 (2008) 4
Amanullah, Cell culture processes for monoclonal antibody production, MAbs 2 (2010) 466-479

+an(M0(Sn) – 1) = ∑ni=1 ai(M0(Si) –1)= σa (M0) - ∑ni=1 ai.
[Sn]1- [Sn-1,n]1) so that M0(r1) =M2([S1])- M2([S1,2]) [resp.
We first compute µ1Sj, j=1, 2, ..., n-1, µ1S1= [S0 ] 1 -[S1 ] 1 =M1([S2])+M1([S3]) + M1([S4])+...
+(n-2) M1([Sn-1])+(n-1)M1([Sn])- M1([S1,2])- 2M1([S2,3])-…- (n-1)M1([Sn-1,n])
J., (British Computer Society), 49(4), 470-479

Fig. 1.
Table 1.
The addition of oxides decreases the intensity of the tin oxide spectrum in the range of 450-474 cm⁻¹, resulting in the formation of absorption peaks at 408 cm⁻¹ and 417 cm⁻¹ after Zn-O bond vibration, as well as at 479 cm⁻¹ and 483 cm⁻¹ after Ni-O bond vibration [5].
(a) range (400-3000 cm-1), (b) range (400-600 cm-1). 4.4.
Sample 𝑰𝒑𝒉 (𝑨) 𝑰dark(𝑨) S 𝑰𝑶𝑵/𝑰𝑶𝑭 NZTO 0% 1,66×10-5 1,37×10-6 12,2 0,081 NZTO 5% 1,68×10-6 1,25×10-6 1,34 0,74 NZTO 10% 1,24×10-6 1,23×10-6 1 1 NZTO 15% 1,23×10-6 1,23×10-6 1 1 From the data in Table 4, the photocurrent values ​​𝐼𝑝ℎ of TO and NZTO are measured with a bias of 12V.

Glass Sci. 1 (2010) 38–62
Mater. 354 (2006) 1–13
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Mater. 184 (1991) 1-21
Mater. 354 (2006) 1-13

FHWA-IF 12-052 - Vol. 1, November 2012
Stahlbau, v 56, n 1, p 1-8, Jan 1987 Language: German [56] Schijve, J., Jacobs, F.A. (1984).
ISRN Civil Engineering, 2012, 1-13.
Mahmoud, CRC Press 2013 Print ISBN: 978-1-138-00112-1 eBook ISBN: 978-1-315-85684-1, DOI: 10.1201/b15790-25
Engineering Structures, 33(1), 202-209.

Precipitates of 1µm can be seen in cell boundaries and grain boundaries.
The size of precipitates is about 1-2µm while the fraction is 1-3% and Ti2(Ni, Pd) precipitates are mostly found on grain boundaries.
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Superelasticity, 1, (2015) 85–106
Forum, 475–479, (2005) 1973–6

Figure 1.
Moreover, the specific surface area calculated by the BET model, total pore volume, and micropore volume of Fe3O4-NPs/AC at P/Po of 0.95 are 479 m2 g-1, 0.42 cm3 g-1 and 0.25 cm3 g-1, respectively, demonstrating a high porosity of the synthesized material.
qt= qe(1- e-k1t) (7) qt=qe2k2t1+qek2t (8) where qt (mg g-1) and qe (mg g-1) are the amount of Ni(II) ions adsorbed on Fe3O4-NPs/AC at any time t and at equilibrium, respectively; k1 (min-1) and k2 (g mg-1 min-1) are the rate constants of the pseudo-first and pseudo-second-order models, respectively.
Kinetic and isotherm parameters for adsorption of Ni(II) onto Fe3O4-NPs/AC Kinetic model Value Isotherm model Value Pseudo-first-order Langmuir qe (mg g-1)(exp) 33.06 qm (mg g-1) 50.72 qe (mg g-1)(cal) 32.83 KL (L mg-1) 0.062 K1 (min-1) 0.062 RL 0.039-0.243 R2 0.998 R2 0.989 Pseudo-second-order Freundlich qe (mg g-1)exp 37.83 KF (mg1−1/n L1/n g-1) 10.73 K2 (g mg-1 min-1) 0.002 1/n 0.291 R2 0.993 R2 0.967 Fitting the experimental adsorption data to different isotherm models is an important step to find a suitable model that can be used for designing the adsorption process in practice.
The values of ΔH (kJ mol-1) and ΔS (kJ mol-1 K-1) were calculated from the slope and the intercept of a plot of lnKc and T-1 (Figure 6), respectively [42].

Fig. 1 Fig. 2 Fig. 3 Fig.1.
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Thermochim acta 280:479-490. 33.

Table 1.
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ISIJ Int. 54 (2014) 1–8. https://doi.org/10.2355/isijinternational.54.1 [6] S.P.
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