Characterization of ZFN-CTAB
The FT-IR spectra of ZFN and ZFN-CTAB were shown in Figure 1. ZFN has two peaks at 3450 cm−1 and 500–600 cm−1 which indicate O-H stretching vibration and metal-oxygen vibration, respectively. The FTIR spectrum of the ZFN-CTAB displays a number of characteristic bands at 3426 cm−1 and 2900–2800 cm−1 (Figure 1). These bands are assigned to O-H stretching vibration and -CH2- stretching vibration of adsorbed CTAB, respectively [16].SEM is useful for determining the particle shape and appropriate size distribution of the adsorbent. In addition, SEM is a primary tool for characterizing the surface morphology and fundamental physical properties of the adsorbent surface. Scanning electron micrograph of magnetic nanoparticle before and after the modification with the CTAB was shown in Figure 2. The SEM image of samples reveals that ZFN and ZFN-CTAB exhibit a compact arrangement of homogeneous nanoparticles with roughly spherical shape. It can be seen that the particle size of samples are smaller than 80 nm.
Figure 3a illustrates the XRD pattern of the CTAB. It has no different characteristic diffraction peaks in the spectrum were observed. The X-ray diffraction pattern of the ZFN-CTAB (Figure 3b) showed that spinel was formed as the most intense (311) peak and Miller indices (220), (222), (400), (422), (511) and (440) matched well with the reflections of the zinc ferrite reported in the previous published paper [17].
Effect of operational parameter on dye removal
Effect of adsorbent dosage
The dye removal using ZFN without surface modification (Dye: 50 mg/L, 0.4 g ZFN and pH = 7) was shown in Figure 4. The dye removal efficiency of ZFN was obtained 51, 27 and 23% for DR31, DG6 and DR23, respectively. In additional dye removal using ZFN-CTAB at different adsorbent dosages (g) was shown in Figure 5.
The increase in dye adsorption with adsorbent dosage is due to the increasing of adsorbent surface and availability of more adsorption sites. However, if the adsorption capacity was expressed in mg adsorbed per gram of material, the capacity decreased with the increasing amount of adsorbent. It can be attributed to overlapping or aggregation of adsorption sites resulting in a decrease in total adsorbent surface area available to the dye and an increase in diffusion path length [18]. The results showed that ZFN-CTAB has higher dye removal efficiency in compare with unmodified ZFN. Thus for further study, optimum amount 0.4 g of ZFN-CTAB was used.
Effect of dye concentration
Adsorption can generally be defined as the accumulation of material at the interface between two phases [18]. The influence of varying the initial dye concentration of dyes on adsorption efficiencies onto ZFN-CTAB was assessed. The results are shown in Figure 6. It is obvious that the higher the initial dye concentration, the lower the percentage of dye adsorbed. Dye removal of ZFN-CTAB at 50, 100, 150 and 200 mg/L dye concentration was 67, 42 34 and 26% for DR23, 86, 54, 40 and 27% for DR31 and 89, 68, 60 and 49% for DG6, respectively. Furthermore, in ternary system, dye removal of ZFN-CTAB at 90, 120, 150 and 200 mg/L dye concentration was 63, 45, 30 and 23% for DR23, 97, 90, 78 and 45% for DR31 and 51, 48, 42 and 37% for DG6, respectively.
The amount of the dye adsorbed onto ZFN-CTAB increases with an increase in the initial dye concentration of solution if the amount of adsorbent is kept unchanged. It can be attributed to the increase in the driving force of the concentration gradient with the higher initial dye concentration. The adsorption of dye by ZFN-CTAB is very intense and reaches equilibrium very quickly at low initial concentration. At a fixed ZFN-CTAB dosage, the percentage of adsorption decreased. In other words, the residual dye concentration will be higher for higher initial dye concentrations. In the case of lower concentrations, the ratio of initial number of dye moles to the available adsorption sites is low and subsequently the fractional adsorption becomes independent of initial concentration [18].
Effect of pH
The effect of pH on the adsorption of dyes onto ZFN-CTAB is shown in Figure 7. At various pH values, the electrostatic attraction as well as the organic property and structure of dye molecules and ZFN-CTAB could play very important roles in dye adsorption on ZFN-CTAB. At pH 2, a significantly high electrostatic attraction exists between the positively charged (−N+) surface of the ZFN-CTAB and negatively charged anionic dyes. As the pH of the system increases, the number of positively charged sites decreased. It does not favor the adsorption of anionic dyes onto ZFN-CTAB.
Effect of salt
The inorganic anions exist in colored industrial wastewater [19]. These substances may compete for the active sites on the adsorbent surface or deactivate the adsorbent. Thus, dye adsorption efficiency decreases.
To investigate inorganic salts effect on dye removal efficiency, 0.02 M of NaHCO3, Na2CO3 and Na2SO4 were used. Figure 8 illustrates that dye removal efficiency of ZFN-CTAB is decreased in the presence of inorganic salts because these salts have small molecules and compete with dyes in adsorption by ZFN-CTAB.
Comparison of single and ternary systems
The results obviously showed that DR31 was removed more than other dyes in ternary system for all effects. The study of dyes adsorption demonstrated that the percentage of adsorption decreased in ternary system (150 ppm) in compare with single system (50 ppm) for each dyes; because some of adsorption sites occupies with other dyes. Investigating of other effect showed that adsorption of dyes had same procedure in both single and ternary systems.
Adsorption isotherm
The adsorption isotherm is important to design of adsorption systems. The mechanism of dye removal was studied by isotherm models. The relation between the mass of the dye adsorbed at a particular temperature, the pH, particle size and liquid phase of the dye concentration is discussed by the adsorption isotherms. The current research presents a method of direct comparison of the isotherm fit of several models to enable the best-fit and best isotherm parameters to be obtained [20–22]. Several isotherms such as Langmuir, Freundlich and Tempkin models were studied in details [23–25].
The Langmuir isotherm explains the adsorption of dye into adsorbent. A basic assumption of the Langmuir theory is that adsorption takes place at specific sites within the adsorbent [26–29]. The Langmuir equation can be written as follows:
(1)
where q
e
, C
e
, K
L
and Q
0
are the amount of dye adsorbed at equilibrium (mg/g), the equilibrium concentration of dye in solution (mg/L), Langmuir constant (L/g) and the maximum adsorption capacity (mg/g), respectively.
The linear form of Langmuir equation is:
(2)
The Freundlich isotherm was developed mainly to allow for an empirical account of the variation in adsorption heat with concentration of an adsorbate (vapor or solute) on an energetically heterogeneous surface.
Isotherm data were tested with Freundlich isotherm that can be expressed by [26]:
where K
F
is adsorption capacity at unit concentration and 1/n is adsorption intensity.
Eq. (4) can be rearranged to a linear form:
(4)
The Tempkin isotherm considered the effects of indirect the heat of adsorption of all the adsorbate molecules on the adsorbent surface layer would decrease linearly with coverage due to adsorbate –adsorbate interactions. The Tempkin isotherm is given as [30]:
(5)
which can be linearized as:
(6)
Where
K
T
is the equilibrium binding constant (L/mg) corresponding to the maximum binding energy and constant B
1
is related to the heat of adsorption.
The parameter values related to Langmuir, Freundlich and Tempkin isotherms were calculated from the slope and intercept of the plots (Ce/qe vs. Ce), (log qe vs. log Ce) and (qe vs. lnCe), respectively. The values of Q
0
, K
L
, K
F
, 1/n, K
T
, B
1
and R2 are shown in Table 2.
Table 2
Linearized isotherm coefficients for dye adsorption onto ZFN-CTAB (Q
0
: mg/g; K
L
: L/mg; K
F
: L/g; K
T
: mg/L and B
1
: mg.g
−1
)
The R2 values show that the dye adsorption isotherm using ZFN-CTAB does not follow the Freundlich and Tempkin isotherms (Table 2). The linear fit between the C
e
/q
e
versus C
e
and the calculated R2 values for Langmuir isotherm model show that the dyes adsorption isotherm can be approximated as Langmuir model (Table 2). This means that the adsorption of dyes takes place at specific homogeneous sites and a one layer adsorption onto ZFN-CTAB surface. The maximum adsorption capacity (Q0) was 26.1, 55.5 and 64.1 mg/g for DR23, DR31 and DG6, respectively.
The maximum adsorption capacity of several adsorbents was shown in Table 3. The results show that ZFN-CTAB has high dye adsorption capability. Thus ZFN-CTAB can be used as an adsorbent to remove dyes.
Table 3
The dye removal ability of different magnetic adsorbents
Adsorption kinetic
The adsorption rate of dyes onto adsorbent was investigated by adsorption kinetics. Adsorption kinetic using pseudo-first order equation, pseudo-second order equation and intraparticle diffusion model were determined in order to investigate the mechanism of dye adsorption onto different adsorbents [31, 32].
A linear form of pseudo-first order model (Eq. 8) is [31]:
(8)
where q
e
, q
t
and k
1
are the amount of dye adsorbed at equilibrium (mg/g), the amount of dye adsorbed at time t (mg/g) and the equilibrium rate constant of pseudo-first order kinetics (1/min), respectively. The linear fit between the log (q
e
–q
t
) and contact time (t) can be approximated as pseudo-first order kinetics.
Linear form of pseudo-second order model (Eq. 9) was illustrated as:
(9)
where k
2
is the equilibrium rate constant of pseudo-second order (g/mg min).
The possibility of intraparticle diffusion resistance affecting adsorption was explored by using the intraparticle diffusion model as:
(10)
where k
p
and I are the intraparticle diffusion rate constant and intercept, respectively.
To understand the applicability of the kinetics models for the dye adsorption onto ZFN-CTAB, linear plots of log(q
e
-q
t
) versus contact time (t), t/q
t
versus contact time (t) and q
t
against t1/2 are plotted. The values of k
1
, k
2
, k
p
, I, R2 (correlation coefficient values) and the calculated q
e
((q
e
)
Cal
.) are shown in Table 4.
Table 4
Linearized kinetic coefficients for dye adsorption onto ZFN-CTAB (Adsorbent: g; (q
e
)
Exp
: mg/g; (q
e
)
Cal.
: mg/g; k
1
: 1/min; k
2
: g/mg min and k
p
: mg/g min
1/2
)
The linearity of the plots (R2) demonstrates that pseudo-first order and intraparticle diffusion kinetic models do not play a significant role in the uptake of the dye by ZFN-CTAB (Table 4). The linear fit between the t/q
t
versus contact time (t) and the calculated R2 values for pseudo-second order kinetics model show that the dye removal kinetic can be approximated as pseudo-second order kinetics (Table 4). In addition, the experimental q
e
((q
e
)
Exp
.) values agree with the calculated ones ((q
e
)
Cal
.), obtained from the linear plots of pseudo-second order kinetics (Table 4).