3.1 Characterization of the Biosorbent
Below is the result of the Characterization of Silver nanoparticles (AgNPs).
Scanning Electron Microscope (SEM) Analysis of Silver Nanoparticle
The SEM image of the silver Nanoparticle is given in Fig. (1), this image shows the uniformity in the size of the nanoparticle.
Fourier Transforms Infrared (FTIR) Spectroscopy of Silver Nanoparticle (AgNPs)
FTIR measurements were performed to recognize the involvement of various functional groups in biomolecules responsible for bioreduction of Ag + and capping/stabilization of silver nanoparticles. The observed strong bands were compared with the standard values to classify the functional groups. At 2921, 2856, 1743, 1631, 1377, 1240, 1043 and 596 cm-1, the FTIR spectrum displays absorption bands suggesting the presence of capping agent with nanoparticles. It has a functional group of O-H. The spectrum confirmed the presence of aromatic amine, amide group, phenolic group and secondary alcohols which may act as a reducing agents for synthesis of silver nanoparticle similar result was also confirm (Wang et al. 2017).
Effect of environmental parameters
Effect of pH
The pH is the most important effect in the study of biosorption. The sorption of the sorbate on the sorbent is often influenced by the increase or decrease in the pH. It allows us to understand the physiochemical relationship between sorbate and sorbent. The solution's pH has a significant influence on DMP uptake because it determines the adsorbent's surface charge and also determines the speciation of the adsorbate and degree of ionization (DMP). This analysis was done with 100ml each of a different concentration of 250–500µg/ml respectively which contained a dried amount of 0.5g of Yeast Based Silver Nanoparticle (sorbent) at different pH of range 3–6 at 300c to study the initial pH effect on the ability dimethyl phthalate removal. As shown in Fig. 3. It can be observed that increasing pH tends to increase in the DMP adsorption quantity (Fomina and Gadd 2014). This increase gradually reach the maximum value sharply at pH 5 and then it remained constant over a wide pH region. It was also observed that sorption rate of DMP was slightly decreased at a pH of 6.0 due to the dimethyl phthalates ion struggle to hydrolyse and precipitate exceedingly by Biosorption (Soni et al. 2012). Further experiments were performed at the initial pH of value 5 in this analysis.
Effect of Temperature
The temperature effect on dimethyl phthalate biosorption was carried out by analyzing temperatures between 30 and 50ºC at pH 5, by using different concentrations of 500–900 µg/ml of dimethyl phthalate with 0.5g of Yeast Based Silver Nanoparticle (Awad, and Erkurt 2014) with the equation above, the equilibrium value of dimethyl phthalate at various temperature range was calculated. The effect of temperature on biosorption by YB-AgNPs is shown in Fig. (4).
However, it can be observed in Fig. (4) that the optimum temperature for this study is 50oC. This condition (50oC) is where the maximum DMP removal (92%) was observed. The effect of temperature in Fig. (4) below show that less DMP remain when the temperature was 50ºC, while the concentration of DMP in the aqueous solution increase with the increase in temperature in fig.( 4). In the aqueous solution the temperature has more effect on DMP biosorption. This may be due to the low temperature, the viscosity of DMP solution on the surface of YB-AgNPs (Wang and Chen 2006). It was also shown from the result that the adsorption study is an Endothermic (Osman et al. 2013). The result of this study was further confirmed that, increases in temperature have much influence in the adsorption study.
The Effect of Initial DMP Concentration
The initial concentration of DMP has great influence on biosorption process. The effect of different initial DMP concentration (500 µg/mto 900 µg/ml) of DMP on biosorption was investigated for 60mins. Steady Increment in likely trends, in biosorption capacity as initial concentration increases from 500 to 900 µg/ml can be observed. The oxidation rate of DMP was increased with respect to increase in the initial concentration of DMP in the reaction Fig. (5), (Jabesa and Ghosh 2016).
Effect of Contact Time
Interaction between the elimination of DMP with contact time was observed to examine the rate at which DMP were removed by YB-AgNPs at different initial DMP concentration and also at different pH and constant concentration of DMP (700 µg/ml). The biosorption of DMP in YB-AgNPs was studied to be a fast process.
It was significant that the rate of biosorption was rapid in the initial stage (5 mins), thereafter continue at a slower and steadily and eventually reached equilibrium at different contact time for different concentration at initial of DMP (Fig. 6). The higher the DMP initial concentration, the higher time required to reach equilibrium. It was noticed that the rate of DMP sorption is not affected by contact time. Under the below conditions, (Fig. 6) shows that the adsorption amount reaches equilibrium value at 30 min and a subsequent little change of sorption occurs (i.e, remains constant thereafter), hence there was no significant changes at contact time. A similar result was obtained when methylene blue dye was removed using polydopamine microsphere (Esfandian et al. 2016).
Effect of Biosorbent Dosage
The effect of biosorbent dosage was determined on the biosorption of DMP. It was observed from the graph that as the biosorbent dosage increased, there was decrease in biosorption. It also means that the lower the dosage of the biosorbent used the higher the biosorption capacity (mg/g). The biosorbent dosage with the highest biosorption capacity is 0.25g (1752 mg/g) followed by 0.5g (900mg/g) while the lowest biosorption capacity was recorded using 1g (512mg/g) which was the highest biosorbent dose used in this experiment (Fig. 7).
Therefore, an increase in biosorbent dosage brought about an increase in the percentage of DMP removal (Fig. 7). The highest percentage of DMP removal was observed with 1g biosorbent dosage (75.29%) followed by 0.5g (66.18%) while the lowest percentage of DMP removal was observed with 0.25g biosorbent dosage (64%). Increment of electrostatic relationship at high biomass fixation could inhibit DMP molecule absorption. DMP molecules in the solution will enter the intracellular part at a low biomass dosage, thereby increasing the concentration gradient of the DMP molecule. It can be said that the capacity of biosorption is improved by increasing the intercellular distance (low biosorbent dosage) (Mahmoud et al., 2016). It was also observed, that increase in biosorption capacity with decreasing biosorbent dose and increase in percentage dye removal with increasing biosorbent dosage when Saccharomyces cerevisiae was used to decolorize certain reactive dye from aqueous solution(Kumari et al. 2007) another study also revealed similar results when S. cerevisiae and R. nigricans was used to adsorb reactive green dye.
Adsorption Isotherms
The relevance of our experimental data for different isotherm models, namely Langmuir, Freundish, and Temkin model, were tested and the results were given in Table (1). The adsorption equilibrium was characterization adsorption equilibrium was characterize by Langmuir, Freundish, and Temkin model.
Langmuir Model
For equilibrium analysis, this is the most commonly used isotherm model (Dada et al. 2012).The model relies on the premise that adsorption occurs on a single layer of the uniform surface (homogeneous of limiting destinations equitably transmitted over the adsorbent's surface, i.e. the adsorbent's surface, i.e. There is a similar biosorption partiality in limiting locations and there is no correlation between the adsorbed molecules and biosorbent free sites. This implies that the active sites are all energetically equal. The model is given a
$${\text{q}}_{\text{e}}=\frac{{\text{q}}_{\text{m}}{\text{b}\text{C}}_{\text{e}}}{1+\text{b}{\text{C}}_{\text{e}}} \left(4\right)$$
If the equation changes into a linear form, it is expressed as
\(\frac{1}{{\text{q}}_{\text{e}}}\) =\(\frac{1}{\text{b}{\text{q}}_{\text{m}}}\frac{1}{{\text{C}}_{\text{e}}}\)+\(\frac{1}{{\text{q}}_{\text{m}}} \left(5\right)\)
Ce= the equilibrium concentration of adsorbate (µg/ml)
qe = greatest monolayer capacity of sorption (mg/g)
b = Langmuir isotherm constant (L/mg)
Therefore, qm or Q0 (highest adsorption capacity) values of biosorbent and b (adsorption constant) are determined from a slope of 1/qeq and 1/ceq respectively. The significant attribute of the isotherm of Langmuir is revealed as RL (a constant without dimension), referred to as the factor of separation. RL can be calculated using the following equation, expressed as
RL=\(\frac{1}{1+\text{b}{\text{C}}_{0}} \left(6\right)\)
The RL value indicates that the isothermal form is irreversible when (RL = 0), favorable when (0 ˂ RL ˃), liner when (RL = 1) or unfavorable (RL ˃).
Table 1
Parameter value of Langmuir, Freundlich, and Temkin Isotherm for adsorption of Dimethyl phthalate on silver nanoparticle-b on yeast (YB-Agapes).
Isotherm model | Parameters | Temperature (⁰C) |
| | 30 | 40 | 50 |
Langmuir | QO (mg/g) | 360 | 746 | 924 |
B (L/m g) | 0.014 | 0.070 | 0.055 |
RL* | 0.0053 | 0.0016 | 0.0021 |
R2 | 0.9685 | 0.9156 | 0.9918 |
Freundlich | KF (mg/g) | 56.46 | 160.20 | 4.46 |
1/n | 0.2828 | 0.2483 | 9.0468 |
N | 3.54 | 4.03 | 0.1105 |
R2 | 0.9578 | 0.9067 | 0.9871 |
Temkin | AT(L/mg) | 382.71 | 760 | 1064.02 |
bT | 12.89 | 4.13 | 0.04 |
B | 195.43 | 630.09 | 998.55 |
R2 | 0.9761 | 0.9736 | 0.5605 |
The Regression coefficient (R2) of Langmuir model for all the temperatures are closer to 1 and higher than Freundlich model. Also, the monolayer maximum adsorption limit estimated from Langmuir for 40o C and 50oC are 924 and 746 mg/g respectively. The closeness of these values to experimental data (904 and 694mg/g) for both 40 and 50oc suggest good application of Langmuir model for his experiment. Likewise, the RL of Dimethyl phthalate adsorption which ranges from (0.0014 and 0.0053) is a good indication that the biosorption of Dimethyl Phthalate onto YB-AgNPs is favorable.
Freundlich Isotherm
The Freundlich isotherm model is often used to represent a heterogeneous surface's adsorption characteristic; the isotherm is thus derived to model multi-layer adsorption (Dada et al. 2012).The actual linear formula initiated by Freundlich is defined as:
$${{\text{q}}_{\text{e}}={\text{K}}_{\text{F}}\text{C}}_{\text{e}}^{\frac{1}{\text{n}}} \left(7\right)$$
Linearizing the equation, it gives
\(\text{l}\text{n}{\text{q}}_{\text{e}}\)=\(\text{l}\text{n}{\text{K}}_{\text{F}}+\frac{1}{\text{n}}\text{ln}{\text{C}}_{\text{e}} \left(8\right)\)
Where KF = Freundlich isotherm steady (mg/g); n = adsorption force; Ce= Concentration of adsorbate (mg/L); qe is the measurement of sorbate adsorbed per gram of adsorbent at balance (mg/g); Kf and 1/n can be computed from the plot of Inqeq against Inceq. The value of 1/n according to the isotherm is between 0 and 1 for the biosorption to be consider effective. It was observed from the data Table 1, the adsorption process can not fit well to freundlich model as R2 parameters are lower compared to Langmuir isotherm. And also the N value exceeds 1 except for 500C.
The nature of adsorption result observed can be consider monolayer because Q0˃Kf for all the result in the four temperature analyzed. (Table 1).
Temkin Isotherm
The relation between the adsorbate and the adsorbent is specifically evaluated by this isotherm. The model acceptance (temperature capacity) of all atoms in the layer will decrease linearly by neglecting very low and extensive concentration values as compared to logarithmic with Scope. As indicated in the case, its deduction is defined by a uniform transmission of limiting energies (up to some of the most extreme limiting energy) by plotting the volume sorbed qe against ln Ce and measuring the constants from the slope and intercept. The following equation provides the mode
\({\text{q}}_{\text{e}}\) =\(\frac{\text{R}\text{T}}{\text{b}}\text{ln}{(\text{A}}_{\text{T}}{\text{C}}_{\text{e}}\left) \right(9)\)
By linearizing the equation, we have
\({\text{q}}_{\text{e}}\) = \(\frac{\text{R}\text{T}}{{\text{b}}_{\text{T}}}\text{ln}{\text{A}}_{\text{T}}\)+ (\(\frac{\text{R}\text{T}}{\text{b}}\left)\text{l}\text{n}{\text{C}}_{\text{e}} \right(10)\)
B =\(\frac{\text{R}\text{T}}{{\text{b}}_{\text{T}}} \left(11\right)\)
\({\text{q}}_{\text{e}}\)=B\({\text{l}\text{n}\text{A}}_{\text{T}}\)+B\({\text{l}\text{n}\text{C}}_{\text{e}} \left(12\right)\)
AT = Temkin isotherm harmony restricting consistent (L/g)
BT = Temkin isotherm steady
R = Gas steady constant (8.314J/mol/k)
T = Temperature at 298K
B = Constant identified with warmth of sorption (J/mol)
It was observed from the result from the above table (AT = 0.04–12.89 L/g, B = 195.43–998.55 J/mol and R2 = 0.5605–0.9761) is a sign that adsorption process was good for all temperature (Dada et al. 2012).
Kinetic Studies
What governs the kinetic adsorption is the rate at which DMP molecules are exchanged for the surface of the adsorbent from the mass solution. It gives an understanding of the possible sorption mechanism, and the time it takes for the sorbate particle to remove on the sorbent's surface.
Pseudo First Order
As far as adsorption capability is concerned, this model is one of the first known to illustrate the rate of adsorption. It is based on the premise that the rate of adsorption is proportional to the limitations on the quantity of free areas (Yousefi et al. 2016) given by;
\({\text{ln}(\text{q}}_{\text{e}}\)-\({\text{q}}_{\text{t}})\)=\({\text{ln}\text{q}}_{\text{e}}-{\text{k}}_{1} \text{t} \left(13\right)\)
Where qe and qt are the equilibrium and time adsorbent adsorption limit; t (mg/g), K1 is the constant pseudo-first order rate (min-1). The of kinetic constants value are measured from the slope and intercept of the plotted graph ln (qe -qt) against t. The relationship coefficient values (R2) are used as a measure for the quality of the fit for the trial. In addition to the relationship coefficient values (R2), the estimates of computed qe and K1 are given in Table 2 in this investigation. The low qe (calc) and even the low R2 values imply that the model is not appropriate to this method compared to the qe (exp) values.
Pseudo Second Order Model
Pseudo-second order model relies on premise that adsorption rate corresponds to the quantity square of empty binding sites (McKay et al. 1999.). In linear terms, the model is depicted as
\(\frac{\text{t}}{{\text{q}}_{\text{t}}}\)=\(\frac{1}{{\text{k}\text{q}}_{\text{e}}2}\) + \(\frac{1}{{\text{q}}_{\text{e}} \text{t}} \left(14\right)\)
Therefore: K is pseudo-second order rate constant (min− 1). The slope and intercept of t/qt against t plot gives the individual estimate of qe and K (Table 2). The expression h (mg/g min) that defines the initial sorption rate can be determined by:
h=\({\text{k}\text{q}}_{\text{e}}2 \left(15\right)\)
The qi (calc) values are as similar as the qe (exp) values for the adsorbent from Table 2. In addition, the coefficients obtained for this model in this analysis are higher (> 0.99) for temperatures than all other examined models indicating that second order kinetic kinetic will positively represent the procedure.
Table 2
Kinetic parameters values of Dimethylphthalate biosorption onto Yeast Based Silver Nanoparticle at different temperatures and pH
Model Parameters | Temperature | pH |
| | 30 | 40 | 50 | 3 | 4 | 5 | 6 |
Pseudo First order | | | | | | | | |
qe (mg/g) | | 341.72 | 1339.97 | 910.51 | 471.54 | 258.01 | 368.7 | 343.8 |
K1(min-1) | | 0.0802 | 0.1997 | 0.0802 | 0.3078 | 0.2354 | 0.15 | 0.0112 |
R2 | | 0.9992 | 0.9344 | 0.7964 | 0.8213 | 0.9325 | 1 | 1 |
Pseudo Second order | | | | | | | | |
Qe (mg/g) | | 416.67 | 1833.3 | 1666.67 | 333.33 | 270.27 | 384.62 | 344.83 |
K2(g/mg.min) | | 0.0020 | 0.0012 | 0.00026 | 0.0012 | 0.0013 | 0.0013 | 0.02 |
R2 | | 0.982 | 0.9796 | 0.9807 | 0.9975 | 0.9433 | 0.993 | 1 |
Weber-Morris | | | | | | | | |
Kid (mg.min0.5) | | 47.55 | 97.302 | 167.95 | 38.307 | 31.311 | 46.063 | 61.514 |
C | | 22.068 | 61.217 | 30.989 | 89.052 | 94.283 | 104.98 | 93.759 |
R2 | | 0.9115 | 0.8815 | 0.9882 | 0.7088 | 0.6252 | 0.6483 | 0.6593 |
Weber Morris Kinetic Model
As indicated by this model, if intraparticle dispersion occurs in the entire adsorption system, the plot of qt versus t1/2 is said to be linear (C = 0) and the dissemination intraparticle is one of the key rate constraining phase of the method, in any case, in a case where the line did not cross the root (C ≠ 0) both intraparticle dispersion and limit phase impact both occur in the adsorption process. The model can be related to the straight formula underneath.
\({ \text{q}}_{\text{t}}= {\text{k}}_{\text{d}}{\text{t}}^{1/2}\)+\({\text{C}}^{1/2} \left(16\right)\)
Where kd (mg/g.min1/2) is a constant rate of Weber Morris model and C is intercepte, it can be seen from the table that C ≠ 0 indicates that the biosorption of DMP on YB-AgNPs was influenced by both intraparticle diffusion and boundary layer and also shows that the model of diffusion intraparticle was not the major rate controlling phase.
Adsorption Thermodynamics
Thermodynamic experiments were performed to establish the adsorption mechanism of DMP on YB-AgNPs at various temperatures (303-323k). Using change in free energy (ΔG), change in enthalpy (ΔH) and change in entropy (ΔS) given by the equations below, the thermodynamic parameters were calculated.
ΔG = -RT\(\text{ ln}{\text{K}}_{\text{C}} \left(17\right)\)
The change in enthalpy (ΔH) and change in entropy (ΔS) parameters were calculated from the equation below
\(\text{ln}{\text{K}}_{\text{C}}\) = \(\frac{{\Delta }\text{S}}{\text{R}}-\frac{{\Delta }\text{H}}{\text{R}\text{T}} \left(18\right)\)
Where ΔG is the Gibbs free energy change,
T: temperature (K), KC (qe/Ce) is called constant of equilibrium.
ΔH and ΔS of biosorption method were observed from the slope and the intercept of the plot of In KC versus 1/T, respectively. The value of ΔH, ΔS, and ΔG were determined using the equations above.
Table 3
Thermodynamic parameters for Adsorption of Dimethyl phthalate on Yeast Based Silver Nanoparticle.
T(K) | ΔGo (kJ/mol) | ΔSo (J/mol k) | ΔHo (KJ/mol |
303 | -1.04 | 244.3 | 74.9 |
313 | -1.91 | | |
323 | -3.70 | | |
Table 3, provides the values of these parameters. It implies that the shift in enthalpy ΔH is positive (endothermic) due to the rise in adsorption for consecutive temperature increases. The negative values of ΔG have shown that sorption is thermodynamically viable and spontaneous in nature. The positive value of ΔS demonstrates the increased randomness at the solid-solution interface during the fixation of the ion at the active locations of the sorbent (Esfandian et al. 2016). According to the literature, physisorption is considered to be G values between 0 and-20 KJ/mol while chemisorption is considered to be chemisorption values between − 80 and − 400 KJ/mol (Özcan et al. 2014). ΔG calculated or YB-AgNPs at different temperatures are between 0 and − 20 which indicates the physical adsorption process.