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Dec.1, 2007  Vol.9 No.12 P.53 Copyright cij17logo.gif (917 bytes)


Adsorption kinetics of basic fuchsine and auramine lake yellow O on expanded graphite

Pang Xiuyan1, Lv pu1, Gong fei1, Ren Haili1, Liang Xiuhua2
(1College of Chemistry and Environmental Science, Hebei University, Baoding, 071002; 2School of Engineering Technology, Hebei, Baoding, 071002)

Abstract In order to investigate the adsorption kinetics of dyes Basic fuchsine (BF) and Auramine lake yellow O (ALYO) on expanded graphite (EG), EG was prepared with 50 mesh crude graphite after chemical oxidation intercalation of potassium permanganate and vitriol. Based on pseudo first-order and second-order kinetic model, the adsorption models of EG for the two dyes are discussed. Adsorption rate and activation energy of BF and ALYO on EG are calculated, and the rate-limiting step for the adsorption process based on the second law of Fick are investigated. Kinetic studies show that the kinetic data are well described by the pseudo second-order kinetic model. Equilibrium adsorbance and initial adsorption rate increases with the increase of the initial dyes concentration. Adsorption process of BF on EG holds small adsorbing activation energy. The internal diffusion appears to be the rate-limiting step for the adsorption process.
Keywords Expanded graphite, adsorption kinetics, rate-limiting step, Basic fuchsine, Auramine lake yellow O

1. INTRODUCTION
As a main source of industrial wastewater, colored wastewaters require pretreatment for color prior to disposal into receiving water bodies or publicly owned treatment works. While both biological and physical/chemical methods have been employed for dyes removal, the former method applied has not been very successful, due to the essential non-biodegradable nature of most of the dyes.Adsorption is a kind of effective measure, active carbon [1-4], anion exchange resin [5], active sludge [6, 7], peat, steel plant slag and fly ash [8] have been reported to be employed for the treatment of dyes. According to Walker's adsorption experiment of acid dyes on active carbon [1], micropore structure was found to be redundant in the adsorption of large molecular weight compounds such as dyes, and only 14% of the total specific surface of the activated carbon is available for adsorption due to the high molecular area and aggregation of the dye.
    Expanded graphite (EG) is a kind of eco-material. It attracts attentions of scientists and engineers as an absorbent with a high sorption capacity for organic materials, such as heavy oil and biomedical molecules [9], because of its large pores structure. But it has been reported not so much about its application in adsorbing of dyes from wastewater. Wang pressed the worm-like particles into low-density plate of 0.1g/cm3. In the treatment of dye waste-water from woolen mill, a decreasing rate of chemical oxygen demanded of 40% was obtained [10]. Research group of Hebei normal university carried out a thermodynamics study of dyes on EG. They reported that the sorption capacity of dyes was influenced by various factors, not only the expanded volume of EG, primary concentration of dyes, but also the amount of EG and pH [11]. Study on the sorption of medium yellow GG on EG proved that the decolored rate arrived to 97% [12]. However, a systematic adsorption kinetics studies need to be carried out to enrich the sorption theory of EG.
    Basic fuchsine (BF) and Auramine lake yellow O (ALYO) are two kinds of dyes with tritane structure and biphenyl methane structure, respectively. They can dissolve in water and often hold deep chroma. Both of them are popularly used in the pigmentation of cotton textile, silk, leather, paper, oil, fat, paint, and so on. In this paper, the sorption kinetic characteristics of BF and ALYO on EG are studied.

2. EXPERIMENTAL
2.1 Preparation and characteristics of EG
Expandable graphite was prepared with 50 mesh crude graphite (C) as material, KMnO4 as oxidant (KMnO4 : C = 0.15:1, mass ratio) and vitriol as intercalation compound (H2SO4: C = 5:1, mass ratio, the mass concentration of vitriol was 50%). EG was prepared with expandable graphite expanded in KSW heating oven at 900 ºC. Structural parameters of EG were characterized by expanded volume, specific surface area and total pore volume. These data were detected with AutoPore II 9220 Mercury Porosimeter (Micromeritics Inc. USA) under varying pressures of 0.58 PSIA to 59814.12 PSIA. The porosity characteristics were showed as Table. 1.

Table. 1 Structural parameter of expanded graphite

Expanded volume
(ml / g)

Specific surface area
(m2/g)

Total pore volume
(cm3/g)

330

1044.99

30.1145

2.2 Sorbates
Dyes of BF with tritane structure and ALYO with biphenyl methane structure were selected as reference compounds. Molecular structures and molecular weight of these dyes are shown in Table. 2.
    Simulated dye wastewaters were prepared by dissolving the different dyes in distilled deionized water at various concentrations. Absorbance values were recorded at the wavelength for maximum absorbance (
lmax) corresponding to each dye and its solution was initially calibrated for concentration in terms of absorbance units.

Table. 2 Chemical structure and molecular weight of dyes used for experiment

Dyes

Structure

Molecular weight

lmax(nm)

BF

338.5

543

ALYO

318.5

430

 

2.3 Adsorption of dye
In adsorption kinetics experiments, a series of desired dye concentration and of fixed volume 100.0 ml were placed in vessels where they were brought into contact with EG at 5ºC, 25 ºC and 45ºC, respectively. The mass of adsorbent to volume of solution was standardized at M/V=0.200 g/0.l l=2.00 g/l. The absorbency of dye solution corresponding to different adsorption time was then analysed, and it was used to calculate the solid phase dye concentration q. The amount of adsorbate captured by the adsorbant was determined as the following:
q= V(C0-C)/M (1)
    where:
    q adsorption amount of adsorbate on adsorbent; mg/g
    C0 initial concentration of dye in solution; mg/l
    C concentration of dye in solution corresponding to a definite time; mg/l
    M mass of adsorbent; g

3 RESULTS AND DISCUSSION
3.1 Equilibrium time
The amount of dyes adsorbed is showed as a function of time in Fig.1~2. As showed in these figures, adsorption occurs more rapidly at higher temperature: it takes only 3.0 h or 4.0 h to reach the adsorption equilibrium at 45ºC, while it takes about 24.0 h at 5ºC. Initial dyes concentrations do not have a significant effect on the equilibrium time.

                          (a)               

                          (b)
Fig. 1 Influence of initial BF concentration and temperature on adsorption kinetics. Initial BF concentration is (a) 100 mg/l, (b) 200 mg/l; temperature() 5ºC, () 25ºC, () 45ºC


            (a)    

            (b)
Fig. 2 Influence of initial ALYO concentration and temperature on adsorption kinetics. Initial ALYO concentration is
(a) 100 mg/l, (b)200 mg/l; temperature (
)5ºC, ()25ºC, ()45ºC

3.2 Adsorption kinetic models
Both pseudo first- and second-order adsorption models were used to describe the adsorption kinetics data [13, 14]. In both models, all the steps of adsorption such as external diffusion, internal diffusion, and adsorption are lumped together, the overall adsorption rate is proportional to either the driving force (as in the pseudo first-order equation) or the square of the driving force (as in the pseudo second-order equation).
First-order model
ln(qe-q)=lnqek1t                  (2)
Second-order model
t/q=1/(k2 qe2)+t/qe          (3)
    where:
    k-adsorption rate constant (min-1 for first-order adsorption, g·mg-1·min-1 for second-order adsorption)
    t
-adsorption time (min)

    Since q reaches a plateau (qe) at equilibrium, q values smaller than the 0.9qe were used for analysis. The plots of ln(qe-q) versus t and t/q versus t were used to test the first- and second-order models, and the fitting results are given in Table. 3 and Table. 4. According to the correlation coefficients, second-order model gives satisfactory fits. At the same time, the qe,cal obtained from the intercepts is obviously inconsistent with the experimental data qe,exp in the first-order model. In the second-order model, the qe,cal agrees reasonably well with the experimental data. Thus, the second-order model is more suitable to describe the adsorption kinetics data. Similar results were observed in biosorption of dye Remazol Black B, RB2, PY2 on biomass and BBF on xerogel [15-17], anionic dye adsorption on cross-linked chitosan beads [14, 18], and polyethylene glycol (PEG) adsorption on zeolite [19].
    Based on the second-order model, the initial adsorption rate and half-adsorption time are estimated in Table. 5 and Table. 6 according to the following equations:
    u=kqe2 (4)
    t1/2=1/(kqe) (5)
    where:
    u initial adsorption rate mg/(g·min)
    t1/2 half-adsorption time min

Table. 3 Comparison of the experiments and the kinetic models of BF adsorption on EG

C0 mg/l

T
ºC

qe,exp
mg/g

First-order

Second-order

qe,cal
mg/g

k1
min-1

r

qe,cal
mg/g

k2
g/(g·min)

r

100

5

104.36

47.17±1.20

0.0096±0.001

0.903

105.60±0.254

9.47±0.023

1.000

25

85.37

47.31±1.20

0.0210±0.002

0.938

88.50±0.872

11.3±0.111

1.000

45

73.65

32.56±1.15

0.020±0.0019

0.956

74.35±0.788

13.43±0.14

0.999

200

5

137.66

62.55±1.18

0.0098±0.001

0.922

139.28±0.550

7.18±0.028

1.000

25

110.36

58.25±1.19

0.022±0.0023

0.942

113.77±1.07

8.79±0.083

1.000

45

98.36

42.30±1.13

0.0168±0.002

0.952

97.37±1.18

10.27±0.13

0.999

    The initial adsorption rate is found to increase with the increase in the initial dyes concentration, but the temperature has different influences on initial adsorption rate. To BF, it decreases with the increase in temperature, and the value of ALYO increases with the increasing in temperature. The influence of temperature and concentration on t1/2 is not obvious.
    The second-order rate constants listed in Tab. 3 and Tab. 4 are used to estimate the activation energy of BF and ALYO adsorption on EG using Arrhenius equation:
Lnk=LnA-Ea/(RT) (6)
    where:
    A pre-exponential factor (g·mg-1·min-1)
    Ea activation energy of adsorption (kJ/mol)

    The slope of plot of ln k versus 1/T is used to evaluate Ea, which was found to be 6.486.62 kJ/mol for BF adsorption on EG (listed in Table.5), and the value of Ea for ALYO adsorption on EG was ignored for the reason of veracity (with the correlation coefficients less than 0.9000). These values are smaller than that in the literature where the activation energy was found to be 16.3-43.8 kJ / mol for the adsorption of BBF on xerogel [16]. The results might be caused by the different porous characteristics of EG and xerogel, and it could also be testified from the different adsorption equilibrium time of 4.0 h on EG and 144.0 h on xerogel.

Table. 4 Comparison of the experiments and the kinetic models of ALYO adsorption on EG

C0
mg/l

T
ºC

qe,exp
mg/g

First-order

Second-order

qe,cal
mg/g

k1
min-1

r

qe,cal
mg/g

k2
g/(g·min)

r

100

5

81.32

47.1±1.11

0.0147±0.001

0.970

82.6±0.91

12.1±0.132

0.999

25

82.36

36.5±1.19

0.0152±0.002

0.925

83.1±0.59

12.04±0.09

1.000

45

101.23

33.5±1.21

0.0171±0.002

0.931

101.8±0.3

9.82±0.033

1.000

200

5

98.36

53.4±1.15

0.0177±0.001

0.963

101.4±1.3

9.86±0.128

0.999

25

101.59

26.1±1.33

0.0136±0.003

0.800

100.7±0.4

9.93±0.042

1.000

45

154.36

53.8±1.18

0.0142±0.002

0.924

153.1±1.1

6.53±0.045

1.000

Table. 5 Kinetic parameters for the second-order adsorption model of BF adsorption on EG

C0
mg/l

T
ºC

u
mg/(g·min)

t1/2
min

Ea
kJ/mol

r

100

5

103.6±0.248

1.01±0.002

6.48±0.044

1.000

25

82.35±0.811

1.04±0.01

45

72.96±0.77

0.95±0.04

200

5

136.06±0.537

1.01±0.004

6.62±0.229

0.998

25

107.05±1.00

1.03±0.009

45

99.35±1.21

0.990±0.012

Table. 6 Kinetic parameters for the second-order adsorption model of ALYO adsorption on EG

C0
mg/l

T
ºC

u
mg/(g·min)

t1/2
min

Ea
kJ/mol

r

100

5

80.02±0.876

1.02±0.011

-

-

25

81.67±0.581

1.01±0.007

45

100.63±0.335

1.006±0.003

200

5

95.39±1.24

1.03±0.012

-

-

25

102.48±0.433

0.991±0.004

45

155.59±1.08

0.992±0.007


3.3 Internal diffusion analysis
The adsorption process on a porous adsorbent generally involves three stages: (i) external diffusion; (ii) internal diffusion (or intra-particle diffusion); (iii) actual adsorption [19]. Quantitative treatment of experimental data may reveal the predominant role of a particular step among the three that actually governs the adsorption rate. The adsorption step is usually very fast for the adsorption of organic compounds on porous adsorbents compared to the external or internal diffusion step [20], and it is known that the adsorption equilibrium is reached within several minutes in the absence of internal diffusion [21]. Thus, the long adsorption equilibrium time in experiments (3.0
24.0 h) suggests that the internal diffusion may dominate the overall adsorption kinetics.
    To provide definite information on the rate-limiting step, an internal diffusion model based on Fick's second law is used to test if the internal diffusion step is the rate-limiting step [22]:
q =kidt1/2     (7)
    where:
    kid internal diffusion constant, mg/(g·min1/2)
    According to the internal diffusion model, a plot of q versus t1/2 should give a straight line with a slope kid and an intercept of zero if the adsorption is limited by the internal diffusion process [22]. The relationships between q and t1/2 at different temperature are shown in Fig. 3 and Fig. 4. Initially in all the cases studied, a linear relationship between q versus t1/2 with a zero intercept is found, suggesting that the internal diffusion step dominates the adsorption process before the equilibrium is reached.

                                    (a)                           

                                    (b)
Fig. 3 Plot of q vs. t1/2 in internal diffusion model. Initial BF concentration is (a) 100 mg/l, (b) 200 mg/l; temperature () 5ºC() 25ºC() 45ºC

                                                   (a)           

                                                 (b)

Fig. 4 Plot of q vs. t1/2 in internal diffusion model. Initial ALYO concentration is (a) 100 mg/l, (b) 200 mg/l; temperature () 5ºC() 25ºC() 45ºC

To see this more clearly, two dimensionless variables are defined, x and q:
x=q/qeq=t/t1/2 (8)
equation (8) can be rewritten as the following

x=k'q1/2 (9)
    where:
    k'
dimensionless internal diffusion rate constant
    x dimensionless adsorption amount
    q dimensionless time

    Fig. 5 and Fig. 6 show the plot of
x versus q1/2, which clearly show that all the data follow the same kinetics. This confirms that the adsorption process can be described by a simple internal diffusion model. For the adsorption of reactive dyes by activated carbon [23], the adsorption of methylene blue by perlite [24], and the adsorption of BBF by xerogel [16], internal diffusion were found to be the rate limiting step.
 
Fig. 5 Plot of x vs. q1/2 in internal diffusion model. Concentration refers to the initial   BF concentration
  
Fig. 6
Plot of
x vs. q1/2 in internal diffusion model. Concentration refers to the initial ALYO concentration

4 CONCLUSION
The use of Expanded graphite for the adsorption of organic dyes from aqueous solution have been examined. The results are summarized as follows:
(1) The adsorption kinetics can be well described by the pseudo second-order kinetic model. Initial adsorption rate increases with the increase in initial BF and ALYO concentration. Temperature and initial dyes concentration do not have obvious influence on t1/2.
(2) The equilibrium adsorption amount is found to increase with the increase in initial BF and ALYO concentration. The internal diffusion of BF or ALYO into the EG is the rate-limiting step of the overall adsorption process.
(3) Adsorption of BF on EG holds small adsorbing activation energy; the result might be caused by the macroporous characteristics of EG.

Acknowledgements  This study was supported by Doctor Foundation of Hebei province Education Office (China, No.B2004402) and Doctor Foundation of Hebei University. The authors gratefully acknowledge their support during the study.

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碱性品红与碱性嫩黄O在膨胀石墨上的吸附动力学研究
庞秀言 吕溥 巩菲 任海丽 梁秀华#
(河北大学化学与环境科学学院 保定 071002;#河北省科技工程学校 保定 071002)
摘要 研究了碱性品红与碱性嫩黄O在以50目天然石墨为原料,高锰酸钾为氧化剂,硫酸为插层剂制备的膨胀石墨上的吸附特性。基于准一级、准二级动力学模型研究了两种染料在膨胀石墨上的吸附模型,计算了其吸附速率和吸附活化能;基于Fick第二定律,确定了吸附过程速率控制步骤。研究表明:两种染料在膨胀石墨上的吸附动力学模型为二级;平衡吸附量随染料初始浓度增加而增大;初始吸附速率随初始浓度的升高而增大;碱性品红在膨胀石墨上的吸附活化能较小;吸附过程为内扩散控制。
关键词 膨胀石墨,吸附动力学,速率控制步骤,碱性品红,碱性嫩黄O

 

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