Renewables
Saleh Al Arni1
Alex F. Drake2
Research Article
Marco Del Borghi1
Attilio Converti1
Study of Aromatic Compounds Derived
from Sugarcane Bagasse:
II. Effect of Concentration
1
2
Department of Chemical
and Process Engineering,
University of Genoa,
Via Opera Pia 15,
I – 16145, Genoa, Italy.
Pharmacy, King’s College
London, Franklin-Wilkins
Building, 150 Stamford Street,
London SE1 9NH, UK.
523
The results of a set of experiments that were designed to integrate current knowledge on the major constituents of sugarcane bagasse lignin, specifically p-coumaric, ferulic, syringic acids, and vanillin are presented. These aromatic compounds
have well-known antioxidant power and they are very important for the food,
pharmaceutical, and nutraceutical industries. Following a study on the effect of
pH upon the spectra of these monomers and the determination of their pKa
values, their self-association properties in ethanol as a solvent, particularly at concentrations < 10–4 M were investigated using UV spectrophotometry and their
Kass values were determined. The results collected allowed to better understand
the chemistry of sugarcane lignin and provide a contribution to the possible
exploitation of this abundant straw material for the recovery of fine chemicals.
Keywords: Concentration, Ferulic acid, Lignin, p-Coumaric acid, Renewables,
Self-Association, Sugarcane bagasse, Syringic acid, Vanillin
Received: November 19, 2009; revised: December 22, 2009; accepted: January 5, 2010
DOI: 10.1002/ceat.200900552
1
Introduction
Lignin is a lignocellulosic biomass fraction that combines with
cellulose and hemicellulose. Being a straw organic material
abundant in nature, it could be used as a cheap source of natural chemical compounds, because of its low cost and reduced
impact on the environment. Natural lignin composition is
poorly known, because it is not yet possible to definitively
determine the complete structure of lignin. Since there is no
compound that can be used as a standard for lignin structure,
their measurements are very dependent on the methodology
employed for experiments.
Can we say that lignin is a heterogeneous polymer of phenolic compounds [1] made up of three principal monomers derived from the hydroxycinnamyl alcohol, such as p-coumaryl
alcohol (C9H10O2), coniferyl alcohol (C10H12O3), and sinapyl
alcohol (C11H14O4), whose chemical structure depends on various environmental factors. Lignin has a complex polymeric,
disordered, and random structure, and consists mainly of ether
linked aromatic rings, which add elasticity to the cellulose and
hemicellulose matrices [2]. Some aromatic carboxylic acids,
–
Correspondence: Prof. A. Converti (converti@unige.it), Department of
Chemical and Process Engineering, University of Genoa, Via Opera
Pia 15, I – 16145, Genoa, Italy.
Chem. Eng. Technol. 2010, 33, No. 3, 523–531
mainly p-coumaric acid and ferulic acid, are present in most
lignins in the form of esters [3]. The hydrocarbon compounds
extracted from lignin as well as its structural monomers such
as p-coumaric, ferulic and syringic acids, vanillin, and others
are labeled in the aromatic ring [4].
Recently, new methods have been explored using different
wavelengths and absorptivities on specific biomass samples.
The aromatic compounds under investigation, but vanillin, do
in fact contain a carboxylic acid group whose carbonyl normally absorbs at about 290 nm, although its precise location
depends on the remaining structure of their molecules [5].
The carbonyl group acts as a chromophore primarily on account of the excitation of non-bonding (O) lone pair electrons
to an anti-bonding (C=O) orbital, which gives rise to a n → p*
transition. Typical absorption energies are about 4 eV at
k = 290 nm. The magnitude of the molar extinction coefficient
(e) reflects both the size of the chromophore and the probability that the light of a given wavelength will be absorbed when
it strikes the chromophore. p-Coumaric, ferulic, and syringic
acids all contain a core styrene chromophore. This chromophore has many transitions which are responsible for the UV
absorption spectrum; in isolation, this group is expected to
have a UV maximum at ∼290 nm [5]. However, various substituents such as -CO2H, -OH, and -OCH3 will induce progressive shifts to longer wavelengths. For this reason, the
absorptivity of lignin compounds typically extracted from
sugarcane bagasse has been determined at k between 200 and
450 nm.
© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim
www.cet-journal.com
524
S. Al Arni et al.
Since lignin has received less attention for production of
chemicals compared to polysaccharides and has not yet been
used in any large-scale industrial application for the recovery
of aromatic compounds, there is a great deal in the use of the
lignin fraction of sugarcane bagasse as source of antioxidants
of particular concern to the food, pharmaceutical, and nutraceutical industries.
Sugarcane bagasse was already taken into consideration in a
previous study as a source of lignin compounds and its alkaline solubilization was investigated [6]. Huge amounts of this
agricultural residue from sugar extraction from sugarcane accumulate in the mills, thus creating environmental problems.
Although utilized in the sugar factories as fuel for the boilers
[7], recently, there has been an increasing trend towards alternative utilization. It is in fact a large and inexpensive raw
material that can be used in several biotechnological processes:
as carbohydrate source for the productions of xylitol [8, 9],
ethanol [10], and several different enzymes [11–13], or even as
a support for cell immobilization [14–17].
Following a previous study on the effect of pH upon the
spectra of the main constituents of its lignin fraction, e.g.,
p-coumaric acid, ferulic acid, syringic acid, and vanillin, and
the determination of their pKa values [18], their self-association properties to form dimers were investigated by optical
spectroscopy.
range 180–450 nm. The baseline spectra of the solvent used to
make up the samples were obtained on the same day as the
sample spectra and subtracted from them. After obtaining the
spectra, data were transferred to the standard analysis software,
Grams 32 Al (Galactic Industries Inc., Salem, NH), for baseline
correction and other studies.
Molar extinction coefficients (e, expressed as M–1cm–1) were
determined for wavelengths (k, expressed in nm) over the
whole spectral range. This was done through the Beer-Lambert
law (A = ecl), by dividing the absorbance (A) by the concentration (c) and the cell path length.
Relevant data obtained from spectra at different concentrations at constant wavelength were plotted to obtain self-association curves. The MathCad 8 Professional program was used
to analyze the maximum values (emax) of e versus concentration to obtain the limiting monomer and dimer spectra, as
well as the association constant (Kass) values.
2
Experimental
m+m>d
2.1
Reagents
Setting the total concentration (Ct) equal to the sum of the
molar concentrations of the dimer (Cd) and the monomer
(Cm):
p-Coumaric acid, ferulic acid, syringic acid, and vanillin used
as standard reagents were pure chemicals purchased from Sigma-Aldrich (Steinheim, Germany).
3
Theory of Dimerization
In ethanol as a solvent, the aromatic compounds under investigation self-associate to form dimers at high concentration.
The dimerization equation was derived as follows. In the case
of self-association equilibrium, a monomer can be said to form
a dimer as described by the following equation:
(1)
Ct = Cm + Cd
(2)
the equilibrium constant of dimerization (Kass) is defined as:
2.2
Sample Preparation
Kass = Cd / Cm2
Weighing of samples was carried out using an electronic microbalance, model MT5 (Mettler Toledo, Columbus, OH), and
the use of an ultrasonic bath was necessary to ensure their
complete dissolution.
The preparation of stock solutions was the first step in conducting these experiments. For concentration studies, 1- to
3-mg samples were put into 25 mL tubes, and 96 % (v/v) ethanol was added as a solvent up to the following concentrations:
0.717 mM p-coumaric acid, 0.254 mM ferulic acid, 0.266 mM
syringic acid, and 0.239 mM vanillin. From these solutions, all
dilutions were derived.
2.3
Analytical Techniques
For spectral measurements, rectangular cuvettes of 1.0-cm
path length (l) or cylindrical cuvettes with l = 1.0, 2.0, and
5.0 cm were used in a UV-VIS-IR spectrophotometer, model
17DS (Aviv Associates, Lakewood, NJ). The instrumental
setting was: spectral band width = 1.0 nm, measurement step
size = 0.5 nm, scan speed = 0.2 s. Scans were typically over the
www.cet-journal.com
(3)
Absorbance based on Beer’s law will now be [19]:
Aobs = Am + Ad = (em Cm l) + (ed Cd l)
(4)
and the extinction coefficient:
eobs = (em Cm + ed Cd) / Ct
(5)
Combining Eqs. (2), (3), and (5), and solving the system
gives:
1
eobs Ct
Ct
(
p "
p2 #)
1± 1 4Kass Ct
1± 1 4Kass Ct
em
ed Kass
2Kass
2Kass
(6)
Applying this equation shows that the positive sign before
the square root is the only acceptable solution.
© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim
Chem. Eng. Technol. 2010, 33, No. 3, 523–531
Renewables
In Eq. (6), the dependent variable, eobs, depends upon three
parameters, specifically the limiting values of the extinction
coefficients of both the monomer (em) and dimer (ed), as well
as Kass.
Using the MathCad 8.0 software, plots of the experimental
data of eobs (Ct) against concentration resulted in graphs that
could be simulated by Eq. (6) and fitted with the best values of
ed, em, and Kass.
4
Results and Discussion
525
∼310, 323, and 275 nm for p-CA, FA, and SA, moved at low
concentrations to ∼291, 310, and 262 nm, respectively. On the
contrary, no clear effect was evident for vanillin, for which a
variation in the percentage of conversion of monomer to dimer was observed, when a change in the concentration took
place at a given wavelength. Such shifts indicate that the BeerLambert law was not obeyed. Whereas, the extinction coefficient of p-CA remained relatively constant (≈ 22000 M–1cm–1),
the extinction coefficients from high to low concentrations for
FA and SA decreased from 18600 to 17000 M–1cm–1 and from
10800 to 9600 M–1cm–1, respectively.
As depicted in Fig. 2, all the selected compounds were present as monomeric species at the lowest concentrations and
self-associated at the highest concentrations, dimerization
being the likely result of the monomer in equilibrium with its
dimer. Although, at this stage, the precise molecular nature of
self-associated vanillin in 96 % ethanol is not known, a proposal is presented in Fig. 2D).
Figs. 3–6 show the simulated curves for p-CA, FA and SA,
and vanillin, respectively, referred to wavelengths corresponding either to maximum or to minimum absorption, specifically k = 210, 227, 291, and 310 nm for p-CA; k = 216, 232, and
323 nm for FA; k = 215, 262, and 275 nm for SA; k = 232, 280,
310, and 358 nm for vanillin.
The equilibrium constants, Kass, as well as the other parameters that appear in Eq. (6) were calculated for all the compounds with the help of the MatCad software package that allowed the simulation of the dimerization curves from the
experimental data. Their values are listed in Tab. 1 together
with those of the extinction coefficients of both the monomeric and dimeric species.
As far as the dimerization constants are concerned, although
they were somehow influenced by the wavelength, p-CA, FA,
and SA showed average Kass values of ∼2 · 105, ∼1 · 106, and
∼4 ·105, respectively. On the other hand, that of vanillin
(Kass ∼ 3 · 104) was 1–2 orders of magnitude lower, as the likely
result of the presence of an aldehyde rather than a carboxylic
acid group.
Tab. 2 shows the limiting values of the extinction coefficients
of both monomeric and dimeric vanillin estimated at different
wavelengths. Using these values, a plot of percentage of self-association versus concentration has been drawn up for vanillin
Previous work on the effect of pH on titration curves of aromatic compounds derived from sugarcane bagasse confirmed
the suitability of the titration method to determine the values
of pKa of the selected compounds [18, 20]. In this way, the pKa
values of p-coumaric (p-CA), ferulic (FA) and syringic acids
(SA), and vanillin in two ionization states were determined
and the effect of pH on their molecular structures associated
with the two equilibrium states was shown. Here, the effect of
varying concentrations of these aromatic compounds on their
respective spectral and self-association behavior was investigated. The absorbance spectra obtained at a series of concentrations were investigated in 96 % ethanol as solvent, using
1.0-, 2.0-, and 5.0-cm path length cuvettes.
The self-association properties of the selected aromatic compounds were investigated by UV spectrophotometry, particularly at concentrations < 10–4 M.
Several isosbestic points were observed where the spectra do
not depend on the concentration of the species. In fact, when
an isosbestic point is present at a given wavelength, the two
chemical species have the same molar absorptivity (e) and
then, the system either possesses more than two states, or more
than one complex state has formed. According to Pouët et al.
[21], the presence of isosbestic points also means a quality and
quantity conservation in the global composition of samples,
with given relations between the concentration of absorbing
compounds or mixtures of compounds. Once the spectra of
the self-associated species had been defined, the molecular
structures associated with the two equilibrium states and the
association constants were determined.
Fig. 1 shows the extinction coefficient spectra of p-CA
(graph A), FA (graph B), SA (graph C), and vanillin (graph D)
versus wavelength at different concentrations using only 1.0-cm path
Table 1. Values of the dimerization constant (Kass) at different wavelengths for p-coumaric, ferulic
length cuvettes. The isosbestic
and syringic acids, and vanillin, as well as of the molar extinction coefficients (e) of both the
monomeric and dimeric species.
points were observed in the spectra
of these compounds at the followp-Coumaric acid
Ferulic acid
Syringic acid
Vanillin
ing wavelengths: a) p-CA: 224, 245,
and 290 nm; b) FA: 209, 231, 255,
Kass (ethanol)
1.25 · 105 (210 nm)
1.0 · 106 (216 nm) 3.3 · 105 (215 nm) 2.3 · 104 (232 nm)
and 291 nm; c) SA: 233 and
1.20 · 105 (227 nm)
1.0 · 106 (232 nm) 5.0 · 105 (262 nm) 3.0 · 104 (280 nm)
5
265 nm; d) vanillin: 335 nm. The e
3.50 · 10 (291 nm)
1.0 · 106 (323 nm) 2.5 · 105 (275 nm) 1.6 · 104 (310 nm)
1.85 · 105 (310 nm)
3.7 · 104 (358 nm)
spectra of p-CA either at low or
high concentrations confirm the
e292 = 13450
e261 = 9460
e280 = 10075
Monomer
e286 = 22080
two-state model of monomer in
e219 = 15404
e231 = 12250
e210 = 27800
e358 = 1860
equilibrium with dimer.
Dimer
e311 = 22370
e323 = 18619
e273 = 10723
e310 = 10570
As shown in the same figure, the
e226 = 11540
e233 = 11970
e215 = 27160
e232 = 15470
absorbance maxima, which oce210 = 10490
e215 = 13662
curred at high concentrations at
Chem. Eng. Technol. 2010, 33, No. 3, 523–531
© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim
www.cet-journal.com
526
S. Al Arni et al.
25000
-1
10000
5000
A
0
200
1
225
15000
-1
15000
Extinction coefficient, ε (M .cm )
Conc.1.42E4
Conc.9.45E5
Conc.6.30E5
Conc.4.20E5
Conc.2.80E5
Conc.1.87E5
Conc.1.24E5
Conc.8.30E6
20000
Extinction coefficient (ε)
Conc1.69E4M
Conc1.13E4M
Conc7.53E5M
Conc5.02E5M
Conc3.35E5M
20000
2
10000
5000
3
250
275
B
0
300
325
200
350
250
300
350
Wavelength, λ (nm)
Wavelengths, λ (nm)
30000
16000
Conc1.18E04
Conc7.89E05
Conc5.26E05
Conc3.26E05
-1
15000
10000
5000
0
200
12000
-1
20000
Conc2.39E04
Conc1.59E04
Conc1.06E04
Conc7.08E05
Conc4.72E05
Conc3.15E05
Conc2.10E05
14000
Extinction coeffecient, ε (M .cm )
-1
-1
Extinction coeffecient, ε (M .cm )
25000
C
10000
8000
6000
4000
2000
D
0
220
240
260
280
300
320
200
340
250
300
350
400
Wavelength, λ (nm)
Wavelenghth, λ (nm)
Figure 1. Molar extinction coefficients in 96 % ethanol solution versus wavelength obtained at different concentrations using 1.0-cm path
length cuvettes: A) p-coumaric acid; B) ferulic acid; C) syringic acid; D) vanillin.
Table 2. Limiting values of extinction coefficients of both monomeric (em) and dimeric (ed) vanillin obtained at different wavelengths.
k [nm]
em [M–1cm–1]
ed [M–1cm–1]
232
12000
16100
280
8500
11000
310
9500
11000
358
2700
10
as a function of its concentration in 96 % ethanol at different
wavelengths (Fig. 7).
At about 280 nm, the extent of vanillin self-association
turned out to be greater in comparison with either lower or
higher wavelengths at all the concentrations tested in this
study. Under these conditions, its dimerization constant was
www.cet-journal.com
∼3 · 104, while the maximum values of the molar extinction
coefficients were ∼11 000 and ∼8500 M–1cm–1 for the dimeric
form (high concentrations) and the monomeric form (low
concentrations), respectively.
5
Conclusion
The self-association properties of the main aromatic compounds present in sugarcane bagasse lignin, specifically p-coumaric acid (p-CA), ferulic acid (FA), syringic acid (SA), and
vanillin, have been investigated in ethanol at different concentrations, in particular < 10–4 M. The UV spectra of both monomeric and self-associated species allowed determination of
their association constants (Kass), which turned out to be so
low that special 5.0-cm path length cuvettes were required for
analysis.
© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim
Chem. Eng. Technol. 2010, 33, No. 3, 523–531
Renewables
O
527
OH
H
O
O
Kass
H
HO
O
O
O
H
H
O
O
HO
HO
Monomer
Dimer
Low concentration
High concentration
A) p-Coumaric acid
O
OH
O
H
H3 C
O
O
Kass
H
O
HO
CH3
O
O
O
H
H
O
O
HO
HO
O
H 3C
O
Monomer
Dimer
H 3C
Low concentration
High concentration
B) Ferulic acid
O
O
O
H
H3C
CH3
OH
O
O
HO
H
O
Kass
O
CH3
O
H3C
O
O
O
O
H
H3C
H
H3C
O
O
HO
HO
O
O
H3C
H3C
Monomer
Dimer
Low concentration
High concentration
C) Syringic acid
H
H
O
O
O
O
H3CO
H3CO
+
OCH3
O
OCH3
O
O
H
O
H
D) Vanillin
Figure 2. Molecular structure in 96 % ethanol solution at high and low concentrations of
A) p-coumaric acid; B) ferulic acid; C) syringic acid; D) vanillin.
Chem. Eng. Technol. 2010, 33, No. 3, 523–531
© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim
www.cet-journal.com
528
S. Al Arni et al.
B
Mol. Extin.Coeff.at 227 nm (M-1 cm-1)
Mol. Extin.Coeff.at 210 nm (M-1 cm-1)
A
4
2 .10
4
1.8 .10
4
Ecalc( Ct ) 1.6 .10
Eobs
j
4
1.4 .10
4
1.2 .10
4
1 .10
0
5
4
1.5 .10
4
1.4 .10
4
Ecalc( Ct ) 1.3 .10
Eobs
j
4
1.2 .10
4
1.1 .10
4
1 .10
5
4
4
4
4 .10 8 .10 1.2 .10 1.6 .10 2 .10
Ct , Ctot
j
Concentration (M)
4 .10
0
D
Mol. Extin.Coeff.at 310 nm (M-1 cm-1)
Mol. Extin.Coeff.at 291 nm (M-1 cm-1)
C
4
2.3 .10
4
2.2 .10
4
Ecalc( Ct ) 2.1 .10
j
4
2 .10
4
1.9 .10
4
1.8 .10
0
4 .10
5
4
4
4
8 .10 1.2 .10 1.6 .10 2 .10
Ct , Ctot
j
Concentration (M)
Simulated
Experimental
Simulated
Experimental
Eobs
5
5
5
4
4
4
8 .10 1.2 .10 1.6 .10 2 .10
Ct , Ctot
j
Concentration (M)
4
2.3 .10
4
2.14.10
4
Ecalc( Ct ) 1.98.10
Eobs
j
4
1.82.10
4
1.66.10
4
1.5 .10
0
Simulated
Experimental
4 .10
5
5
4
4
4
8 .10 1.2 .10 1.6 .10 2 .10
Ct , Ctot
j
Concentration (M)
Simulated
Experimental
Figure 3. Molar extinction coefficients of p-coumaric acid in 96 % ethanol solution versus concentration. k (nm): (A) 210, (B) 227,
(C) 291, (D) 310. (×) Experimental values; (line) simulated curves.
The isosbestic points were observed in the spectra of these
compounds at the following wavelengths: a) p-CA: 224, 245,
and 290 nm; b) FA: 209, 231, 255, and 291 nm; c) SA: 233 and
265 nm; d) vanillin: 335 nm.
p-CA exhibited Kass ∼ 2 · 105 and a maximum molar extinction coefficient (emax = 22000 M–1cm–1) at ∼291 nm at low
concentrations (monomer), which shifted to ∼310 nm at
high concentrations (dimer). However, emax appeared to be
almost independent of the concentration. FA exhibited
Kass ∼ 1 · 106, emax ≈ 18600 M–1cm–1 at k ∼ 323 nm as a dimer
and emax ∼ 17000 M–1cm–1 at 318 nm as a monomer. SA
behaved similarly to FA, showing a value of Kass ∼ 4 · 105,
emax ∼ 1800 M–1cm–1 at k ∼ 275 nm as a dimer and
www.cet-journal.com
emax ∼ 9600 M–1cm–1 at k ∼ 262 nm as a monomer. The dimerization constant of vanillin (Kass ∼ 3 · 104) was 1–2 orders
of magnitude lower than those of the other compounds, and
the maximum molar extinction coefficients of its dimeric
and monomeric forms were emax ≈ 11 000 M–1cm–1 and
8500 M–1cm–1, respectively, both at k ∼ 280 nm.
These results allowed us to increase our understanding of
the chemistry of sugarcane lignin and provide a contribution
to the possible exploitation of this abundant straw material for
the recovery of fine chemical products.
© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim
Chem. Eng. Technol. 2010, 33, No. 3, 523–531
Renewables
A
A
4
2.9 .10
4
1.44 .10
Ecalc
Eobs
4
( Ct ) 1.38 .10
j
1.32 .10
4
4
1.26 .10
4
1.2 .10
1 .10
5
3.2 .10
5
5
4
7.4 .10 1.16 .10 1.58 .10
Ct , Ctot
j
Concentraion (M)
4
2 .10
4
Mol. Extin.Coeff.at 215 nm (M-1 cm-1)
Mol. Extin.Coeff.at 216nm (M-1 cm-1)
4
1.5 .10
4
2.82 .10
4
Ecalc ( Ct ) 2.74 .10
Eobs
j
4
2.66 .10
4
2.58 .10
4
2.5 .10
0
4 .10
Simulated
Experimental
Eobs
( Ct ) 1.18
.10 4
j
.10 4
1.12
1.06
.10 4
4
1 .10
1 .10
5
3.2 .10
5
5
7.4 .10 1.16
Ct , Ctot
4
.10 1.58
.10
4
2 .10
4
Eobs
j
7600
5
4 .10
0
4
1.48 .10
4
1.34 .10
3.2 .10
5
5
4
7.4 .10 1.16 .10 1.58 .10
Ct , Ctot
j
Concentraion (M)
4
2 .10
4
1.02
Ecalc
Eobs
( Ct )
j
.10 4
9400
8600
7800
7000
0
Simulated
Experimental
Figure 4. Molar extinction coefficients of ferulic acid in 96 % ethanol solution versus concentration. k (nm): (A) 216, (B) 232,
(C) 323. (×) Experimental values; (line) simulated curves.
C
4
1.1 .10
(M-1 cm-1)
4
( Ct ) 1.62 .10
5
5
4
4
4
8 .10
1.2 .10
1.6 .10
2 .10
Ct , Ctot
j
Concentration (M)
Simulated
Experimental
Mol. Extin.Coeff.at 275nm
Mol. Extin.Coeff.at 323 nm (M-1 cm-1)
4
8200
7000
4
1.76 .10
4
1.2 .10
1 .10
2 .10
8800
Ecalc ( Ct )
C
4
1.9 .10
j
4
9400
Simulated
Experimental
Eobs
4
1.6 .10
4
1 .10
j
Concentration (M)
Ecalc
5
8 .10
1.2 .10
Ct , Ctot
j
Concentration (M)
B
4
Mol. Extin.Coeff.at 262 nm (M-1 cm-1)
Mol. Extin.Coeff.at 232 nm (M-1 cm-1)
Ecalc
.10
5
Simulated
Experimental
B
4
1.3 .10
1.24
529
4 .10
5
5
8 .10
1.2 .10
Ct , Ctot
j
Concentration (M)
4
1.6 .10
4
2 .10
4
Simulated
Experimental
Figure 5. Molar extinction coefficients of syringic acid in 96 %
ethanol solution versus concentration. k (nm): (A) 215, (B) 262,
(C) 275. (×) Experimental values; (line) simulated curves.
Acknowledgements
References
The authors thank the Italian Ministry of Education, University and Research (MIUR), and the University of Genoa for the
PhD fellowship of Dr. S. Al Arni.
[1] E. N. Aquino-Bolaños, E. Mercado-Silva, Postharvest Biol.
Technol. 2004, 33 (3), 275. DOI: 10.1016/j.postharvbio.
2004.03.009
[2] M. Paster, Industrial bioproduct: Today and tomorrow, U. S.
Department of Energy, Office of Energy Efficiency and Renewable Energy, Office of the Biomass Program, Washington,
D.C. 2003, online: http://www.bioproducts-bioenergy.gov/
Chem. Eng. Technol. 2010, 33, No. 3, 523–531
© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim
www.cet-journal.com
530
S. Al Arni et al.
B
A
4
1.1 .10
Ecalc ( Ct )
Eobs
j
1.4 .10
4
1.3 .10
4
1.2 .10
4
1.1 .10
4
1 .10
4
Mol. Extin.Coeff.at 280 nm (M-1 cm-1)
Mol. Extin.Coeff.at 232 nm (M-1 cm-1)
4
1.5 .10
0
4 .10
5
8980
6960
Ecalc ( Ct )
Eobs
j
4940
2920
900
5
4
4
8 .10 1.2 .10 1.6 .10 2 .10
Ct , Ctot
j
Concentraion (M)
0
4 .10
Simulated
Experimental
C
D
Mol. Extin.Coeff.at 358 nm (M-1 cm-1)
Mol. Extin.Coeff.at 310 nm (M-1 cm-1)
1800
4
1.06 .10
4
Ecalc ( Ct ) 1.02 .10
j
5
4
4
4
8 .10 1.2 .10 1.6 .10 2 .10
Ct , Ctot
j
Concentraion (M)
Simulated
Experimental
4
1.1 .10
Eobs
5
9800
9400
9000
0
4 .10
1560
Ecalc ( Ct ) 1320
Eobs
j
1080
840
600
5
5
4
4
8 .10 1.2 .10 1.6 .10 2 .10
Ct , Ctot
j
Concentraion (M)
0
4 .10
5
5
4
4 . 4
8 .10
1.2 .10 1.6 .10
2 10
Ct , Ctot
j
Concentraion (M)
Simulated
Experimental
Simulated
Experimental
Figure 6. Fitting of the self-association spectral data of vanillin to a two-component dimer model. k (nm): (A) 232, (B) 280, (C) 310,
(D) 358. (×) Experimental values; (line) simulated curves.
100
90
80
Percentage
70
60
Vanillin
50
percent232
percent280
percent310
percent358
40
30
20
10
0
0,00004
0,00008
0,00012
0,00016
0,00020
0,00024
Concentration (M)
Figure 7. Percentage of conversion of monomeric to dimeric vanillin as a function of the concentration in 96 % ethanol. k (nm): (×) 232,
(䊊) 280, (~) 310, (q) 358.
www.cet-journal.com
© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim
Chem. Eng. Technol. 2010, 33, No. 3, 523–531
Renewables
[3]
[4]
[5]
[6]
[7]
[8]
[9]
[10]
[11]
pdfs/bioproductsopportunitiesreprotfinal.pdf (accessed June,
2005).
R. D. Hartley, J. Sci. Food Agric. 1972, 23 (11), 1347. DOI:
10.1002/jsfa.2740231110
R. Ji et al., Chemosphere 2005, 60 (9), 1169. DOI: 10.1016/
j.chemosphere.2005.02.014
P. W. Atkins, Physical Chemistry, 5th ed., Oxford University
Press, Oxford 1994.
S. Al Arni, M. Zilli, A. Converti, Cienc. Tecnol. Aliment. 2007,
5 (4), 271.
J. Zandersons et al., Biomass Bioenerg. 1999, 17 (3), 209.
DOI: 10.1016/S0961-9534 (99)00042-2
W. Carvalho, S. S. Silva, A. Converti, M. Vitolo, Biotechnol.
Bioeng. 2002, 79 (2), 165. DOI: 10.1002/bit.10319
A. A. Cunha et al., Appl. Biochem. Biotechnol. 2009, 157 (3),
527. DOI: 10.1007/s12010-008-8301-5
B. F. Sarrouh, S. S. Silva, D. T. Santos, A. Converti, Chem.
Eng. Technol. 2007, 30 (2), 270. DOI: 10.1002/ceat.200600271
S. Mathew, T. E. Abraham, Enzyme Microb. Technol. 2005, 36
(4), 565. DOI: 10.1016/j.enzmictec.2004.12.003
Chem. Eng. Technol. 2010, 33, No. 3, 523–531
531
[12] J. C. Meza et al., Process Biochem. 2005, 40 (10), 3365. DOI:
10.1016/j.procbio.2005.03.004
[13] M. Mazutti, J. P. Bender, H. Treichel, M. Di Luccio, Enzyme
Microb. Technol. 2006, 39 (1), 56. DOI: 10.1002/jctb.2273
[14] A. Pandey, C. R. Soccol, P. Nigam, V. T. Soccol, Bioresour.
Technol. 2000, 74 (1), 69. DOI: 10.1016/S0960-8524(99)
00142-X
[15] L. Sene, A. Converti, M. G. A. Felipe, M. Zilli, Bioresour.
Technol. 2002, 83 (2), 153. DOI: 10.1016/S0960-8524(01)
00192-4
[16] M. Zilli et al., Biodegradation 2004, 15 (2), 87. DOI: 10.1023/
B:BIOD.0000015613.91044.a4
[17] D. T. Santos et al., J. Food Eng. 2008, 86 (4), 542. DOI:
10.1016/j.jfoodeng.2007.11.004
[18] S. Al Arni, A. F. Drake, M. Del Borghi, A. Converti, Chem.
Eng. Technol., under revision.
[19] S. B. Brown, An Introduction to Spectroscopy for Biochemists,
Academic Press, London 1980.
[20] S. Al Arni, Ph.D. Thesis, University of Genoa, Italy 2008.
[21] M.-F. Pouët, E. Baures, S. Vaillant, O. Thomas, Appl. Spectrosc. 2004, 58 (4), 486. DOI: 10.1366/000370204773580365
© 2010 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim
www.cet-journal.com