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Jordan Journal of Chemistry Vol. 2 No.2, 2007, pp. 133-144
JJC
Characterization and Thermal Decomposition of Indolylidene Aniline Azo-Dyes Derivatives
Salem A. Hameed*
King Abdulaziz University, Faculty of Science, Chemistry Department
P.O.Box 80203, Jeddah 21589, Saudi Arabia Received on May 31, 2007 Accepted on Sep. 30, 2007
Abstract New heterocyclic azo-dyes derived from aniline derivatives using indolyl aldehyde as a
coupler have been prepared and investigated by elemental analysis, IR,1H-NMR and Uv- vis
spectra furthermore, the spectral properties of the dyes, solvent effect and buffer solution pH
effect have been studied for determination of pKa values (9.62-12.25) for all compounds.
Kinetics of differential scanning calorimetry (DSC) of these compounds were measured. The
activation energy and also critical temperature (Tc), glassy transition temperature (Tg) and
melting point (Tm) temperatures were calculated.
Keywords: Azo-dyes; Spectroscopy; pKa-Value; Differential Scanning Calorimetry
(DSC).
Introduction Azo-dyes are one of the most important and versatile classes of synthetic organic
compounds,with an enormous variety of applications.[1,2] Technological applications of
these dyes result from the combination of the properties of the azo-group and several
types of aromatic-substituted ligands that confer to them intense color over the whole
visible range, thermal and photochemical stability, non-complex synthetic
methodologies and low costs of production. More recently, some of these dyes have
been studied as materials for non-linear optical applications when they contain
substituents on the aromatic rings with push-pull electron ability.[3,4]
Azo-dyes as guests or attached to the polymer chains can undergo photo and
thermal isomerization reactions from the most stable anti-form to the syn. In general,
these reactions produce remarkable changes of the dipole moments of these
molecules leading to photo induced optical birefringency.[5-7] The sequential reversible
isomerization anti-syn-anti leads to the possibility of optical storage, photo induced
switching,[8] formation of surface gratings.[9-11] In the present investigation concerned
with preparation of new dyes, determined ionization constant, solvent effect and kinetic
thermal analysis.
* Corresponding author. E-mail : [email protected].
134
Experimental Materials:
All chemicals used in the synthesis of all dyes were obtained from BDH chemical
company and were used without further purification . The solvents used were
spectroscopic grade .
Apparatus:
The elemental analysis (C,H,N) were carried out on a microanalysis unit of
Perkin Elmer model 2400 and given in table 1.
Table (1): Elemental analysis of azo compounds.
%C %H %N
Calc(found) Calc(found) Calc(found)
Molecular Formula (Mol.Wt.)
m.p oC)(
Comp.
16.86
14.47)(
4.42
4.86)(
72.28
(72.72)
C15H11N3O
(249)
190-195 I
15.85
(15.39)
4.15
4.72)(
67.92
68.95)(
C15H11N3O2
(265)
195-199 II
15.96
15.53)(
4.94
5.07)(
73.00
73.24)(
C16H13N3O
(263)
130-135 III
12.80
12.45)(
3.04
3.99)(
54.89
54.75)(
C15H10N3OBr
(328)
162-163 IV
14.33
13.48)(
3.75
4.22)(
65.52
66.49)(
C16H11N3O3
293)(
190-195 V
The infrared spectra of the dyes were recorded as KBr pellets on a Perkin Elmer
FT-IR spectrophotometer. 1H-NMR spectra of the dyes were recorded on a Brucker 400MHz.
UV/Vis. absorption spectra of the dyes in different solvents and different buffer
solutions at room temperature were recorded using Perkin Elmer Lampda EZ 210
UV/Vis. spectrophotometer.
Differential scanning calorimetry (DSC) curves were obtained using the Mettler
TA3000 DSC apparatus . Samples were heated at 5, 10, 15 and 20 oC / min.
Synthesis of dyes:
NaNO2 (0.025 mol) was slowly added with stirring to distilled water while allowing
the temperature to -5.0oC.[6-8] The solution of indolyl aldehyde was then cooled to -
5.0oC. NaOH (10%) was added drop by drop with stirring, allowing the temperature to -
5.0oC. The reaction mixture was then cooled to-5.0oC, and the diazo component
indolyl-3-aldehde (0.025 mol) was added drop by drop and stirring was continued at
this temperature for 3 h. The clear diazonium salt solution thus obtained was used
immediately in the coupling reaction (see scheme 1). Aniline (0.025 mol), was
dissolved in 20 cm3 of HCl (1:1), then cooled in an ice-bath at a -5.0oC. The diazonium
solution previously prepared was added drop by drop over 1 h with vigorous stirring at
135
-5.0oC. The reaction mixture was stirred for further 3 h at -5.0oC. The product was then
filtered off, washed with water until acid-free, dried at 50.0oC in an oven to give azo
dye .
NH2
X
NaNO2
H2 OH Cl N=N-Cl
X
N
C=O
H
cool
N
C=O
N=N
X
H
H
H
where x = H , p-OH , p-CH3 , p- Br , 0-COOH
Scheme1 Results and discussion
The relevant IR spectra bands that can provide diagnostic structural evidence for
the existence of azo (enol) or hydrazone (keto) tautomers are given in table2. The
data of this table reveals that the coupled moiety (specifically the position of the OH
relative to the azo one ) plays an important rule in detecting which form predominant in
the solid (figure 1).
It is evident from the data of table2 identify the predominant present compounds
in solid state carbonyl and both azo N=N and C-N stretching vibrations are shown,
unfortunately, ν C-N can not be used for diagnostic purpose because of the interference
with ring C=N vibration of the hetero ring moiety. On the other hand, the bands
observed in the range 3500-3000 cm-1 are little use for diagnostic purpose due to the
possible mixing between the chelate hydrogen – bonding vibration with that of the N-H
group[6].
136
Table(2): IR- Spectra of azo compounds. CHAr υ C-N υ N=N υ C=O υ C=C υ
Comp.
3160.5
1134.6
1447.9
1806.6
1614.5
I
3155.1
1134.4
1446.7
1806.6
1625.2
II
3178.6
1131.9
1446.6
1806.7
1615.0
III
3187.6
1277.7
1490.8
1806.7
1603.3
IV
3177.3
1134.1
1446.0
1806.7
1622.0
V
Figure 1: IR spectra of I,II,III,IV and V.
137
The structure of the compounds under study are investigated on the basis of 1H-
NMR spectra (table 3). The data shows two signals at 7.19 and 8.17 ppm which can
assigned to the protons of benzene ring,[10] compounds ( figure 2) , shows signal at
low field ( δ ≈10.5ppm) which can be assigned to the proton of NH or OH, since the
proton signal of the hydrogen bonded NH must appear at low field. This supports the
IR suggestion of the possibility for the structure of these compounds.
Table(3): ¹H-NMR- Spectra of azo compounds.
CH [Ar]δ (ppm)
CHOδ (ppm)
NHδ (ppm)
Comp.
7.19 - 8.17 9.97 11.99 I
7.21 - 8.21 9.98 - 10.06 11.99 II
6.54 - 8.67 9.983 11.99 III
6.55 - 8.20 9.97 - 9.98 11.99 IV
7.21 - 8.21 9.99 11.99 V
Figure 2: 1H-NMR spectra of I .
Electronic absorption spectra:
The electronic absorption spectra of the ethanolic solutions of the compounds
under investigation are studied, λmax (nm) and εmax (dm3 mol-1cm-1) values of the different
bands obtained in various solvents are summarized in table 4. The data indicate that the
138
spectra of the compounds comprise mainly three bands in the Uv-visible regions. The
bands are influence by the nature of the substituted (X) and these are due to excitation
of π-electrons of aromatic ring, one composed of double head band and shoulder, the
maximum of these bands are slightly influenced by changing the solvent polarity. This
behaviour characteristic of such type of electronic transition. For the aryl derivatives the
π–π* band is red shifted compared to other azo compounds this is attributed to a
longitudinal of the π system in aryl and indolyl moieties. The data show that the
observed red shift in the CT shoulder is in a little accordance with the following
sequence which is in harmony with the increase in the solvent polarity : CCl4 < EtOH <
Acetone < DMF. Table (4): Molar extinction coefficient of azo compounds at λ ~300 nm in different
solvents.
E (dm3.mol-1.cm-1)
Acetone CCl4 DMF EtOH
Colour
Comp.
1084.6
251.6
232.7
826.2
Dark brown
I
1034.8
686.6
658.2
1159.3
Orange Light
II
1010.1
667.4
511.6
1230.6
Yellow
III
519.0
712.0
183.8
522.2
Golden
IV
1284.0
608.0
623.4
1212.5
Brown
V
Spectra in buffer solutions:
Generally, the spectra of these compounds in buffer solutions are very similar
and show two or three bands due to the existence of different species as
monocationic, neutral, monoanionic and /or dianionic. The effect of buffer solutions on
the absorption spectra of I as representative (figure 3) are explained, the pk,s are
calculated from absorbance–pH, (figure 4) and discussed , the mean pk,s values are
sited in table 5 .
140
Figure 4: Limiting modified absorption method of I .
From table 5, it is concluded that the difference between the pka values of
compounds I,II,III,IV and V is attributed to the substituent groups in the phenyl ring.
This is mainly due to electron–donating character of the substituted P–OH and P–
COOH groups which increasing the pka values, the pka values decrease as a result of
electron–drawing character from these groups, increasing the electron–donating
character leads to the easier charge–transfer toward the hetero ring.
Table (5): The pKa,s values of the azo compounds obtained by the modified
limiting method.
AAA
−maxmax
pH = pKa+log min
maxAA
AA−
−pH = pKa+log
pka pka
( nm)λ
Com.
11.75 11.10
12.10 11.85
440 595
I
12.15 12.25
12.24 11.88
475 520
II
11.90 11.78
11.75 9.62
480 580
III
11.82 11.98
11.86 11.76
480 580
IV
10.98 11.74
11.42 9.93
480 520
V
141
Thermal analysis: The fraction of crystallized material, calculated using the partial area analysis,
the crystallization activation energy (Ec) were calculated from the differential scanning
calorimetry (DSC) using different methods.
The DSC curves of the investigated compounds were indicated by one
exothermic crystallization peak, Tp (figure 5) corresponding to the crystallization
process, the onset temperature of crystallization,Tc has been defined as a temperature
corresponding to interaction of two linear portions of the DSC trace in the exothermic
direction[12]. The peak temperature of crystallization,Tp is the temperature at which the
overall crystallization rate attains its maximum value, the values of Tc and Tp for the
investigated (I,II) are given in table 6 as a function of heating rates α. The table
reveals that these values are shifted to higher values by increasing the heating rates.
The activation energy of crystallization ,Ec for the investigated compounds has been
estimated using the following methods :
Ozawa- Chen method :
ln (α / T2 ) = _ Ec / RT + const.
Plot of ln (α / T2 ) versus 1/T yields a straight line, then Ec can be evaluated .
Table(6): The Physical constants and activation energy of I and II.
Ec , x102 kcal mol-1
Comp.
heating
rate oC/min.
Tc (0C)
Tg (0C)
Tm (0C)
Ozawa-Chen
method
The Coats- Redferm –
Sestak method
I
5
10
15
20
183
184
185
185
195
196
198
199
199
201
202
208
75.69
73.07
72.54
79.33
3.13
2.77
2.61
2.10
II
5
10
15
20
184
191
192
192
199
200
201
206
204
205
206
206
77.57
76.84
77.57
76.08
2.61
2.54
2.77
1.96
142
Figure 5: DSC curves of I at different heating rates.
Before the second method can be applied to evaluate the activation
energy of crystallization (Ec), the order of the crystallization reaction (n), must
be determined using Ozawa method,[13] the value of n can be determined at
any fixed temperature as the slope of the reaction :
log [_ ln (1 _ x) ] = const. _ n ln α
The plot of log [_ln (1_x)] versus lnα for the investigated compounds at
four different temperatures, the average deduced value of n is equal (1≈2)[14].
The Coats- Redferm – Sestak method :
determines the influence of temperature on the crystallization fraction
(x) for at a particular heating rate in this method the following equation is
used:
ln [_ ln (1 _ x) / T 2n] = _ n Ec / RT + const.
The plot of ln [_ ln (1 _ x) / T 2n] versus 1/ Tof I,II at a heating rate 10oC /min is
shown in figure 6 and the Ec value was determined 2.77x102 and 2.54x102 kcal/mol
respectively.
143
Figure 6: The relation of ln[-ln(1-x)] versus 1/T of I(a) andII(b) at heating rate 10oC/
min.
The straight different in the value of Ec evaluated by different formulations may
be attributed to the different approximations that have been adopted while arriving at
the final equation of the various formalisms. This is due to the fact that the activation
energy in this method has been derived from the variation of the temperature that
scans the whole curves starting from the beginning of the crystallization process till
approximately its ends. Besides, it allows the determination of the dimensionality of
growth and the crystallization mechanism involves in amorphous materials. Table 6
shows the values of the effective activation energies of crystallization Ec calculated by
means of different models.
144
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[2] Rau, H. In Photochemistry and Photophysics; Rabeck, J.F. ed., CRC Press Inc.: Boca Raton, 1990, 2, 119; Rau, H., In Photoreactive Organic Thin Films; Sekkat, Z.; Knoll, W. eds., Academic Press: Amsterdam, 2002, p.3.
[3] Clemlaand, D.S.; Zyss, J. eds . In Nonlinear Optical Properties of Organic Materials and Crystals, Academic Press: New York, 1987.
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