thermo-physical examination: synthesized 2-furano-4(3h)-quinazolinone and open quinazolinone...
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Title: Thermo-physical examination: Synthesized2-furano-4(3H)-quinazolinone and open quinazolinone(diamide) anticancer analogs with sodium dodecyl sulfate
Author: Varun Bhardwaj Poonam Sharma Malleshappa N.Noolvi Harun M. Patel S. Chauhan M.S. Chauhan KundanSharma
PII: S0040-6031(13)00477-2DOI: http://dx.doi.org/doi:10.1016/j.tca.2013.09.013Reference: TCA 76626
To appear in: Thermochimica Acta
Received date: 15-7-2013Revised date: 6-9-2013Accepted date: 10-9-2013
Please cite this article as: V. Bhardwaj, P. Sharma, M.N. Noolvi, H.M.Patel, S. Chauhan, M.S. Chauhan, K. Sharma, Thermo-physical examination:Synthesized 2-furano-4(3H)-quinazolinone and open quinazolinone (diamide)anticancer analogs with sodium dodecyl sulfate, Thermochimica Acta (2013),http://dx.doi.org/10.1016/j.tca.2013.09.013
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Thermo-physical examination: Synthesized 2-furano-4(3H)-quinazolinone and open quinazolinone (diamide) anticancer analogs with sodium dodecyl sulfate
Varun Bhardwaj a, Poonam Sharma a,*, Malleshappa N. Noolvi b, Harun M. Patel c, S. Chauhan d, M.S. Chauhan d, Kundan Sharma d
aDepartment of Biotechnology, Bioinformatics and Pharmacy, Jaypee University of Information Technology, Waknaghat, Solan (Himachal Pradesh) 173234 India. bDepartment of Pharmaceutical Chemistry, Shree Dhanvantary Pharmacy College, Kim, (Surat) Gujarat 394110 India. cDepartment of Pharmaceutical Chemistry, R.C. Patel Institute of Pharmaceutical Education and Research, Shirpur (Dhule) 425405, Maharashtra, India. dDepartment of Chemistry, Himachal Pradesh University, Summer hill, Shimla (Himachal Pradesh) 173005 India.
Corresponding Author (*):
Dr. Poonam Sharma, Tel: +91-1792-239389, Fax: +91-1792-245362
Email: [email protected] , [email protected]
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Abstract
In this study, the solution and self aggregation properties of sodium dodecyl sulfate (SDS) in
presence of synthesized small molecules i.e. 3-(2-chloro benzylideneamine))-2-(furan-2-yl)
quinazoline-4(3H) one (Q1) and N-(2-(p-tolyl carbamoyl) phenyl) furan-2-carboxamide (Q2)
has been determined. The two compounds were earlier screened for anticancer activity from
NCI, USA. In order to investigate the physico-chemical properties, simple and controlled
methods were employed to obtain critical micellar concentration (CMC) values and thermo-
acoustic parameters via conductance, compressibility coefficient (β), apparent molar volume
(φv) and apparent molar adiabatic compressibility (φk) of SDS in the presence of Q1/Q2 at
different temperatures (25, 30, and 35 °C). In addition, the effect of the addition of Q1/Q2 in
SDS solution and to gain information regarding interaction between the molecules, FTIR and
1H NMR spectroscopic analysis was also carried out. The presence of different substitutions
on the molecules affecting SDS behavior has also been discussed.
Keywords: Quinazolinone; Thermodynamic; Spectroscopic analysis
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1. Introduction
Quinazolines, the derivatives of benzo-pyrimidine are the compounds used in the
pharmaceutical industry, in medicine and even in agriculture because of their wide spectrum
of biological activities [1]. The quinazoline skeleton appears in many alkaloids, most
commonly in the form of 4-(3H)-quinazolinone moieties [2]. There is an evidence to suggest
that the introduction of additional heteroatoms into a drug molecule is potentially better for
increased bioactivity along with altering physiochemical properties and factors, such as
solubility and stability [3]. As quinazoline or quinazolinone includes wide range of biological
activities, it can be considered to be a versatile structure. A wide range of literature shows
that quinazoline compounds possess antihistamine [4], antiviral [5], antimicrobial [6], and
antimalarial properties [7]. Quinazoline have demonstrated anticancer and a range of other
central nervous system effects [8-10]. On the other hand, surfactants are amphiphilic
molecules consisting of polar (hydrophilic) and non-polar (hydrophobic) parts. These
molecules are of commercial important because of their amphiphilic structure which is
responsible for causing them to concentrate at interface or to undergo aggregation i.e.
formation of micelle [11]. Thermodynamic behavior of a solid in a liquid plays an important
role in drug design as well as in optimization of production processes. Micrometric and sub
micrometric particles of pharmaceutical and related compounds like hydrophobic enzymes,
anti-inflammatory drugs, anti-cancer drugs, antibiotics and biopolymers can be formed by
employing the SCF-GAS technique, where the application of an anti-solvent decreases the
solubility of a material dissolved in the solution. Surfactants have been of tremendous
scientific importance because of their many promising applications in detergents, cosmetics,
material fabrication, and drug delivery, among other areas [12]. The degree of solubilization
and the site occupied by the solubilizate depend upon the structural and chemical nature of
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both the surfactant and the solubilizate as well as the concentration of the species in solution
and the temperature. The presence of the solubilizate can affect the process of micellization
and affects the thermodynamics of the micellization via interactions [13]. Two newly
synthesized molecules have been considered in this study as shown below and denoted as Q1
and Q2.
The choice of these two compounds is based on our previous study where the compounds
were synthesized rationally targeting EGFR tyrosine kinase (TKs) and were screened for
anticancer activity at National Cancer Institute (NCI), USA at a single high dose (10-5 M) in
full NCI 60 cell panel and five dose assay [14]. However, quinazoline is an important moiety
in drug industry, the activity in addition to different substitutions of these molecules attracted
us to study their behavior in hydro-ethanolic mixture i.e. 43.36 weight (%) ethanol + water
mixture. With this profile of ring system we intended to investigate their effect on SDS
properties. In this context, the present paper describes the structural effect, micellar study and
thermodynamic parameters. Spectroscopic study was also taken into account to provide
insight on the interactions and locus of the molecules within the surfactant micelle. In
continuation of our study on pharmaceutical active molecules [15-17] and their interaction
with surfactants, here we report the impact of Q1 and Q2 on SDS physicochemical properties.
The similar kind of literature reveals the importance and application of physicochemical
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parameters/evaluation in pharmaceutical and food science [18-24]. This study therefore will
provide the hint of designing new molecules as bioactive compounds via kind of interactions
occurring with sulpho, chloro and amide substitutions on specific ring system.
2. Experimental
2.1. Material
Sodium dodecyl sulfate (SDS) of AR grade and purity > 99% and ethanol absolute (purity
≥ 99.9 %) was obtained from Merck Chemicals (Germany). Freshly prepared doubly distilled
water was utilized, prepared from double distillation unit (HARCO & Co.) whose specific
conductance and pH is in the range ≈ (1-4) × 10-7 S cm-1 and 6.5-7.0 at 25 °C respectively.
Compounds namely, 3-(2-chloro benzylideneamine))-2-(furan-2-yl) quinazoline-4(3H) one
(Q1) and N-(2-(p-tolyl carbamoyl) phenyl) furan-2-carboxamide (Q2) were synthesized
according to the procedure given in our earlier finding. The HPLC purity % area of Q1 and
Q2 were found 96.35 and 94.17, respectively. The structural characterization was carried out
using FTIR, NMR and Mass spectroscopy as given below [14].
Q1: Melting point 201-204 °C; IR (KBr) �max 2920, 1650, 1488, 1399, 554 cm-1; 1H NMR
(DMSO-d6) δ ppm: 7.09 (t, 1H, J = 4.0 Hz, furan-H), 7.50-8.25 (m, 10H, Ar-H and furan-H),
8.79 (s, 1H, N=CH); 13C NMR (DMSO-d6) δ ppm: 169.1, 160.4, 144.2, 142.3, 141.8, 140.3,
134.6, 132.2, 132.1, 131.4, 130.4, 127.4, 127.1, 125.6, 125.9, 120.3, 108.8, 108.9; HRMS
(EI) m/z calcd for C19H12ClN3O2: 349.0618; found:349.0622.
Q2: Melting point 188-189 °C; IR (KBr) �max 3350, 2913, 1676, 1624,1606, 1505, 1453,
1328,1140 cm-1; 1H NMR (DMSO-d6) δ ppm: 3.43 (s, 2H, NH2), 7.68 (d, 1H, J = 8.0 Hz, Ar-
H), 6.57-7.98 (m, 10H, Ar-H and furan-H) 10.53 (s,1H,-NHCO-), 11.71(s,1H,-CONH-); 13C
NMR (DMSO-d6) δ ppm; 168.5, 163.7, 146.7, 142.8, 141.4, 136.4, 135.5, 130.2, 128.7,
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127.6, 124.4, 122.3, 118.6, 116.3, 114.4, 112.3; HRMS (EI) m/z calcd for C18H15N3O5S:
385.0732; found: 385.0735.
2.2. Apparatus and methods
Specific conductance (κ) was obtained using Cyber Scan CON-510 and the conductivity cell
was calibrated with 0.01 mol dm-3 KCl sample solution supplied by Merck Chemicals. The
uncertainty of the conductivity measurement was estimated to be ± 0.5%. The temperature
was maintained constant at ± 0.1 °C by circulating thermostat through a double walled vessel
containing the solution. The concentration of Q1 and Q2 was fixed i.e. 0.01 and 0.02 mol
Kg-1, respectively. All the density (ρ) and ultrasonic velocity (u) measurements has been
executed in a digital high precision instrument, DSA- Anton Paar Digital 5000 with range of
temperatures from 25-35 °C at an interval of 5 °C. All the samples were prepared 24 hours in
advance to settle the time dependent effect. The reproducibility of ultrasonic sound velocity
and density has been ± 0.2 ms-1 and ± 2 × 10-6 gcm-3 respectively over the entire
concentration and temperature range of measurements. Density and sound velocity data was
further utilized to calculate various parameters such as the compressibility coefficient (β),
apparent molar volume (φv) and apparent molar adiabatic compressibility (φk). FTIR and
proton-NMR spectra of the compounds were recorded to analyze interaction and location of
Q1 and Q2 within micelle. FTIR spectra were recorded at a frequency range of 4000-400
cm-1 with match pair of quartz cells using Shimadzu Infra Red Spectrometer, (model FTIR-
8400S). Proton-NMR was recorded with Bruker Avance-II 400 NMR spectrometer operating
at 400 MHz. The chemical shifts were considered and measurement of various resonant peaks
with respect to internal standard TMS are given on the δ scale in parts per million (ppm).
3. Result and Discussion
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3.1. Conductance study:
The micellization behaviour of SDS has been traced in presence of Q1 and Q2 in hydro-
alcoholic solution i.e. 43.36 weight (%) ethanol + water mixture. The choice of short chain
alcohol was based on its nature of getting solubilized in aqueous phase and affecting the
process of micelle formation by modifying the solvent properties. Fig. 1 represents the
conductivity plot as a function of SDS concentration at three different temperatures at 5 °C
interval. The intersection point of the two straight lines represents the usual critical micellar
concentration (CMC). The effect of increasing temperature and SDS concentration has also
been observed. It is remarkable to note that in presence of Q1 and Q2, CMC is less than to
SDS’s region of micellization i.e. 8 mmol Kg-1 [25]. From the obtained values of CMC in
presence of Q1 and Q2, it is clear that Q2 produces a stronger reduction effect on micelle
formation of SDS than Q1. This decrease in the CMC value, mainly attributed to the
interactions between the synthetic molecule and amphiphilic moiety i.e. SDS and is
characteristic of amphiphiles of opposite charges. The CMC values of surfactant increases
with temperature and presence of amino and diamide groups in Q2 contributes eminently for
better interaction and therefore causing shift in micellization to much earlier. The Xcmc data
reported in Table 1 was further utilized to calculate various thermodynamic parameters. The
standard enthalpy, entropy and Gibbs free energy of micellization (ΔH°m, ΔS°
m and ΔG°m)
were calculated by using following equations [26].
ΔH°m = - RT 2 (2-α) [d ln(Xcmc)/dT ]
ΔS°m = (ΔH°
m - ΔG°m)/T
ΔG°m = R T (2-α) (ln Xcmc)
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In the given equations, α denotes the degree of ionization of surfactant which was obtained
using relation, α = S2/S1, S1 and S2 are the slopes in the pre micellar and post micellar region
and d ln (Xcmc)/dT is the slope of the straight line obtained by plotting ln Xcmc against
temperature. All the values of ΔG°m and ΔH°
m were found to be negative revealing
exothermic behavior of the surfactant whereas ΔS°m were positive indicating that
micellization is entropically controlled. The values of ΔG°m with Q1 were found less negative
which might be because of steric hindrance of micelle formation as shown in Table 1 and Fig.
2. The ΔH°m values do not vary significantly with increase in temperature. Here, it can be
understood by assuming that London dispersion interactions represent the main attractive
force for micelle formation [27]. Therefore it is suggested that micellization is facilitated by
the presence of Q1 and Q2 with respect to solvent composition used and temperature as well.
Moreover, Q2 with higher negative ΔG°m values is solubilized to greater extent and has
tendency to transfer from dispersed to the micellar phase.
3.2. Volumetric and compressibility study:
The density (ρ) in addition to sound velocity (u) was obtained which provides information
regarding different interactions with respect to behavior of Q1 and Q2 in hydroalcoholic
solution. The study was performed at 25, 30 and 35 °C in water-ethanol composition [43.36
weight (%)] containing fixed concentration of Q1 (0.01 mol Kg-1) and Q2 (0.02 mol Kg-1) as
reported in Table 2. The increase in temperature favors the increase of kinetic energy and
volume expansion resulting in decrease of density, moreover suggests that thermal energy is
greater than the interaction energy at higher temperatures. The density and speed of sound
data is reported in Table 2 and was further utilized for calculating apparent molar volume (φv)
and apparent molar adiabatic compressibility (φk) using relation [28] as:
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φv = (do-d)/mddo + M/d
φk = (β-βo)/mdo + φv β
Where, m is the molality of the solution, M is the molecular mass of SDS (288.38 gmol-1), d
(kgm-3) is the density of the solution, do is the density of the pure solvent system. Similarly, β
and βo denotes respectively for adiabatic compressibility coefficient of the solution and
solvent. The values for β were calculated using β= 1/dv2. Both properties are highly sensitive
to the extrinsic experimental conditions and therefore are suggested to be relevant to extract
information, especially with regard to the existence of solute-solute and solute-solvent
intermolecular interactions [29]. All the values of φv were found positive in prepared
composition at all temperatures as reported in Table 3. Fig. 3 and Fig. 4 describe the behavior
of φv in presence of Q1 and Q2. Errors in φv and φk values were calculated and found to lay in
the range ± 0.4 m3mol-1 and ± 0.1 m3mol-1TPa-1 respectively. It was observed that at initial
SDS concentration ionic interactions dominate which decreases as concentration of SDS
molecules increases within the environment, whereas at higher SDS concentration
hydrophobic-hydrophobic interactions become more dominant among the molecules leading
to micellization of SDS. Hence, making - breaking of structure strengthen the hydrophobicity
of SDS molecules and facilitates the process of micelle formation. It is clear from the
conductance study that Q2 produces a stronger effect on SDS properties which might be
because of the presence of -NH2- or the diamide in its structure. Moreover, the presence of
carbonyl group which has the active oxygen atom with capability of accepting or donating
electron according to the envionmental condition. These pharmacophore probably
contributing more efficiently in association to SDS and moreover affecting the
physcicochemical behavior of SDS. The anomalous behavior is also suggestive of association
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of some kind of hydrophobic clustering of alcohol molecules. The φk versus SDS
concentration illustrates the same pattern as that of φv, thus supporting each other.
3.3. FTIR and 1H-NMR analysis:
To get more insight on the structure and intermolecular interaction occurring due to the
presence of different function groups on SDS and Q1/Q2, the system is characterized by
Fourier Transform infrared spectroscopy (FTIR) [30,31]. The existing structural changes are
interpreted in terms of frequency or band shift as presented in Fig. 5 (a,b,c). The methylene
anti-symmetric and symmetric vibrations have been clearly observed at 2957 cm-1, 2851 cm-1,
and 2919 cm-1 for alkyl -CH- stretching and 1469 cm-1 for alkyl -CH- deformation,
respectively. The spectrum of SDS depict bands at 1222 cm-1 and 1082 cm-1, signifying -S=O
(stretching) vibrational modes of sulphonic acid group present in SDS. The presence of
Q1/Q2 effect was observed via substantial shifting of bands as presented in Fig. 5(b) and
5(c). The band due to -S=O stretching vibrations in presence of SDS shifted to 1220 cm-1 and
1079 cm-1 in presence of Q1, in addition, -CH- vibrations were observed at 2922 cm-1 , 2958
cm-1 and 2852 cm-1. On the other hand in presence of Q2, -S=O stretching vibrations shifted
to 1224 cm-1 and 1077 cm-1 moreover -CH- vibrations were obtained at 2929 cm-1 , 2959 cm-1
and 2855 cm-1. The kind of shifting clearly depicts that the environment is tightly packed and
indicating that Q2 molecule is more interactive and bounding more efficiently than Q1.
To obtain more understanding into the interaction between the moieties and the locus
of Q1/Q2, proton nuclear magnetic resonance [32] of the SDS system both in the absence and
presence of Q1/Q2 were recorded. Due to the precision of the NMR spectrometer, a change
of ~ 0.01 ppm or greater is considered a significant change. The 1H NMR spectrum of SDS
and SDS in presence of Q1/Q2 is presented in Fig. 6 (a,b,c). The intense resonances at ~ 3.83
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ppm and ~ 1.57 ppm corresponding to α -CH2- and β -CH2- as shown in structure of SDS.
However, moving toward hydrophobic part of SDS, the resonance at ~ 1.25 ppm and ~ 0.87
ppm with integral of 18 protons and 3 protons correspond to bulkier chain -(CH2)9- of SDS
and -CH3- group, respectively (SDS structure shown in figure below).
The chemical shift was observed with the addition of Q1/Q2 in SDS, particularly, α -CH2-, β
-CH2- and -(CH2)9- segments of SDS. The α -CH2- showed upfield movement with a shift of
~ 0.123 ppm. The β -CH2- and -(CH2)9- segments of SDS showed downfield movement of
~ 0.012 ppm and ~ 0.015 ppm, respectively (Fig. 6 b). This might be because of the presence
of electronegative group present in Q1 causing deshielding. The upfield movement of
α -CH2- is due to preliminary interaction of SDS molecule and exposed hydrophobic part of
Q1. On the other hand, the shifts were noticed at higher side in presence of Q2. The upfield
movement of ~ 0.213 ppm was observed for α -CH2- whereas β -CH2- and bulkier segments
of SDS showed movement of ~ 0.013 ppm and ~ 0.028 ppm, respectively as shown in Fig. 6
(c). Interestingly, the resonance of -CH3- protons were observed with ~ 0.014 ppm shift in
presence of Q2 which was absent in case of Q1. This clearly reveals the penetration of Q2
toward the core of micelle in comparison to Q1 which lies at interface or outer surface of the
micelle. This might also be possible that carbonyl group or sulfonic part interacts with
surfactant chain segment and significantly leading to deeper penetration of Q2 toward
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micellar core. A hypothetical model representing interaction of Q1 and Q2 at site is presented
in Fig. 7.
4. Conclusion
Conclusively, the dependence of micelle formation of SDS in presence of Q1/Q2 with respect
to temperature and solvent composition is observed. Decrease in CMC in presence of Q2 is
because of the dilution of micellar surface charges which leads to faster aggregation of
surfactant molecules into micelles. From thermodynamic study, the values of ΔG°m suggested
that the process of micellization is spontaneous which was confirmed by negative values of
ΔH°m. The values of ΔS°
m indicate that micelle formation in this studied system is
entropically controlled. The variation of φv and φk values provided valuable information
regarding the structural rearrangement of the constituent molecules i.e. Q1/Q2 and surfactant
thereby indicating electrostatic and hydrophobic interactions as the main driving forces
involved in formation of micelles. The FTIR and 1H NMR spectral study observations
confirm the interaction between SDS and Q1/Q2 molecule leading to packing of Q1 or Q2
molecule within the micelle. All the studies were found in support of each other with respect
to the concentration range of micellization region.
Acknowledgement
Among authors V. Bhardwaj and P. Sharma are thankful to SAIF department, Panjab
University Chandigarh for providing FTIR and NMR study reports.
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Figure Captions
Fig. 1. Specific conductivity plot of SDS at different temperatures containing Q2 in 43.36
weight (%) ethanol + water mixture.
Fig. 2. The variation of ΔG°m, ΔH°
m and ΔS°m with regard to Q1 and Q2 at different
temperatures.
Fig. 3. Apparent molar volume (φv) versus SDS 43.36 weight (%) ethanol + water mixture
containing Q1 at different temperatures.
Fig. 4. Apparent molar volume (φv) versus SDS in 43.36 weight (%) ethanol + water mixture
containing Q2 at different temperatures.
Fig. 5. FTIR spectrum representing (a) SDS, (b) SDS in presence of Q1 and (c) SDS in presence of Q2.
Fig. 6. NMR spectrum of (a) SDS, (b) SDS in presence of Q1 and (c) SDS in presence of Q2.
Fig. 7. Hypothetical model representing the location of Q1 and Q2.
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List of Tables
Table 1 CMC, Xcmc, α, ΔH°m, ΔG°
m, and ΔS°m values of SDS in 43.36 weight (%) ethanol +
water mixture at 25, 30 and 35 °C containing Q1 and Q2 at three different temperatures.
Table 2 Density (ρ) (kgm-3), ultrasonic velocity (u) (ms-1) and compressibility coefficient (β)
(TPa-1) of SDS (0.002-0.014 mol kg-1) in 43.36 weight (%) ethanol + water mixture at 25, 30
and 35 °C.
Table 3 Apparent molar volume (φv) (m3mol-1), and apparent molar compressibility (φk)
(m3mol-1TPa-1) of SDS in 43.36 weight (%) ethanol + water mixture at 25, 30 and 35 °C.
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Table 1 CMC, Xcmc, α, ΔH°m, ΔG°
m, and ΔS°m values of SDS in 43.36 weight (%) ethanol +
water mixture at 25, 30 and 35 °C containing Q1 and Q2 at three different temperatures.
Compounds T °C CMC (103)
Xcmc (103) α ΔH°
m (kJ mol-1)
ΔG°m
(kJ mol-1) ΔS°
m (J mol-1 K-1)
25 7.4 9.9 0.61 -7.77 -15.86 27.14
30 7.6 10.1 0.64 -7.92 -15.85 26.18
35 7.9 10.5 0.66 -8.04 -15.64 24.65
25 5.8 7.7 0.51 -8.37 -18.00 32.32
30 6.1 8.1 0.52 -8.58 -17.88 30.71
35 6.4 8.6 0.54 -8.73 -17.75 29.28
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Table 2 Density (ρ) (kgm-3), ultrasonic velocity (u) (ms-1) and compressibility coefficient (β)
(TPa-1) of SDS (0.002-0.014 mol kg-1) in 43.36 weight (%) ethanol + water mixture at 25, 30
and 35 °C.
Q1 (0.01 mol Kg-1) Q2 (0.02 mol Kg-1) [SDS] mol Kg-1 25 °C 30 °C 35 °C 25 °C 30 °C 35 °C ρ (kgm-3)
0.002 873.293 862.642 859.094 842.935 838.932 829.502 0.004 873.183 862.864 859.392 843.420 838.975 829.483 0.006 874.464 863.752 859.889 843.494 838.892 829.290 0.008 874.321 863.621 859.878 843.074 838.754 829.234 0.010 874.102 863.498 859.724 842.281 838.201 829.134 0.012 874.092 863.435 859.489 841.821 838.189 829.178 0.014 874.001 863.378 859.302 841.835 838.105 829.134
u (ms-1) 0.002 1422.34 1411.13 1389.54 1382.67 1375.43 1370.89 0.004 1421.56 1410.38 1388.84 1382.23 1375.38 1370.81 0.006 1419.43 1409.89 1387.43 1382.02 1375.21 1370.72 0.008 1418.55 1409.01 1386.45 1381.93 1375.18 1370.67 0.010 1416.06 1408.34 1385.32 1381.84 1375.11 1370.60 0.012 1415.63 1407.34 1384.98 1381.88 1375.02 1370.53 0.014 1415.39 1406.45 1384.09 1381.82 1375.00 1370.46
β (TPa-1) × 10-10 0.002 5.660 5.822 6.029 6.205 6.301 6.415 0.004 5.667 5.826 6.033 6.206 6.300 6.416 0.006 5.676 5.824 6.041 6.207 6.303 6.418 0.008 5.684 5.832 6.049 6.211 6.304 6.419 0.010 5.705 5.838 6.061 6.217 6.309 6.420 0.012 5.709 5.847 6.066 6.220 6.310 6.421 0.014 5.711 5.855 6.075 6.221 6.311 6.422
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Table 3 Apparent molar volume (φv) (m3mol-1), and apparent molar compressibility (φk)
(m3mol-1TPa-1) of SDS in 43.36 weight (%) ethanol + water mixture at 25, 30 and 35 °C.
Q1 (0.01 mol Kg-1) Q2 (0.02 mol Kg-1) [SDS] mol Kg-1 25 °C 30 °C 35 °C 25 °C 30 °C 35 °C
φv (m3mol-1) 0.002 0.00434 0.00347 0.00295 0.00242 0.00198 0.00175 0.004 0.00246 0.00183 0.00154 0.00129 0.00115 0.00105 0.006 0.00149 0.00113 0.00103 0.00099 0.00089 0.00087 0.008 0.00125 0.00095 0.00085 0.00093 0.00078 0.00075 0.010 0.00111 0.00085 0.00077 0.00094 0.00077 0.00068 0.012 0.00099 0.00076 0.00073 0.00091 0.00070 0.00062 0.014 0.00092 0.00071 0.00068 0.00084 0.00066 0.00058
φk (m3mol-1TPa-1) 0.002 2.4565 2.01739 1.77883 1.4983 1.2493 1.1212 0.004 1.39332 1.06327 0.93018 0.8055 0.7232 0.6765 0.006 0.85023 0.65755 0.62067 0.6157 0.5668 0.5555 0.008 0.71111 0.55531 0.51795 0.5752 0.4948 0.4789 0.010 0.63501 0.49326 0.46838 0.5840 0.4892 0.4372 0.012 0.56979 0.44836 0.44061 0.5656 0.4448 0.3981 0.014 0.52752 0.41593 0.41834 0.5224 0.4177 0.3761
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Graphical Abstract
Graphical Abstract (for review)
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Fig. 1.
Figure(s)
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Fig. 2.
Figure(s)
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Fig. 3.
Figure(s)
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Fig. 4.
Figure(s)
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(a)
Figure(s)
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(b)
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(c)
Fig. 5(a,b,c).
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(a)
Figure(s)
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(b)
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(c)
Figure 6(a,b,c).
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Fig. 7.
Figure(s)
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In this study, interaction of two synthesized analogs and SDS has been examined.
Thermo-acoustic parameters were calculated from density and ultrasonic sound velocity data.
Existence of hydrophobic and electrostatic forces was observed.
Spectroscopic study provided the locus of molecules within micellar structure.
*Highlights (for review)