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IOSR Journal of Applied Physics (IOSR-JAP)
e-ISSN: 2278-4861.Volume 4, Issue 1 (May. - Jun. 2013), PP 01-04
www.iosrjournals.org
www.iosrjournals.org 1 | Page
Analysis of Transport Properties and Acoustical Parameters of
Sulphanilamide in Non- Aqueous Medium
Santhakumari.S1
, Padmavathy.R2
, JasmineVasantharani.E2
1
Department of Physics,Shrimati Indira Gandhi College,Thiruchirappalli,Tamilnadu.
2
Department of Physics,Seethalakshmi Ramaswamy College,Thiruchirappalli,Tamilnadu.
Abstract; Sulphanilamide is the parent compound of all the sulpha-durgs which is important in urinary tract
infections and meningococcal meningitis profilaxes. Ultrasonic velocity measurements are highly sensitive to
molecular interactions and used to provide qualitative informations about the physical nature and strength of
the molecular ∕inter-ionic interactions. In the present work, non-aqueous solutions of Sulphanilamide have
been prepared with different concentrations and the experiments were carried out from a low temperature of 50
c
to a high temperature of 550
c. The ultrasonic velocity data combined with density and viscosity provides the
standard means for determining the internal pressure, free volume and acoustical parameters. The various
interactions occurring in the solutions are interpreted interms of ion-ion and ion-solvent interactions. An
attempt is made to identify the entry of solvate into the samples and the entry of drug molecules into the solvate
which supports to identify the molecular structure.
Keywords : Acoustical parameters, free volume, Internal pressure, ion-solvent interactions ,ion-ion
interactions.
I. Introduction
Sulphanilamide compounds identified as chemotherapeutic agents, possess broad spectrum of
biological properties [1].Study of non –aqueous solutions is interesting for the physical understanding of the
ion –solvent interactions. The passage of ultrasonic waves through solutions and liquids disturb the equilibrium
between solute and solvent molecules. The velocity of such a wave is a thermodynamic quantity and is related to
the physio – chemical properties of the medium[2].The velocity of ultrasonic waves in a medium and several
other acoustic parameters which are dependent on it, helps to determine the overall response of the medium and
about the nature of interactions between the molecules of the medium[3,4].Ultrasonic velocity of a
liquid/solution is fundamentally related to the binding forces between the adequately employed in
understanding the nature of molecular interaction in pure liquids[5,6,7].
The present work dealt with the ultrasonic investigations and acoustical study of (sulfanilamide)
sulphanilamide in formamide .
II. Experimental Technique
The solutions of different molalities of sulphanilamide are prepared with AR grade formamide.Density
of the solution is measured with 25ml of specific gravity bottle by a Digital balance of accuracy of .0001gm/cc.
Cannonfenske viscometer is used for the viscosity measurements, and the time is noted by stop watch with an
accuracy of ± 0.1sec. Mittal’s interferometer of frequency to 2MHz, with an accuracy of ± 2 m/s is used.
. Internal pressure (πi) and free volume (vf) and acoustical parameters are evaluated by the following formulae.
(i) Internal pressure (πi) = bRT [kη/u]1/2
ρ2/3
/M7/6
atms
(ii) Free volume (vf) = [ Meff u/kη]3/2
cc
(iii) Adiabatic compressibility (β) = [1/u2
ρ] cm2
/dynes
(iv) Specific acoustic impedance (Z) = ρu (Rayl)
(v) Intermolecular free length (Lf) = KT (βad
1/2
)A0
III . Results and Discussion
In the present study internal pressure, exhibits an increasing trend with respect to increasing molalities
as shown in fig (1).Internal pressure is a measure of cohesive energy of the system hence these variations may
be due to the structure making nature of the solute in the solvent . It implies that there is a strong solute- solvent
interaction taking place in the solution[8].The dependence of parameter on temperature has also been used to
explain the strength of interactions with change in temperatures[9,10].The internal pressure decreases with rise
in temperature of the solution. Since when the temperature is increased, there is a tendency for the ions to move
for away from other ,reducing the possibility of interaction, which may further reduce the cohesive forces and
Analysis Of Transport Properties And Acoustical Parameters Of Sulphanilamide In Non- Aqueous
www.iosrjournals.org 2 | Page
ultimately leads to a decrease in internal pressure[11].The variations of Vf with molalities as shown in fig (2)
also confirm the structure making nature of the solute in the solvent.
The adiabatic compressibility increases with decrease in molality and rise in temperature [12]as shown
in fig (3). When the salt is added to the solvent ,the compressibility is lowered. This lowering is attributed to the
influence of the electrostatic field of the ions on the surrounding solvent molecules. such a decrease may be due
to (i) an increase in the number of incompressible molecule[13,14,15] (ii) structural changes occurring in the
solution .This may be due to the association taking place between the molecules. When the temperature
increases, the associated groups of molecules breakdown increasingly and the forces of attraction between the
molecules decrease. This leads to an increase in the adiabatic compressibility of the system[16]. The linear
increase in specific acoustic impendence with the molalities at a given temperature is observed in the solution as
shown in fig (4). This linear increase due to the effect of strong solute-solvent interaction[17]existing in the
solutions. The specific acoustic impedance is available as 18.39Rayl at 250
c*
of formamide from the
literature[18]. In the present investigation ,the inter-molecular free length of solutions is found to decrease with
respect to the various molality and increases with temperature. These changes reveal the fact that there is a
strong interaction exist between the solute and solvent[19]. When the salt is added to a solvent ,the strength of
the interaction increases as intermolecular free length decreases, with the molality changes [20]are shown in the
fig (5).
IV. Figures&Tables
TABLE(1) Internal pressure (atms)
Molality(m)
5°c 15°c 25°c 35°c 45°c 55°c
0.001 19448 15828 14076 12895 12087 10933
0.005 19843 16591 14080 12983 12239 10992
0.01 19658 16774 13943 12867 12090 10703
0.015 19779 16493 14002 12934 12117 10786
0.02 19376 16535 13916 12842 11875 10582
TABLE (2)FreeVolume (CC)
Molality(m)
5°c 15°c 25°c 35°c 45°c 55°c
0.001 .0076 0.0150 0.0242 0.0369 0.0557 0.0791
0.005 .0075 0.0140 0.0233 0.0356 0.0517 0.0767
0.01 .0073 0.0138 0.0225 0.0346 0.0489 0.0743
0.015 .0070 0.0133 0.0219 0.0340 0.0480 0.0724
0.02 .0069 0.0130 0.0208 0.0331 0.0473 0.0707
TABLE(3)Adiabatic compressibilityx10-11
(cm2
/dynes)
Molality(m)
5°c 15°c 25°c 35°c 45°c 55°c
0.001 3.23 3.28 3.41 3.52 3.62 3.69
0.005 3.19 3.27 3.35 3.45 3.59 3.66
0.01 3.16 3.24 3.32 3.39 3.55 3.61
0.015 3.14 3.22 3.28 3.36 3.51 3.58
0.02 3.13 3.20 3.28 3.33 3.44 3.54
TABLE (4) Specific acoustic impedance (Rayl)
Molality(m
5°c 15°c 25°c *
35°c 45°c 55°c
0.001 18.85 18.65 18.22 17.87 17.55 17.34
0.005 18.96 18.66 18.45 18.02 17.63 17.40
0.01 19.05 18.74 18.54 18.21 17.74 17.53
0.015 19.13 18.85 18.60 18.27 17.84 17.61
0.02 19.15 18.90 18.68 18.36 18.01 17.71
Analysis Of Transport Properties And Acoustical Parameters Of Sulphanilamide In Non- Aqueous
www.iosrjournals.org 3 | Page
TABLE(5)Intermolecular free length (A0
)
Molality(m)
5°c 15°c 25°c 35°c 45°c 55°c
0.001 1.071 1.106 1.156 1.195 1.231 1.260
0.005 1.065 1.104 1.142 1.184 1.225 1.255
0.01 1.060 1.100 1.134 1.173 1.218 1.247
0.015 1.055 1.095 1.133 1.169 1.211 1.241
0.02 1.054 1.092 1.128 1.164 1.200 1.234
Fig:1 Internal pressure (atms) Fig:2 Free Volume (cc)
Fig: 3 Adiabatic compressibility (cm2
/dyne) Fig: 4. Specific acoustic impedance (Rayl)
Fig ;5 Intermolecular free length(A0
)
1.05
1.10
1.15
1.20
1.25
.001 .005 .01 .015 .02
Intermolecularfree
length(A0)
Molality(m)
Inter molecular free length Vs
Molality
5°c
15°c
25°c
35°c
45°c
55°c
3.0
3.2
3.4
3.6
3.8
.001 .005 .01 .015 .02
Adiabatic
compressibility(cm2/dynes
Molality(m)
Adiabatic compressibility Vs
Molality
5°c
15°c
25°c
35°c
45°c
55°c
17.0
17.5
18.0
18.5
19.0
19.5
Specificaccousticimpedance(rayl)
Molality(m)
Specific acoustic impedance Vs
Molality
5°c
15°c
25°c
35°c
45°c
55°c
10000
12000
14000
16000
18000
20000
.001.005 .01 .015 .02
Internalpressure(atms)
Molality(m)
Internal pressure Vs Molality
5°c
15°c
25°c
35°c
45°c
55°c
Analysis Of Transport Properties And Acoustical Parameters Of Sulphanilamide In Non- Aqueous
www.iosrjournals.org 4 | Page
V. Conclusion
Sulfanilamide is a potent antibiotic because this drug undergoes metabolic alterations in tissues [21] .The
detailed study of acoustic parameters suggests that there is a molecular association existing between the molecules
of the solution. The addition of solute into the solvent brings about a strong solute-solvent interaction in the
solution.
References
[1]. R.A.Herole, V.S.Velingkar Int. journal of pharmaceutical chemistry (2005)45-49.
[2]. R.Palani, G.Srinivasan and B.Geeta lakshmi Int. journal of chemtech vol.3,No.1( 2011) 284 – 289.
[3]. Bhatti,S.S and singh,D.P., Ind.J. of pure &Applied physics (1982)961
[4]. Singh D.D ,J.Acoust.soci.India volume 14(1986)79-84
[5]. Kannappan A.N and Rajendran Ind pure &appl.phy vol 29(1991)451.
[6]. Kannappan A.N and Rajendran Ind pure &appl.phy vol 30(1992)240.
[7] Isht vibhu, Amit misra,manish Gupta and Shukla J.P Ind.Acad of sci.62(5)(2004)1147.
[8]. Thirumaran.S,Karthikeyan.N.Int.journal of chemical Research vol.3,(2011)83-98.
[9]. Jasmine Vasantha Rani E., Padmavathy R.,Kannagi K., Acoustic waves , 11(2011)152-162.
[10] Jasmine Vasantha Rani E.,Geetha, K., Solachi,V., Padmavathy R., and Kavitha J., J. Acou.Soc.India,vol.31 ,1-4(2003),323-326.
[11]. Kalyanasundaram,S., Manuel Stephen,H.,Gopalan A., Polym., Jand Mater,R(1995)323-333.
[12]. Syal V.K.etal.,J.Acous.soc.Ind.,vol 30(2002)84-87
[13]. Shahina Islam ,Waris B.N., Thermochemica acta,424(2004)165-174.
[14] Singhal S.P., Ind J. Pure and Appl.phys.,vol.3(1965)238-242.
[15]. Jahagirdhar D.V ., Arbad B.K., Walveier A.., Lande M..K and Shankarwar A.G ., Ind J .Pure and Appl.Ultrasonics,Vol 21(1999)
108-112.
[16]. Bhullerk., Bhavaneet k., et.al Acoustica 73(1991) . 291-293.
[17]. Erying and Kin card J.F., J.Chem.phys 41(1937)24.
[18]. DeepaJoshi, AsokkumarT.P, Ponia,BasentKumarand Deepa Bhatnagar. Journal of pure &Applied physics .32(2010)22-31.
[19]. Tewari k.,Patra C., Padhy S and ChakravarthyV.phys .,chem.Liq 32 (1996)149.
[20]. Agnihotri S.C ,and Om prakash. J.Acoust.soci.Ind,vol xiii No-4(1985) 186.
[21]. Sumathi .S ,Thamarai . P., Sheela C.D., Ebenezer R ., and Saravana Bhavas P J.of Co-ordination chemistry vol 64(2011)1673-
1682.

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Analysis of Transport Properties and Acoustical Parameters of Sulphanilamide in Non- Aqueous Medium

  • 1. IOSR Journal of Applied Physics (IOSR-JAP) e-ISSN: 2278-4861.Volume 4, Issue 1 (May. - Jun. 2013), PP 01-04 www.iosrjournals.org www.iosrjournals.org 1 | Page Analysis of Transport Properties and Acoustical Parameters of Sulphanilamide in Non- Aqueous Medium Santhakumari.S1 , Padmavathy.R2 , JasmineVasantharani.E2 1 Department of Physics,Shrimati Indira Gandhi College,Thiruchirappalli,Tamilnadu. 2 Department of Physics,Seethalakshmi Ramaswamy College,Thiruchirappalli,Tamilnadu. Abstract; Sulphanilamide is the parent compound of all the sulpha-durgs which is important in urinary tract infections and meningococcal meningitis profilaxes. Ultrasonic velocity measurements are highly sensitive to molecular interactions and used to provide qualitative informations about the physical nature and strength of the molecular ∕inter-ionic interactions. In the present work, non-aqueous solutions of Sulphanilamide have been prepared with different concentrations and the experiments were carried out from a low temperature of 50 c to a high temperature of 550 c. The ultrasonic velocity data combined with density and viscosity provides the standard means for determining the internal pressure, free volume and acoustical parameters. The various interactions occurring in the solutions are interpreted interms of ion-ion and ion-solvent interactions. An attempt is made to identify the entry of solvate into the samples and the entry of drug molecules into the solvate which supports to identify the molecular structure. Keywords : Acoustical parameters, free volume, Internal pressure, ion-solvent interactions ,ion-ion interactions. I. Introduction Sulphanilamide compounds identified as chemotherapeutic agents, possess broad spectrum of biological properties [1].Study of non –aqueous solutions is interesting for the physical understanding of the ion –solvent interactions. The passage of ultrasonic waves through solutions and liquids disturb the equilibrium between solute and solvent molecules. The velocity of such a wave is a thermodynamic quantity and is related to the physio – chemical properties of the medium[2].The velocity of ultrasonic waves in a medium and several other acoustic parameters which are dependent on it, helps to determine the overall response of the medium and about the nature of interactions between the molecules of the medium[3,4].Ultrasonic velocity of a liquid/solution is fundamentally related to the binding forces between the adequately employed in understanding the nature of molecular interaction in pure liquids[5,6,7]. The present work dealt with the ultrasonic investigations and acoustical study of (sulfanilamide) sulphanilamide in formamide . II. Experimental Technique The solutions of different molalities of sulphanilamide are prepared with AR grade formamide.Density of the solution is measured with 25ml of specific gravity bottle by a Digital balance of accuracy of .0001gm/cc. Cannonfenske viscometer is used for the viscosity measurements, and the time is noted by stop watch with an accuracy of ± 0.1sec. Mittal’s interferometer of frequency to 2MHz, with an accuracy of ± 2 m/s is used. . Internal pressure (πi) and free volume (vf) and acoustical parameters are evaluated by the following formulae. (i) Internal pressure (πi) = bRT [kη/u]1/2 ρ2/3 /M7/6 atms (ii) Free volume (vf) = [ Meff u/kη]3/2 cc (iii) Adiabatic compressibility (β) = [1/u2 ρ] cm2 /dynes (iv) Specific acoustic impedance (Z) = ρu (Rayl) (v) Intermolecular free length (Lf) = KT (βad 1/2 )A0 III . Results and Discussion In the present study internal pressure, exhibits an increasing trend with respect to increasing molalities as shown in fig (1).Internal pressure is a measure of cohesive energy of the system hence these variations may be due to the structure making nature of the solute in the solvent . It implies that there is a strong solute- solvent interaction taking place in the solution[8].The dependence of parameter on temperature has also been used to explain the strength of interactions with change in temperatures[9,10].The internal pressure decreases with rise in temperature of the solution. Since when the temperature is increased, there is a tendency for the ions to move for away from other ,reducing the possibility of interaction, which may further reduce the cohesive forces and
  • 2. Analysis Of Transport Properties And Acoustical Parameters Of Sulphanilamide In Non- Aqueous www.iosrjournals.org 2 | Page ultimately leads to a decrease in internal pressure[11].The variations of Vf with molalities as shown in fig (2) also confirm the structure making nature of the solute in the solvent. The adiabatic compressibility increases with decrease in molality and rise in temperature [12]as shown in fig (3). When the salt is added to the solvent ,the compressibility is lowered. This lowering is attributed to the influence of the electrostatic field of the ions on the surrounding solvent molecules. such a decrease may be due to (i) an increase in the number of incompressible molecule[13,14,15] (ii) structural changes occurring in the solution .This may be due to the association taking place between the molecules. When the temperature increases, the associated groups of molecules breakdown increasingly and the forces of attraction between the molecules decrease. This leads to an increase in the adiabatic compressibility of the system[16]. The linear increase in specific acoustic impendence with the molalities at a given temperature is observed in the solution as shown in fig (4). This linear increase due to the effect of strong solute-solvent interaction[17]existing in the solutions. The specific acoustic impedance is available as 18.39Rayl at 250 c* of formamide from the literature[18]. In the present investigation ,the inter-molecular free length of solutions is found to decrease with respect to the various molality and increases with temperature. These changes reveal the fact that there is a strong interaction exist between the solute and solvent[19]. When the salt is added to a solvent ,the strength of the interaction increases as intermolecular free length decreases, with the molality changes [20]are shown in the fig (5). IV. Figures&Tables TABLE(1) Internal pressure (atms) Molality(m) 5°c 15°c 25°c 35°c 45°c 55°c 0.001 19448 15828 14076 12895 12087 10933 0.005 19843 16591 14080 12983 12239 10992 0.01 19658 16774 13943 12867 12090 10703 0.015 19779 16493 14002 12934 12117 10786 0.02 19376 16535 13916 12842 11875 10582 TABLE (2)FreeVolume (CC) Molality(m) 5°c 15°c 25°c 35°c 45°c 55°c 0.001 .0076 0.0150 0.0242 0.0369 0.0557 0.0791 0.005 .0075 0.0140 0.0233 0.0356 0.0517 0.0767 0.01 .0073 0.0138 0.0225 0.0346 0.0489 0.0743 0.015 .0070 0.0133 0.0219 0.0340 0.0480 0.0724 0.02 .0069 0.0130 0.0208 0.0331 0.0473 0.0707 TABLE(3)Adiabatic compressibilityx10-11 (cm2 /dynes) Molality(m) 5°c 15°c 25°c 35°c 45°c 55°c 0.001 3.23 3.28 3.41 3.52 3.62 3.69 0.005 3.19 3.27 3.35 3.45 3.59 3.66 0.01 3.16 3.24 3.32 3.39 3.55 3.61 0.015 3.14 3.22 3.28 3.36 3.51 3.58 0.02 3.13 3.20 3.28 3.33 3.44 3.54 TABLE (4) Specific acoustic impedance (Rayl) Molality(m 5°c 15°c 25°c * 35°c 45°c 55°c 0.001 18.85 18.65 18.22 17.87 17.55 17.34 0.005 18.96 18.66 18.45 18.02 17.63 17.40 0.01 19.05 18.74 18.54 18.21 17.74 17.53 0.015 19.13 18.85 18.60 18.27 17.84 17.61 0.02 19.15 18.90 18.68 18.36 18.01 17.71
  • 3. Analysis Of Transport Properties And Acoustical Parameters Of Sulphanilamide In Non- Aqueous www.iosrjournals.org 3 | Page TABLE(5)Intermolecular free length (A0 ) Molality(m) 5°c 15°c 25°c 35°c 45°c 55°c 0.001 1.071 1.106 1.156 1.195 1.231 1.260 0.005 1.065 1.104 1.142 1.184 1.225 1.255 0.01 1.060 1.100 1.134 1.173 1.218 1.247 0.015 1.055 1.095 1.133 1.169 1.211 1.241 0.02 1.054 1.092 1.128 1.164 1.200 1.234 Fig:1 Internal pressure (atms) Fig:2 Free Volume (cc) Fig: 3 Adiabatic compressibility (cm2 /dyne) Fig: 4. Specific acoustic impedance (Rayl) Fig ;5 Intermolecular free length(A0 ) 1.05 1.10 1.15 1.20 1.25 .001 .005 .01 .015 .02 Intermolecularfree length(A0) Molality(m) Inter molecular free length Vs Molality 5°c 15°c 25°c 35°c 45°c 55°c 3.0 3.2 3.4 3.6 3.8 .001 .005 .01 .015 .02 Adiabatic compressibility(cm2/dynes Molality(m) Adiabatic compressibility Vs Molality 5°c 15°c 25°c 35°c 45°c 55°c 17.0 17.5 18.0 18.5 19.0 19.5 Specificaccousticimpedance(rayl) Molality(m) Specific acoustic impedance Vs Molality 5°c 15°c 25°c 35°c 45°c 55°c 10000 12000 14000 16000 18000 20000 .001.005 .01 .015 .02 Internalpressure(atms) Molality(m) Internal pressure Vs Molality 5°c 15°c 25°c 35°c 45°c 55°c
  • 4. Analysis Of Transport Properties And Acoustical Parameters Of Sulphanilamide In Non- Aqueous www.iosrjournals.org 4 | Page V. Conclusion Sulfanilamide is a potent antibiotic because this drug undergoes metabolic alterations in tissues [21] .The detailed study of acoustic parameters suggests that there is a molecular association existing between the molecules of the solution. The addition of solute into the solvent brings about a strong solute-solvent interaction in the solution. References [1]. R.A.Herole, V.S.Velingkar Int. journal of pharmaceutical chemistry (2005)45-49. [2]. R.Palani, G.Srinivasan and B.Geeta lakshmi Int. journal of chemtech vol.3,No.1( 2011) 284 – 289. [3]. Bhatti,S.S and singh,D.P., Ind.J. of pure &Applied physics (1982)961 [4]. Singh D.D ,J.Acoust.soci.India volume 14(1986)79-84 [5]. Kannappan A.N and Rajendran Ind pure &appl.phy vol 29(1991)451. [6]. Kannappan A.N and Rajendran Ind pure &appl.phy vol 30(1992)240. [7] Isht vibhu, Amit misra,manish Gupta and Shukla J.P Ind.Acad of sci.62(5)(2004)1147. [8]. Thirumaran.S,Karthikeyan.N.Int.journal of chemical Research vol.3,(2011)83-98. [9]. Jasmine Vasantha Rani E., Padmavathy R.,Kannagi K., Acoustic waves , 11(2011)152-162. [10] Jasmine Vasantha Rani E.,Geetha, K., Solachi,V., Padmavathy R., and Kavitha J., J. Acou.Soc.India,vol.31 ,1-4(2003),323-326. [11]. Kalyanasundaram,S., Manuel Stephen,H.,Gopalan A., Polym., Jand Mater,R(1995)323-333. [12]. Syal V.K.etal.,J.Acous.soc.Ind.,vol 30(2002)84-87 [13]. Shahina Islam ,Waris B.N., Thermochemica acta,424(2004)165-174. [14] Singhal S.P., Ind J. Pure and Appl.phys.,vol.3(1965)238-242. [15]. Jahagirdhar D.V ., Arbad B.K., Walveier A.., Lande M..K and Shankarwar A.G ., Ind J .Pure and Appl.Ultrasonics,Vol 21(1999) 108-112. [16]. Bhullerk., Bhavaneet k., et.al Acoustica 73(1991) . 291-293. [17]. Erying and Kin card J.F., J.Chem.phys 41(1937)24. [18]. DeepaJoshi, AsokkumarT.P, Ponia,BasentKumarand Deepa Bhatnagar. Journal of pure &Applied physics .32(2010)22-31. [19]. Tewari k.,Patra C., Padhy S and ChakravarthyV.phys .,chem.Liq 32 (1996)149. [20]. Agnihotri S.C ,and Om prakash. J.Acoust.soci.Ind,vol xiii No-4(1985) 186. [21]. Sumathi .S ,Thamarai . P., Sheela C.D., Ebenezer R ., and Saravana Bhavas P J.of Co-ordination chemistry vol 64(2011)1673- 1682.