ISSN : 0970 - 020X, ONLINE ISSN : 2231-5039
     FacebookTwitterLinkedinMendeley

The Physico-Chemical and Solvolytic Study of Alprazolam Drug In Ethanol at 303 K

Chandra Kant Bhardwaj1*, Anjna Kumari2, Anjul Singh2

*1Department of Chemistry, Doon Institute of Engg. and Technology, Rishikesh, U.K.(India) 2Department of Chemistry D. S. College, Aligarh, U.P. [India]

DOI : http://dx.doi.org/10.13005/ojc/300261

Article Publishing History
Article Received on :
Article Accepted on :
Article Published : 04 Jun 2014
Article Metrics
ABSTRACT:

The physico-chemical and solute –solvent interaction of Alprazolam in ethanol were reported  at 303 K.  The solute solvent  interaction have been carriedout by computing various acoustic  parameters, Specific acoustic impedance(z),Intermolecular freelength(Lf),Isentropic compressibility (bs) , Apparent molal adiabatic compressibility  (fk  ) , Shear’s  relaxation ( ts ), and Solvation number (Sn).These parameters have been evaluated by using ultrasound velocity, density and viscosity data.These results are interpreted in terms of solute-solvent interaction between the molecules.

KEYWORDS:

Solute-solvent interaction; Ultrasound velocity; Alprazolam.

Download this article as: 

Copy the following to cite this article:

Bhardwaj C. K, Kumari A, Singh A. The Physico-Chemical and Solvolytic Study of Alprazolam Drug In Ethanol at 303 K. Orient J Chem 2014;30(2).


Copy the following to cite this URL:

Bhardwaj C. K, Kumari A, Singh A. The Physico-Chemical and Solvolytic Study of Alprazolam Drug In Ethanol at 303 K. Orient J Chem 2014;30(2). Available from: http://www.orientjchem.org/?p=3554


Introduction

Alprazolam is a triazolobenzodiazepine compound with antianxiety and sedative-hypnotic actions, that is efficacious in the treatment of panic disorders, with or without agoraphobia and in generalized anxiety disorders.It is marketed under the trade name xanax.

 In the present study, we are reported the ultrasound velocity, density and viscosity measurements at 303K have been used to calculate Intermolecular freelength(Lf) [1] , Specific acoustic impedance(z) [2], Apparent molal adiabatic compressibility  (fk  ) [3] ,  Shear’s  relaxation ( ts ), and Solvation number (Sn) [4] of Alprazolam compound in ethanol at 303 K .  Several investigators have reported the results on ultrasound studies of liquid mixtures [4-12].

EXPERIMENTAL

The solutions were prepared by dissolving the accurately known weight of  Alprazolam in ethanol and kept for some time. A continuous interferometer technique was employed for measurement of ultrasound velocity at 2Mhz. The density and viscosity were determined using vibrating densitometer DMA 48  fitted with a Hook G thermostat and viscometer. The  experiment were reported atleast twice and results were reproducible with experimental error 0.00002 Kgm3 and 0.001 cm/ sec respectively.

Computation of different physical parameters

Ultrasound Velocity (V)

V = 2d × 105 cm/ sec. or V = 2d × 103 m/ sec

Density

Formula1

where ‘M’: is the weight of the liquid filled in pyknometer used.

‘r’is radius of capillaries

‘h1’& ‘h2’are the heights of the liquid in capillaries

Viscosity ( η)

Formula 2

where

h’            is the viscosity of liquid

r’            is the density of liquid.

t’             is the time flow of liquid

‘a’&’b’     are viscometeric constants.

Specific Acoustic Impedance

Z = Vr.

Where, V and ‘p’ are the ultrasonic velocity and density respectively.

Isentropic Compressibility 

Formula 3

where ‘V’ is the ultrasound velocity and ‘p’ is the density of liquid mixtures.

Intermolecular Free Length

Formula 4

where,

‘K’ is temperature dependent constant.

Molal Adiabatic Compressibility

Formula 5

 

where ‘p0’ and ‘βs0’ are compressibility and density of pure solvent and ‘βs’ & ‘p’ are the compressibility and density of the solution respectively.

‘C’ is the concentration in mole/liter of solute.

‘M’ is the molecular weight of solute.

Solvation Number 

Formula 6

Where ‘ n1 ‘ moles of solvent and ‘ n2 ‘   moles of solute

Shear’s Relaxation Time (t)

Formula 7

RESULT AND DISCUSSION

The ultrasound velocity of the solution of Alprazolam drug in ethanol increases with increasing concentration Alprazolam drug which is shown in above table.

Table-: Alpra zolam + ethanol At 303K

Conc. of ethanol mol/litre

Ultrasound velocity m/sec.

Density gm/mol. (Exp.)

Specific Acoustic Impedance (C.G.S.) z´10-5

Isentropic compressibility (Exp.) cm2/dyne.1012

Lowering Isentropic compressibility cm2/deyne.1012

Intermolecular free length (Ao)

Viscosity (Exp.) (C.P.)

Apparent molal Adiabatic compressibility cm2/dyne.109

Solvation number

Shear’s Relaxation time

0.0025

1166

0.7883

0.0919

93.31

-6.76

0.6095

1.2546

-274.1037

46.2196

156.0890

0.0050

1170

0.7923

0.0927

92.20

-7.87

0.6059

1.2960

-167.4630

53.8089

159.3216

0.0075

1175

0.7965

0.0936

90.94

-9.13

0.6017

1.3374

-134.2552

62.4238

162.1642

0.0100

1178

0.8010

0.0944

89.97

-10.10

0.5985

1.3786

-115.1329

69.0559

165.3769

0.0125

1184

0.8052

0.0953

88.59

-11.48

0.5939

1.4201

-106.6343

78.4912

167.7422

0.0150

1188

0.8091

0.0961

87.57

-12.50

0.5905

1.4515

-98.3142

85.4652

169.4771

0.0175

1190

0.8137

0.0968

86.78

-13.29

0.5878

1.5026

-91.5657

90.8666

173.8608

0.0200

1196

0.8178

0.0978

85.49

-14.59

0.5834

1.5442

-88.7363

99.6866

176.0182

0.0225

1199

0.8199

0.0983

84.84

-15.23

0.5812

1.5853

-82.4719

104.1308

179.3291

0.0250

1202

0.8263

0.0993

83.76

-16.31

0.5775

1.6271

-81.4079

111.5150

181.7145

 

The variation of velocity with concentration ( C) can be expressed  by the following relationship.

Formula 8

The result shows that while the density increases, the isentropic compressibility decreases with increasing concentration of the solute and quantity (dp/dc) is positive while (dβs/ dc) is negative. Since the value of

Formula 9

are larger than the value of

Formula 10

for the system . The concentration derivatives of velocity( dv/dc) is positive. i.e. the ultrasonic velocity increases with increasing the concentration of solute (13-16).

Figure 1 A Figure 1. A
Click here to View Figure

 

Intermolecular free length and isentropic compressibility (  βs  ) of Alprazolam drug solution decreases with increase in molar concentration of solute (Fig.1-b) .The complementary use of isentropic compressibility data can provide interesting information of of solute- solvent interaction.

Figure 1 B Figure 1. B
Click here to View Figure

 

Apparent molal adiabatic compressibility () varies linearly s the square root of concentration.The value of apparent molal adiabatic compressibilities are negative with the increase in molar concentration. The values of apparent molal adiabatic compressibility as shown in figure  1 (c) . The values of  for the solutions of Alprazolam drug  were tabulated in table. These results are in agreement with the result reported by Masson (17) for electrolytic solution.

Figure 1. C Figure 1. C
Click here to View Figure

 

The value of specific acoustic impedance (z) increases with increasing the concentration of Alprazolam drug can be explained on the basis of lyophobic interaction between solute and solvent molecules which increase the intermolecular distance making relatively under gaps between the molecules and becoming the main cause of impedance in the propagation of ultrasound waves are tabulated.

The increase with the concentration suggest a significant interaction between the solute solvent molecules and the values are in agreement with the reported for solution of cobalt carboxylates (18).

From the above discussion it is concluded that solvolytic study of Alprazolam in ethanol at 303 K shows specific ion – solvent interaction. Alprazolam drug shows significant solvolysis in ethanol.

REFRENCES

  1. Jacobson,B., Acta Chem.Scand., 6 : 1485 (1952).                  
  2. Elpiner,I.E., Ultrasound Physical, Chemical& Biological effects. New York Consultants Bureau, 371 (1960).
  3. Passynskii, A., Act Physico Chem., (U.S.S.R), 8 : 357 (1933); J. Phys. Chem., (U.S.S.R.), 11: 451 (1938).
  4. Hori, Mistsukazu, Mishiwki, Nobuhiko, Kata Gijustu, 17(12) :45-48 (2002).
  5. Kannappan, A.N. and  Palani, Rashid, Indian J. Chem., Vol. 46A : 54-59 (2007).
  6.  Josh, M.N., Diego, A.H., J. Chem. Engg. Data, 51 (2) :722 (2006).
  7. Begum, Zareena, Sandhya Sri, P.B., Karuna Kumar, D.B., Rambabu, C., Journal Of Molecular Liquids, vol. 178 : 99- 112 (2013).
  8. Prabhabati, C.L., Shiv Kumar, K., Venkatashwarlu, P. and Raman, G.K., Ind. J. Chem., 43A , : 294 (2004).
  9. Mehra, Rita and Israni, Rekha, Ind. J. Chem. Soc., 81 : 221 (2004).
  10. Das, U.N., Roy, G.S., and Mohanty, S., Ind. J. of Chem. Tech., 11 : 714 (2004).
  11. Prakash, S., Chaturvedi,C.V., Ind. J. Chem., 10 : 669 (1972) .
  12. Waeissler, A., J.Chem. Phys., 15 : 210 (1947).
  13. Sharma, R.K., Bhardwaj , C.K., Yadav, S.S., Material Science Research India, 3(1a) : 97-102 (2006).
  14. Ramabrahman, K. and Suryanarayan, M., Ind. J. Pure Appl. Phys., 6, 422 (1968).
  15. Miknailor, I.G., Rozina, M.V. & Snutilov, V.A., Akust. Zh., 10 : 213 (1964).
  16. Bachem, C., Physica (Netherlands), 101: 541 (1935).
  17. Masson, D.O., Phil. Mag. B., 218 (1929).
  18. Padmini, P. and Rao, B., Indian J. Phys. 34 : 565 (1960)


Creative Commons License
This work is licensed under a Creative Commons Attribution 4.0 International License.