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71 CHAPTER 4 PARTIAL MOLAL VOLUMES, PARTIAL MOLAL COMPRESSIBILITIES AND VISCOSITY B-COEFFICIENTS OF SALBUTAMOL SULPHATE IN AQUEOUS METHANOL SOLUTIONS AT 303.15 K, 308.15 K, 313.15 K AND 318.15 K 4.1 INTRODUCTION Solute-solvent interactions play an important role in a variety of phenomena. In bio-physical chemistry, drug interaction is a subject of intensive studies, involving complex molecular mechanisms. Despite years of investigations, many important drug actions and their mechanisms are not fully understood. Structure activity relationship is one of the most common rationale presented for explaining drug reactions. One of the precise features that confer the solution properties of drug molecules is the implication of hydrophobic and charge contributions. In water, however, since the polar groups are hydrated, the intermolecular aggregation of drug molecules through their hydrophobic parts is expected to occur in a way analogous to miscillization, favouring their limited aqueous solubilization. However, this aggregating tendency is affected with the addition of the non-aqueous component. Alcohol molecules contain both hydrophilic groups and hydrophobic tails. This unique quality towards an aqueous environment leads to a complex self association behaviour which is

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71

CHAPTER 4

PARTIAL MOLAL VOLUMES, PARTIAL MOLAL

COMPRESSIBILITIES AND VISCOSITY

B-COEFFICIENTS OF SALBUTAMOL SULPHATE IN

AQUEOUS METHANOL SOLUTIONS AT 303.15 K,

308.15 K, 313.15 K AND 318.15 K

4.1 INTRODUCTION

Solute-solvent interactions play an important role in a variety of

phenomena. In bio-physical chemistry, drug interaction is a subject of

intensive studies, involving complex molecular mechanisms. Despite years of

investigations, many important drug actions and their mechanisms are not

fully understood. Structure activity relationship is one of the most common

rationale presented for explaining drug reactions.

One of the precise features that confer the solution properties of

drug molecules is the implication of hydrophobic and charge contributions.

In water, however, since the polar groups are hydrated, the intermolecular

aggregation of drug molecules through their hydrophobic parts is expected to

occur in a way analogous to miscillization, favouring their limited aqueous

solubilization. However, this aggregating tendency is affected with the

addition of the non-aqueous component. Alcohol molecules contain both

hydrophilic groups and hydrophobic tails. This unique quality towards an

aqueous environment leads to a complex self association behaviour which is

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72

not exhibited in non aqueous solvents. The solution behaviour of alcohol

molecules in the water region is largely established by the phenomenon of a

polar or hydrophobic hydration. There are some reports available in literature

on the volumetric and transport properties of some drugs in aqueous methanol

solution system. Sharma et al (2008) have reported the values of ultrasonic

velocity and viscosity studies of narcotic drugs Parvodex and Tramacip in

binary mixtures of water +alcohol at 25oC. They have calculated free volume,

internal pressure and molar cohesive energy, from these results they

characterized the systems of hydrogen bonding in aqueous alcohol. The

studied drugs behave as structure promoter and enhance the presence of

interactions in the aqueous alcohol system.

Syal et al (2005) determined ultrasonic velocity values of Drug

Parvon–spas in mixed alcohol-water solvent systems at 25oC, and they have

characterized by hydrogen bonding in methanol, ethanol and propan-1-ol,

solute-solvent interactions .Further the studied drugs behave as structure

promoter in the aqueous alcohol systems. Sharma et al (2008a) have

determined partial molar volumes of the drugs namely Parvon-spas,

Parvon-Forte, Tramacip, Parvodex in various aqueous mixtures of alcohols at

25oC. Furthermore, the results are correlated to understand the solution

behaviour of drugs in aqueous-alcoholic systems, as a function of the nature

of the alcohol and solutes.

Sharma et al (2007) have reported viscosity values of drugs namely

Parvon-spas, Parvon-Forte, Tramacip, Parvodex in various aqueous mixtures

of alcohols (methanol, ethanol and 1-prapanol) at 25oC. The viscosity data

have been analyzed for the evaluation of A and B coefficients using

Jones-Dole equation. B-coefficients were found to be positive thereby

showing drug-solvent interactions. From these studies they concluded that all

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the drug cations can be regarded as structure-makers due to hydrophobic

hydration of the drug molecules.

The partial molal volume is a characteristic parameter which is

indicative of molecular interactions in the solution phase. The transport

properties of drug molecules have important implications for the permeation

of the drug molecules through biological membranes. Thus, the behaviour of

the drugs in solutions may be of importance from a pharmacological point of

view. Further, alcohols are often present in drug delivery formulation.

Literature survey shows that thermodynamic and transport

properties of salbutamol sulphate in aqueous methanol solutions have not

been attempted. This chapter highlights the molecular interaction studies of

the drug salbutamol sulphate in water-methanol mixtures at different

temperatures. The data on density ( ), ultrasonic speed (u) and viscosity ( )

of salbutamol sulphate in different concentrations of aqueous methanol

solution are presented at four different temperatures. From these

experimental data, several thermodynamic and transport parameters like

apparent molal volume V , partial molal volume 0V , molal expansivity 0

2E ,

isobaric thermal expansion coefficient ( 2 ), second derivative of infinite

dilution of apparent molal volume with temperature 202 / TV , isentropic

compressibility sk , change in isentropic compressibility s , relative change

in isentropic compressibility ( 0/ ss kk ), apparent molal compressibility K ,

partial molal compressibility 0K , viscosity B-coefficient, variation of B-

coefficient with temperature, i.e., dB/dT, free energy of activation per mole of

solvent *01 and solute *0

2 are computed. The thermodynamic and

transport properties are discussed in terms of drug-solvent interaction and

structure making ability of the drug in the aqueous methanol solution.

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4.2 EXPERIMENTAL

The densities, ρ, ultrasonic speeds, u and viscosities, η, of

salbutamol sulphate in aqueous methanol volume by volume ratio are

measured at temperatures, 303.15, 308.8.15, 313.15 and 318.15 K, using a

single capillary pycnometer, a single-crystal variable-path multifrequency

ultrasonic interferometer operating at 2 MHz and a Ubbelohde type suspended

level viscometer which are discussed in detail in Chapter 2.

4.3 RESULTS

The experimentally measured density values for the of salbutamol

sulphate in aqueous methanol solution at T = 308.15, 313.15 and 318.15 K are

shown in Table 4.1. The Uncertainty values with density are also given in

the same Table 4.1.

Table 4.1 Densities, , of Salbutamol Sulphate in Aqueous Methanol

Solution at different temperatures

mS / mol kg-1

10-3 / kg m-3

303.15 K 308.15 K 313.15 K 318.15 K

(V/V-90%W+10%M)

0.0000 0.9858 0.9856 0.9830 0.9804

0.0500 0.9930 0.9922 0.9886 0.9852

0.0750 0.9976 0.9965 0.9922 0.9885

0.1000 1.0026 1.0015 0.9963 0.9923

0.1250 1.0088 1.0071 1.0006 0.9965

0.1500 1.0141 1.0124 1.0051 1.0012

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Table 4.1 (Continued)

mS / mol kg-1

10-3 / kg m-3

303.15 K 308.15 K 313.15 K 318.15 K =4.2010-4 =4.0110-4 =3.2910-4 =3.0910-4 (V/V-80%W+20%M)

0.0000 0.9781 0.9747 0.9727 0.9694 0.0500 0.9851 0.9812 0.9782 0.9742 0.0750 0.9889 0.9854 0.9816 0.9774 0.1000 0.9939 0.9902 0.9854 0.9811 0.1250 0.9989 0.9954 0.9896 0.9849 0.1500 1.0039 1.0002 0.9938 0.9893

=3.8310-4 =3.8210-4 =3.1310-4 =2.9510-4 (V/V-70% W + 30% M)

0.0000 0.9588 0.9585 0.9582 0.9534 0.0500 0.9652 0.9647 0.9635 0.9582 0.0750 0.9693 0.9689 0.9669 0.9613 0.1000 0.9751 0.974 0.9709 0.9650 0.1250 0.9798 0.9792 0.9749 0.9689 0.1500 0.9859 0.9847 0.9792 0.9731

=4.0410-4 =3.9210-4 =3.1210-4 =2.9310-4 (V/V-60% W+40%M)

0.0000 0.9438 0.9432 0.9410 0.9386 0.0500 0.9500 0.9492 0.9459 0.9432 0.0750 0.9545 0.9533 0.9489 0.9461 0.1000 0.9594 0.9583 0.9522 0.9494 0.1250 0.9645 0.9634 0.9558 0.9528 0.1500 0.9704 0.9688 0.9595 0.9564

=3.9610-4 =3.8410-4 =2.7410-4 =2.6510-4 (V/V-50% W+50%M)

0.0000 0.9315 0.9301 0.9279 0.9241 0.0500 0.9373 0.9357 0.9326 0.9286 0.0750 0.9412 0.9393 0.9354 0.9314 0.1000 0.9453 0.9435 0.9385 0.9347 0.1250 0.9502 0.9481 0.9424 0.9385 0.1500 0.9556 0.9526 0.9462 0.9432

=3.5610-4 =3.3610-4 =2.7110-4 =2.8110-4 mS- stands for molal concentration of salbutamol sulphate:

-uncertainty in density values

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Density values are used to calculate the apparent molal volumes of

salbutamol sulphate in aqueous methanol solution using equation 1.1 and are

given in Table 4.2. The error values for apparent molal volume are evaluated

using equation 1.2 and are given in Table 4.2 within parenthesis.

Table 4.2 Apparent Molal Volume V of Salbutamol Sulphate in

Aqueous Methanol Solution at Different Temperatures

mS / mol kg-1

V 610 /m3 mol-1

308.15 K 308.15 K 313.15 K 318.15 K

(V/V-90%W+10%M)

0.0500 433.7(2.17) 446.2(2.06) 468.1(1.70) 485.9(1.61)

0.0750 418.1(1.08) 430.7(1.06) 455.5(0.85) 471.9(0.81)

0.1000 405.2(0.72) 414.7(0.68) 443.0(0.57) 458.8(0.54)

0.1250 386.6(0.54) 399.4(0.51) 433.2(0.42) 446.9(0.40)

0.1500 380.9(0.43) 390.6(0.41) 424.6(0.34) 434.7(0.32)

(V/V-80%W+20%M)

0.0500 440.1(1.99) 451.7(2.00) 473.9(1.65) 490.3(1.57)

0.0750 434.3(1.00) 436.6(1.00) 463.2(0.83) 477.5(0.79)

0.1000 417.7(0.66) 421.7(0.67) 452.8(0.55) 464.8(0.52)

0.1250 407.0(0.50) 408.6(0.50) 442.3(0.41) 455.7(0.39)

0.1500 399.3(0.40) 402.1(0.40) 434.8(0.33) 444.6(0.31)

(V/V-70%W+30%M)

0.0500 459.2(2.19) 463.6(2.13) 483.7(1.70) 496.8(1.61)

0.0750 444.3(1.10) 445.8(1.06) 471.2(0.85) 484.9(0.81)

0.1000 417.1(0.73) 425.9(0.71) 457.5(0.57) 471.5(0.54)

0.1250 409.8(0.55) 412.4(0.53) 448.5(0.43) 460.9(0.40)

0.1500 393.8(0.44) 400.5(0.42) 439.7(0.34) 451.1(0.32)

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Table 4.2 (Continued)

mS / mol kg-1

V 610 /m3 mol-1

308.15 K 308.15 K 313.15 K 318.15 K

(V/V-60%W+40%M)

0.0500 468.7(2.22) 473.4(2.15) 499.6(1.55) 507.5(1.50)

0.0750 445.8(1.11) 455.1(1.07) 489.8(0.77) 496.9(0.75)

0.1000 428.8(0.74) 434.6(0.72) 480.6(0.52) 486.2(0.50)

0.1250 416.0(0.55) 420.7(0.54) 471.7(0.39) 478.2(0.38)

0.1500 400.7(0.44) 408.4(0.43) 464.4(0.31) 470.8(0.30)

(V/V-50%W+50%M)

0.0500 482.4(2.05) 487.5(1.94) 509.7(1.57) 516.2(1.64)

0.0750 465.2(1.03) 473.4(0.97) 501.3(0.79) 506.0(0.82)

0.1000 453.3(0.68) 458.4(0.65) 492.8(0.53) 494.3(0.55)

0.1250 437.9(0.51) 444.9(0.48) 479.3(0.39) 481.7(0.41)

0.1500 423.0(0.41) 435.9(0.39) 470.5(0.32) 465.3(0.33)

mS- stands for molal concentration of salbutamol sulphate

Partial molal volume 0V of salbutamol sulphate are evaluated from

linear plot of V Vs m are shown in Figure 4.1 using the least squares method

of the following general equation (1.3). The evaluated values of 0V and slope

Sv are given in Table 4.3.

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350

370

390

410

430

450

470

490

510

0.04 0.06 0.08 0.10 0.12 0.14 0.16

m / (mol.kg-1)

V

10

-6m

3 mol

-1)

Figure 4.1 Plot of apparent molal volume ( V ) against molal

concentration (m) of salbutamol sulphate in (♦) 303.15

K, (■) 308.15 K, (▲) 313.15 K, (Δ) 318.15 K of (90% W +

10% M)

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Table 4.3 Partial Molal Volume 0V , Experimental Slopes SV, Limiting

Molal Expansivity 02E , Isobaric Thermal Expansion

Coefficient 2 and Hepler’s Constant ( 2 0V /T2) of

Salbutamol Sulphate in Aqueous Methanol Solution at Different Temperatures

T/K 0V 106

(m3mol-1) SV106

(m3l1/2mol-3/2)

02E 106

(m3mol-1k-1) 2 103

(k-1)

202 / TV

(m6mol-2k-2) (V/V-90%W+10%M)

303.15 459.6(4.56) -547.5

3.308

7.196

0.0857 308.15 473.2(3.42) -569.6 6.989 313.15 488.5(2.23) -436.6 6.771 318.15 510.7(1.05) -510.2 6.476

(V/V-80%W+20%M) 303.15 463.3(3.84) -435.7

3.272

7.062 0.0700 308.15 475.0(4.25) -508.9 6.888 313.15 493.1(1.51) -396.9 6.635 318.15 511.8(1.76) -452.9 6.393

(V/V-70%W + 30%M) 303.15 490.9(6.78) -661.1

1.916

3.902 0.1228 308.15 493.5(4.02) -638.3 3.882 313.15 504.4(2.74) -442.7 3.798 318.15 519.2(1.62) -461.6 3.690

(V/V-60%W + 40%M) 303.15 498.9(4.53) -663.9 1.802 3.612 0.0291 308.15 504.2(4.15) -657.8 3.573 313.15 516.6(1.12) -353.4 3.488 318.15 524.8(1.19) -368.5 3.437

(V/V-50%W + 50%M) 303.15 510.8(1.70) -584.3 2.302 4.507 0.0103 308.15 512.7(2.81) -526.6 4.490 313.15 530.9(2.12) -401.8 4.336 318.15 543.1(2.81) -504.3 4.238

W - stands for Water M – stands for methanol

Parenthesis indicates standard error

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The values of molal expansivity are calculated (Rudan-Tasic 1998)

from the partial molal volume using the following relation (4.1)

02E = PTV )/( 0 (4.1)

The evaluated values of 02E are also given in Table 4.3.

From the partial molal volume 0V the isobaric thermal expansion

coefficient of the solute at infinite dilution, 2 is evaluated using the

following equation (Iqbal and Siddiquah 2006)

2 = PTVV )/)(/1( 00 = 002 / VE (4.2)

and the calculated values are included in Table 4.3.

The partial molal volume values, 0V , are related to temperature ‘T’

using the quadratic equation given by 1.16. The values of 202 / TV are

evaluated and given in Table 4.3.

The experimental data on ultrasonic speed of salbutamol sulphate in

aqueous methanol solutions are given in Table 4.4. The uncertainty u values

for ultrasonic speed are calculated and also given in Table 4.4.

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Table 4.4 Ultrasonic Speed u , of Salbutamol Sulphate in Aqueous Methanol Solution at Different Temperatures

mS / mol kg-1

u / m s-1 303.15 K 308.15 K 313.15 K 318.15 K

(V/V-90% W + 10%M) 0.0000 1535.0 1539.8 1545.0 1548.6 0.0500 1546.8 1552.6 1559.0 1563.7 0.0750 1550.9 1556.8 1564.4 1569.7 0.1000 1554.3 1559.4 1568.8 1574.6 0.1250 1555.3 1562.5 1572.5 1578.7 0.1500 1555.7 1564.9 1576.0 1582.0

u = 3.2310-4 u = 3.6810-4 u = 4.5610-4 u = 4.9510-4 (V/V-80% W + 20% M)

0.0000 1554.3 1556.8 1561.6 1565.0 0.0500 1567.9 1569.6 1575.8 1580.2 0.0750 1572.8 1574.1 1581.5 1585.9 0.1000 1576.5 1577.4 1586.3 1590.4 0.1250 1579.8 1580.2 1590.1 1595.1 0.1500 1583.3 1583.5 1594.0 1598.7

u =4.2410-4 u =3.8910-4 u =4.7610-4 u =4.9510-4

(V/V-70%W + 30% M) 0.0000 1566.1 1560.2 1556.0 1549.8 0.0500 1578.8 1573.3 1570.6 1564.6 0.0750 1583.5 1577.4 1575.8 1570.6 0.1000 1585.3 1579.8 1579.4 1575.4 0.1250 1588.8 1581.8 1584.6 1579.8 0.1500 1589.6 1583.2 1588.5 1583.6

u = 3.5510-4 u = 3.4510-4 u = 4.7210-4 u = 4.9810-4

(V/V-60% W + 40% M) 0.0000 1549.6 1544.3 1541.6 1538.2 0.0500 1562.8 1557.1 1556.1 1553.1 0.0750 1566.8 1561.5 1562.1 1559.1 0.1000 1569.9 1564.3 1567.3 1564.2 0.1250 1572.7 1566.8 1572.2 1569.2 0.1500 1574.1 1568.7 1576.6 1573.8

u = 3.6710-4 u = 3.6410-4 u = 5.1410-4 u = 5.2110-4

(V/V-50%W + 50% M) 0.0000 1528.4 1517.6 1506.5 1493.6 0.0500 1542.4 1530.6 1520.8 1508.0 0.0750 1546.9 1535.3 1526.6 1513.9 0.1000 1551.4 1538.7 1531.9 1518.7 0.1250 1554.4 1541.6 1536.0 1522.8 0.1500 1556.5 1544.6 1540.0 1525.4

u = 4.2010-4 u = 3.9610-4 u = 4.9410-4 u = 4.7610-4

mS - stands for molal concentration of salbutamol sulphate u - stands for uncertainty in ultrasonic speed

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The data on ultrasonic speed and density are used to calculate the

isentropic compressibility Sk using the equation 1.17 and the values are given

in Table 4.5. The uncertainty in Sk values are calculated using the equation

1.18 and are given in parenthesis of Table 4.5.

Table 4.5 Isentropic Compressibilities Sk of Salbutamol Sulphate in

Aqueous Methanol Solution at Different Temperatures

mS / mol kg-1

Sk 1011 (Pa-1)

303.15 K 308.15 K 313.15 K 318.15 K

(V/V-90%W + 10%M) 0.0000 43.05(1.98) 42.79(1.89) 42.61(1.65) 42.53(1.59)

0.0500 42.09(1.93) 41.81(1.84) 41.61(1.60) 41.51(1.54)

0.0750 41.67(1.89) 41.40(1.81) 41.18(1.58) 41.05(1.52)

0.1000 41.28(1.87) 41.06(1.79) 40.78(1.55) 40.64(1.50)

0.1250 40.97(1.84) 40.67(1.76) 40.41(1.53) 40.26(1.48)

0.1500 40.68(1.82) 40.33(1.74) 40.05(1.51) 39.90(1.46)

(V/V-80%W + 20%M) 0.0000 42.32(1.83) 42.33(1.82) 42.15(1.59) 42.11(1.53)

0.0500 41.29(1.78) 41.36(1.77) 41.16(1.54) 41.10(1.49)

0.0750 40.87(1.75) 40.95(1.74) 40.73(1.52) 40.68(1.47)

0.1000 40.48(1.73) 40.58(1.72) 40.32(1.50) 40.29(1.45)

0.1250 40.11(1.70) 40.23(1.70) 39.96(1.48) 39.90(1.43)

0.1500 39.73(1.68) 39.87(1.67) 39.60(1.46) 39.54(1.41)

(V/V-70%W + 30%M) 0.0000 42.52(1.93) 42.86(1.89) 43.10(1.64) 43.66(1.61)

0.0500 41.56(1.87) 41.87(1.84) 42.07(1.59) 42.63(1.56)

0.0750 41.14(1.85) 41.48(1.79) 41.65(1.57) 42.17(1.54)

0.1000 40.80(1.82) 41.13(1.77) 41.29(1.55) 41.75(1.52)

0.1250 40.43(1.80) 40.81(1.74) 40.85(1.53) 41.35(1.50)

0.1500 40.14(1.77) 40.51(1.72) 40.47(1.51) 40.97(1.48)

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Table 4.5 (Continued)

mS / mol kg-1

Sk 1011(Pa-1)

303.15 K 308.15 K 313.15 K 318.15 K

(V/V-60%W + 40%M)

0.0000 44.12(2.00) 44.45(1.96) 44.71(1.60) 45.02(1.58)

0.0500 43.09(1.94) 43.45(1.91) 43.66(1.55) 43.95(1.53)

0.0750 42.67(1.91) 43.02(1.88) 43.18(1.53) 43.48(1.51)

0.1000 42.29(1.89) 42.64(1.85) 42.75(1.51) 43.04(1.49)

0.1250 41.91(1.86) 42.28(1.83) 42.32(1.49) 42.62(1.47)

0.1500 41.59(1.84) 41.94(1.81) 41.92(1.47) 42.21(1.45)

(V/V-50%W + 50%M)

0.0000 45.95(1.96) 46.68(1.89) 47.48(1.70) 48.50(1.78)

0.0500 44.84(1.90) 45.61(1.84) 46.36(1.65) 47.35(1.73)

0.0750 44.40(1.87) 45.16(1.81) 45.87(1.63) 46.84(1.70)

0.1000 43.95(1.85) 44.76(1.79) 45.40(1.60) 46.38(1.68)

0.1250 43.55(1.82) 44.38(1.77) 44.97(1.58) 45.94(1.66)

0.1500 43.19(1.80) 44.00(1.74) 44.56(1.56) 45.56(1.64)

mS - stands for molal concentration of salbutamol sulphate

Parenthesis indicates uncertainty of ks.

The change Sk and relative change ( 0/ SS kk ) in isentropic

compressibility are calculated by using the equations from 1.19–1.22 and are

listed in Tables 4.6 and 4.7.

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Table 4.6 Sk –Change in Isentropic Compressibility of Salbutamol

Sulphate in Aqueous Methanol Solution at Different

Temperatures

mS / mol kg-1

Sk 1011(Pa-1)

303.15 K 308.15 K 313.15 K 318.15 K (V/V-90%W+10%M)

0.0500 0.961 0.982 0.999 1.021 0.0750 1.377 1.387 1.436 1.475 0.1000 1.766 1.731 1.835 1.886 0.1250 2.077 2.122 2.201 2.268 0.1500 2.372 2.458 2.561 2.624

(V/V-80%W+20%M) 0.0500 1.027 0.963 0.989 1.010 0.0750 1.441 1.375 1.427 1.439 0.1000 1.837 1.744 1.829 1.821 0.1250 2.208 2.099 2.192 2.213 0.1500 2.584 2.459 2.555 2.569

(V/V-70%W+30%M) 0.0500 0.958 0.981 1.030 1.037 0.0750 1.380 1.380 1.455 1.498 0.1000 1.718 1.722 1.815 1.916 0.1250 2.092 2.044 2.254 2.315 0.1500 2.383 2.344 2.633 2.691

(V/V-60%W+40%M) 0.0500 1.025 1.004 1.057 1.075 0.0750 1.447 1.435 1.529 1.547 0.1000 1.833 1.812 1.963 1.980 0.1250 2.206 2.173 2.389 2.406 0.1500 2.535 2.511 2.788 2.815

(V/V-50%W+50%M) 0.0500 1.110 1.064 1.124 1.153 0.0750 1.555 1.517 1.613 1.662 0.1000 2.004 1.916 2.080 2.122 0.1250 2.399 2.301 2.509 2.558 0.1500 2.762 2.682 2.922 2.943

mS- stands for molal concentration of salbutamol sulphate

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Table 4.7 0/ SS kk -Relative Change in Isentropic Compressibility of

Salbutamol Sulphate in Aqueous Methanol Solution at

Different Temperatures

mS / mol kg-1

0/ SS kk 102

303.15 K 308.15 K 313.15 K 318.15 K (V/V-90%W+10%M)

0.0500 2.285 2.350 2.401 2.459 0.0750 3.304 3.351 3.487 3.592 0.1000 4.278 4.217 4.500 4.641 0.1250 5.068 5.216 5.446 5.632 0.1500 5.831 6.095 6.393 6.574

(V/V-80%W+20%M) 0.0500 2.486 2.329 2.403 2.457 0.0750 3.525 3.357 3.503 3.536 0.1000 4.539 4.297 4.536 4.519 0.1250 5.505 5.217 5.485 5.545 0.1500 6.504 6.166 6.453 6.495

(V/V-70%W+30%M) 0.0500 2.307 2.344 2.449 2.432 0.0750 3.354 3.326 3.492 3.553 0.1000 4.209 4.186 4.396 4.588 0.1250 5.174 5.008 5.517 5.598 0.1500 5.936 5.785 6.505 6.567

(V/V-60%W+40%M) 0.0500 2.379 2.311 2.421 2.446 0.0750 3.391 3.335 3.539 3.557 0.1000 4.334 4.250 4.592 4.599 0.1250 5.263 5.140 5.645 5.646 0.1500 6.095 5.986 6.649 6.668

(V/V-50%W+50%M) 0.0500 2.474 2.333 2.424 2.434 0.0750 3.502 3.359 3.516 3.548 0.1000 4.559 4.281 4.582 4.575 0.1250 5.508 5.185 5.579 5.568 0.1500 6.394 6.096 6.558 6.459

mS- stands for molal concentration of salbutamol sulphate

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The apparent molal compressibility k values of salbutamol

sulphate in aqueous methanol solution are obtained using the equation 1.23

and are listed in Table 4.8. The error values for apparent molal

compressibility are evaluated using equation 1.2 and are given in Table 4.8

within parenthesis.

Table 4.8 Apparent Molal Compressibility, K of Salbutamol

Sulphate in Aqueous Methanol Solution at Different

Temperatures

mS / mol kg-1

K 1015 (m3 mol-1 Pa-1 )

303.15 K 308.15 K 313.15 K 318.15 K

(V/V-90%W+10%M)

0.0500 12.60(0.06) 12.82(0.09) 8.455(0.10) 6.487(0.10)

0.0750 12.01(0.03) 9.334(0.04) 7.191(0.05) 6.817(0.05)

0.1000 11.86(0.02) 5.363(0.03) 5.998(0.03) 5.901(0.03)

0.1250 10.44(0.01) 9.784(0.02) 4.055(0.02) 5.099(0.03)

0.1500 10.42(0.01) 8.756(0.02) 3.560(0.02) 4.909(0.02)

(V/V-80%W+20%M)

0.0500 28.16(0.08) 10.79(0.08) 8.26(0.09) 6.79(0.10)

0.0750 18.91(0.04) 9.22(0.04) 6.92(0.05) 3.62(0.05)

0.1000 18.76(0.02) 7.71(0.02) 5.46(0.03) 5.44(0.03)

0.1250 17.35(0.02) 7.84(0.02) 3.51(0.02) 0.76(0.03)

0.1500 17.48(0.01) 7.79(0.01) 2.96(0.02) 0.82(0.02)

(V/V-70%W+30%M)

0.0500 9.14(0.07) 10.64(0.07) 11.54(0.10) 5.72(0.10)

0.0750 9.09(0.04) 6.96(0.04) 6.13(0.05) 5.03(0.05)

0.1000 8.93(0.02) 4.39(0.02) 0.53(0.03) 4.05(0.03)

0.1250 8.87(0.02) 2.23(0.02) 4.94(0.02) 3.62(0.03)

0.1500 7.57(0.01) 0.70(0.01) 5.20(0.02) 3.32(0.02)

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Table 4.8 (Continued)

mS / mol kg-1

K 1015 (m3 mol-1 pa-1 )

303.15 K 308.15 K 313.15 K 318.15 K

(V/V-60%W+40%M)

0.0500 15.26(0.08) 7.19(0.08) 6.49(0.11) 6.05(0.11)

0.0750 14.20(0.04) 6.98(0.04) 5.05(0.05) 3.62(0.06)

0.1000 12.84(0.03) 6.74(0.03) 3.14(0.04) 1.61(0.04)

0.1250 12.61(0.02) 6.41(0.02) 3.47(0.03) 1.26(0.03)

0.1500 12.43(0.02) 6.11(0.02) 2.76(0.02) 1.17(0.02)

(V/V-50%W+50%M)

0.0500 21.92(0.09) 6.40(0.09) 5.91(0.11) 5.02(0.11)

0.0750 16.02(0.05) 3.57(0.04) 1.85(0.05) 2.75(0.05)

0.1000 15.84(0.03) 0.78(0.03) 0.50(0.04) 0.38(0.04)

0.1250 15.29(0.02) 0.44(0.02) 0.82(0.03) 0.17(0.03)

0.1500 14.95(0.02) 0.36(0.02) 0.32(0.02) 0.29(0.02)

mS- stands for molal concentration of salbutamol sulphate

Parenthesis indicates standard errors

The partial molal compressibility 0k of homologous amino acids

are evaluated using the least square fit of equation 1.24. The evaluated values

of 0k and SK are listed in Table 4.9.

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Table 4.9 Partial Molal Compressibility, 0K and Experimental

Slope, SK, of Salbutamol Sulphate in Aqueous Methanol

Solution at Different Temperatures

T/K 0K 1015

(m3 mol-1 Pa-1)

SK1017

(m3 mol-2 kg Pa-1)

(V/V-90%W+10%M) 303.15 13.83(0.43) 2.37 308.15 12.29(0.36) 3.01 313.15 11.02(0.46) 5.17 318.15 7.79(0.50) 1.95

(V/V-80%W+20%M) 303.15 29.30(0.40) 9.17 308.15 11.62(0.10) 2.95 313.15 11.03(0.48) 5.61 318.15 8.44(0.21) 5.92

(V/V-70%W + 30%M) 303.15 10.07(0.58) 1.34 308.15 14.83(0.98) 9.84 313.15 12.22(0.05) 5.54 318.15 6.84(0.31) 2.48

(V/V-60%W + 40%M) 303.15 16.36(0.64) 2.89 308.15 7.79(0.059) 1.10 313.15 7.81(0.95) 3.62 318.15 7.59(0.13) 4.84

(V/V-50%W+50%M) 303.15 22.67(0.26) 5.86 308.15 8.39(0.17) 6.08 313.15 6.77(0.20) 4.88 318.15 6.54(0.14) 4.81

W - stands for Water M - stands for methanol

Parenthesis indicates standard error

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In order to support the results obtained from volumetric and

compressibility data, the viscosity data have been obtained for all binary

solutions at the reported temperatures and values are given in Table 4.10. The

uncertainty values for viscosity are evaluated and are given in the same

Table 4.10.

Table 4.10 Viscosities of Salbutamol Sulphate in Aqueous Methanol

Solution at Different Temperatures

mS / mol kg-1

(mPa s)

303.15 K 308.15 K 313.15 K 318.15 K

(V/V-90% W + 10%M)

0.0000 0.961 0.853 0.764 0.691

0.0500 1.009 0.969 0.812 0.762

0.0750 1.050 1.011 0.874 0.792

0.1000 1.094 1.051 0.909 0.820

0.1250 1.142 1.099 0.943 0.861

0.1500 1.200 1.137 0.965 0.896

=3.310-3 =4.110-3 =3.110-3 =2.910-3

(V/V-80% W + 20%M)

0.0000 1.091 0.991 0.885 0.790

0.0500 1.140 1.114 0.977 0.864

0.0750 1.188 1.160 1.016 0.898

0.1000 1.245 1.209 1.057 0.931

0.1250 1.305 1.259 1.105 0.967

0.1500 1.353 1.309 1.151 1.021

=4.110-3 =4.610-3 =3.810-3 =3.210-3

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Table 4.10 (Continued)

mS / mol kg-1

(mPa s)

303.15 K 308.15 K 313.15 K 318.15 K

(V/V-70%W + 30%M)

0.0000 1.211 1.108 0.978 0.871

0.0500 1.246 1.216 1.073 0.948

0.0750 1.285 1.268 1.114 0.983

0.1000 1.344 1.328 1.161 1.023

0.1250 1.421 1.387 1.210 1.070

0.1500 1.482 1.435 1.265 1.116

=4.210-3 =4.810-3 =4.110-3 =3.510-3

(V/V-60%W+40%M)

0.0000 1.317 1.227 1.056 0.965

0.0500 1.352 1.290 1.102 1.003

0.0750 1.359 1.356 1.151 1.045

0.1000 1.450 1.412 1.202 1.091

0.1250 1.553 1.482 1.240 1.137

0.1500 1.582 1.528 1.314 1.189

=4.510-3 =4.610-3 =3.810-3 =3.210-3

(V/V-50%W+50%M)

0.0000 1.370 1.305 1.135 1.014

0.0500 1.396 1.328 1.153 1.033

0.0750 1.418 1.398 1.213 1.077

0.1000 1.496 1.460 1.266 1.130

0.1250 1.568 1.516 1.311 1.174

0.1500 1.659 1.584 1.376 1.225

=4.510-3 =4.410-3 =3.810-3 =3.310-3

mS- stands for molal concentration of salbutamol sulphate

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Using the linear plots of r versus C (Figure 4.2) the viscosity

B-coefficients are evaluated by the least squares method of equation 1.28.

The evaluated values of B- coefficients are given in Table 4.11.

0.9

1

1.1

1.2

1.3

1.4

0.00 0.05 0.10 0.15

C / (mol.dm-3)

η r

Figure 4.2 Plot of Relative Viscosity ( r ) Against Molarity (C) of

Salbutamol Sulphate in Aqueous Methanol (90%W+10%

M) at (♦) 303.15 K, (■) 308.15 K

The data of B-coefficient of the solutions are used to estimate mean

volume of the solvent, the free energy of activation per mole of the solute

)( *02 and solvent )( *0

1 using equations 1.29, 1.31 and 1.32 and values are

given in Table 4.11.

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Table 4.11 Viscosity B-Coefficients, Mean Volume of Solvent 01V

Activation Free Energy of Solvent *01

and Solute *02 of

Salbutamol Sulphate in Aqueous Methanol Solution at Different Temperatures

T/K B- Coeff 103

(m3 mol-1)

01V 106

(m3 mol-1)

*01

(kJ mol-1)

*02

(kJ mol-1)

(V/V-90%W+10%M) 303.15 2.184(0.079) 18.27 26.949 325.733 308.15 2.179(0.039) 18.28 27.087 330.033 313.15 2.171(0.227) 18.33 27.247 333.093 318.15 2.169(0.100) 18.37 27.425 337.099

(V/V-80%W+20%M) 303.15 2.191(0.052) 18.42 27.288 324.804 308.15 2.187(0.030) 18.48 27.501 328.183 313.15 2.180(0.070) 18.52 27.658 331.605 318.15 2.176(0.136) 18.58 27.809 335.037

(V/V-70%W+30%M) 303.15 2.232(0.140) 18.79 27.602 324.570 308.15 2.230(0.048) 18.79 27.830 330.161 313.15 2.229(0.086) 18.80 27.958 334.127 318.15 2.210(0.088) 18.89 28.114 334.855

(V/V-60%W+40%M) 303.15 2.254(0.333) 19.08 27.853 323.052 308.15 2.240(0.073) 19.09 28.133 326.389 313.15 2.237(0.140) 19.14 28.205 329.908 318.15 2.226(0.055) 19.19 28.425 332.648

(V/V-50%W+50%M) 303.15 2.282(0.250) 19.34 27.986 322.956 308.15 2.242(0.044) 19.37 28.326 322.539 313.15 2.241(0.071) 19.41 28.428 326.445 318.15 2.229(0.042) 19.49 28.595 328.552

W - stands for Water M – stands for methanol

Parenthesis indicates standard error

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4.4 DISCUSSION

It is observed from Table 4.1, that the density of ternary system

increases with an increase in concentration of salbutamol sulphate. This may

be attributed to the shrinkage in the volume which in turn is due to the

presence of the solute / drug. In other words, the increase in density may be

interpreted due to the enhanced structure of the solvent mixture due to the

added drug (Sharma et al. 2008). Partial molal volume 0V (Table 4.3) are

positive in aqueous methanol solution indicating the presence of strong

drug-solvent interactions between the molecules, and the structure making

effect of salbutamol sulphate in aqueous methanol solution (Sharma et al.

2008). Further it is seen from Table 4.3, that 0V values increase with increase

in temperature. The variation of 0V values with temperature may be

explained based on scaled particle theory (Gurney 1954) as discussed in

Chapter 3.

It is further seen from Table 4.3, that sV shows negative values at all

the studied temperatures. sV is the measure of solute-solute interaction and

depends on charge, nature of solute and solvent respectively. The negative

values of sV indicate the presence of weak solute-solute interactions in the

solution (Ali et al 2002).

It is further attributed to the fact that in solvent of high dielectric

constant like water, the solutes remain completely ionized even at fairly high

concentration. Similar observations have been reported by Parmar et al

(2004) of Citric acid and Tartaric acid in binary aqueous mixtures of ethanol

at various temperatures using the negative Sv values. However, at a particular

temperature, with the increase of methanol content in aqueous methanol

solution, 0V increases thereby showing that solute-solvent interactions

improve on the addition of more and more methanol in water

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(Parmar et al 2004). From Table 4.3, it is seen that the values of partial molal

expansivity 02E are positive indicating that the drug acts as a structure maker

(Iqbal and Chaudhry 2009a). Further they indicate the predominance of

hydrophobic hydration over the electrostriction of water methanol molecules

around the solute molecules.

Furthermore, the isobaric thermal expansion coefficient )( 2

(Table 4.3) shows a decreasing behaviour with increasing temperature in

aqueous methanol solution studied in the present work, because when the

temperature is increased the density of the solution decreased (Table 4.1),

resulting in a decrease in partial molal expansivity coefficient )( 2 . A similar

trend was reported by Iqbal and Siddiquah (2006) in mafenamic acid alcohol.

The positive values of Hepler’s constant i.e., 202 / TV (Table 4.3)

indicate the structure making ability of the solute in aqueous methanol

solution (Iqbal and Chaudhry 2009b). From Table 4.4 it is observed that

ultrasonic speed increases with increase in temperature. An increase in the

ultrasonic velocity in any solution with the addition of a solute is indicative of

greater association of molecules due to effective solute-solvent interactions

(Syal et al 1998). Isentropic compressibility Sk decreases with increase in

concentration of methanol and temperature. This decrease in compressibility

values may be viewed as follows. Water is regarded as an equilibrium mixture

of two structures such as an ice –like structure and a close packed structure

(Hall 1948, Arakawa and Sasaki 1969).Compressibility of liquid water is

given by sk = k + )1/( 22Tk relax , where k is an instantaneous part of

compressibility and relaxk , a relaxational part of compressibility (Hall 1948).

The relaxation time corresponding to relaxk is of the order of 10-11s. The

relation <<1 holds good in the present experiment, where is the

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angular frequency. Thus the isentropic compressibility obtained is equal to

( k + relaxk ). With rise in temperature, k increases due to thermal expansion,

and relaxk , decreases due to thermal rupture of the ice-like structure. Thus the

decrease in isentropic compressibility values with increase in temperature

may be attributed to the corresponding decrease in relaxk , which is dominant

over the corresponding increase in k . Hirata and Arakawa (1972) gave

similar conclusion for aqueous solutions of Tetraalkylammonium salts.

From Tables 4.6 and 4.7, it is seen that sk and 0/ ss kk increases

with increase in drug concentration and temperature (Figures 4.3 and 4.4

respectively). This may be attributed to an increase in the incompressible part

in the solution. The variation of the change and relative change in isentropic

compressibility values with temperature may be attributed to thermal rupture

of water structure. A close observation of plots of sk and 0/ ss kk versus

salbutamol sulphate concentration (Figures 4.3 and 4.4) indicate that the

intercept values for all the systems (% of methanol) are zero or close to

zero.Such a behaviour supports the strong solute – solvent intermolecular /

interionic interactions in these systems. Similar trends were reported in

electrolyte systems (Riyazudeen and Bansal 2006).

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96

0

0.5

1

1.5

2

2.5

3

0.04 0.06 0.08 0.10 0.12 0.14 0.16m / (mol.kg-1)

βS(1

0-11 P

a-1)

Figure 4.3 Plot of Change in Isentropic Compressibility ( sk ) against

Molal Concentration ( m ) of salbutamol Sulphate in

(♦) 303.15K, (■) 308.15 K, (▲) 313.15 K, (Δ) 318.15 K of

(90%W + 10%M)

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97

0

1

2

3

4

5

6

7

0.04 0.06 0.08 0.10 0.12 0.14 0.16

m / (mol.kg-1)

Δβ s

/ β

S0 (1

0-2)

Figure 4.4 Plot of Relative Change in Isentropic Compressibility

( 0/ ss kk ) Against Molal Concentration ( m ) of SBS in

(♦) 303.15 K, (■) 308.15 K, (▲) 313.15 K, (Δ) 318.15 K of

(90%W + 10%M)

It is well known that ionic groups of solute attract strongly

surrounding water molecules called electrostriction which causes a large

decrease both in volume and incompressibility of the aqueous methanol

solutions. Since the partial molal compressibility is a more sensitive measure

of solute - solvent interactions than in the partial molal volume (Hoiland

1986), the effect of electrostriction is more obvious for the former

thermodynamic property. As seen from Table 4.9, the values of partial molal

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compressibilities 0K are negative at all mixed volume systems and

temperatures studied, thereby showing the presence of strong solute-solvent

interactions. Further the compressibility decreases steeply with decrease of

temperature, that is the characteristic for dilute aqueous solutions regardless

of whether they are hydrophilic or hydrophobic solutes (Kikuchi 1995).

Similar conclusions were drawn by Yasuda et al (1988) for several aqueous

mono hydrochlorides. The positive values of sk further support the weak

solute-solute interaction in mixed solutions.

It is further seen from Table 4.10, that viscosity values increase

with increase in concentration of salbutamol sulphate, when a solute is

dissolved in a solvent some of the solvent molecules are attracted to the solute

as the result of solute-solvent interaction and thus increase the solution

viscosity. Generally, the increase in viscosity of the solution on addition of

solute indicates the structure-making aspects of solutes (Iqbal and Chaudhry

2008). The relative viscosity values of the solutions decrease with an increase

in temperature. The increase in temperature may have caused the increase in

the kinetic energy of molecules and ions present in the solution, which in turn,

decreases, the solute-solvent interactions (Riyazuddeen and Imrankhan 2008).

The viscosity B-coefficients provide information about the salvation of the

solutes and their effects on the structure of the solvent in the near

environment of the solute molecule. Further some activation parameters of

viscous flow can be obtained using B-coefficients (Jenkins and Marcus 1995).

The viscosity B-coefficients (Table 4.11) originally introduced as an

empirical term has been found to depends upon solute-solvent interactions

and on the relative size of the solute and solvent molecules, are positive

indicating the strong solute-solvent interactions in addition to the

structure-making ability of the solute (Sharma and Ahluwalia 1973).

Furthermore, from Table 4.11, it is clear that with increase of temperature the

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99

values of B-coefficient of the solution decrease (Figure 4.5). Thus dB/dT is

negative in the case of salbutamol sulphate and acts a structure maker in these

solutions, thereby, complimenting the volumetric and compressibility

conclusions.

2.165

2.17

2.175

2.18

2.185

2.19

2.195

300.00 305.00 310.00 315.00 320.00

T / K

B-c

oeff

/(10-3

m3 .m

ol-l )

Figure 4.5 Variation of Viscosity B-Coefficient against Temperature of

SBS in (♦)10%,(■)20% of Aqueous Methanol

From Table 4.11, it is clear that *02 and *0

1 increases with

increase in concentration of methanol content in aqueous methanol solution. It

is further seen that *02 > *0

1 thus indicating the structure-making ability of

the solute and strong solute-solvent interactions (Ali et al 2002, Mishra et al

2001). In other words the formation of the transition state is accompanied by

the rupture and distortion of intermolecular forces in solvent structure.