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IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 1 | Jan-2015, Available @ http://www.ijret.org 96
INVESTIGATION OF MOLECULAR INTERACTION OF AMINO
ACIDS IN AQUEOUS n-PROPANOL SOLUTIONS AT 308.15 K
Richard D’ Souza1
G. Meenakshi2
1
Research Scholar, Department of Physics, Bharathiyar University, Coimbatore, Tamil Nadu, India.
2
Associate Professor (Rtd), Department of Physics, Kanchimamunivar Center for PG Studies, Pondicherry, India
Abstract
The physical properties that has been investigated are, density (ρ),viscosity (η), and ultrasonic velocity (U) of L-valine,
L- leucine and L-glutamine in aqueous n-propanol solution (0%-30%) in steps of 10% at 308.15K have been measured. The
derived acoustical parameters namely adiabatic compressibility (β), apparent molal compressibility (ϕK), apparent molal volume
(ϕV), limiting apparent molal compressibility(ϕ°K), limiting apparent molal volume(ϕ°V) and their constants (sk, sv), transfer
adiabatic compressibility (Δϕ°K), transfer volume(Δϕ°V) , and viscosity B-coefficient are calculated using the experimental data.
The change that has been observed in the parameter with respect to molality of the solute has been interpreted in terms of ion-ion
and ion- solvent interactions.
Key words: Molecular interaction, solute-solvent interaction, ion-ion interaction, ion-solvent interaction.
--------------------------------------------------------------------***----------------------------------------------------------------------
1. INTRODUCTION
In recent years, the Physicist wished to understand the
structure of liquid molecules. The only means they had of
investigating these structures were by chemical reaction that
led to the changes which themselves were known. The
liquids and liquid mixtures help chemical physicist to
explore the “dynamic behavior” of rigid molecules, using
both physical and chemical methods. Denaturation of
globular proteins in aqueous solutions is a fundamental
biological process which till date is not completely
understood and continues to be a subject of extensive
investigations [1]. Knowledge of various solute-solute and
solute-solvent interactions is very important to understand
various fundamental phenomena like stability of proteins,
folding/unfolding processes, denaturation of proteins etc., in
aqueous solutions [2]. It is rather difficult to study the
interaction of protein molecules because it has got a nature
of complex structure. It is quite interesting to study the
physio- chemical behavior of the non-electrolyte like
propanol with amino acids [3].
The physical properties of dilute aqueous solutions of non-
electrolytes depend on the solute and solvent i.e., water
whose structure acts as breaker or maker. The influence of
small quantity of amino acids over the hydrogen bonded
structure of water in the solution may expect to yield good
results. It will also help to study the nature of molecular
interactions between the organic solute with water which act
as a solvent [4].
2. MATERIALS AND METHODS
In the present study, the spectroscopic reagent (SR) and
analytical reagent (AR) grades of minimum assay of 99.9%
are used and obtained from E-Merck, Germany and Sd Fine
chemicals, India. Water used in the experiment was
deionized, distilled and are degassed to making solutions.
An aqueous solution of n-propanol 0% - 30 % mol. dm-3
in
steps of 10 % is prepared by volume and has been used for
the present study. The amino acids in the concentration
range of 0.02 - 0.1 mol dm-3
has been made by volume on
the molality concentration with a precision of ± 1×10-4
g on
an electronic digital balance (Model: Shimadzu Ax - 200).
The density has been measured by using the relative
measurement method with an accuracy of ± 0.01 kg m-3
, and
obtained by using a specific gravity bottle. An Ostwald’s
viscometer (5ml) has been used for the viscosity
measurements. Efflux time has been determined using a
digital chronometer within ± 0.01 s. For velocity
measurements, Ultrasonic interferometer having a frequency
of 3 MHz (Mittal Enterprises, New Delhi, Model: F-18)
with an overall accuracy of 0.1% has been used. A digital
electronic constant temperature bath has been used for
experimental purpose. The accuracy of the temperature
measurement is ± 0.1 K.
3. RESULT AND DISCUSSION
The values of ultrasonic velocity (U), density (ρ), and
viscosity (η), for different molar concentrations of L- valine,
L-leucine and L-glutamine in aqueous n-propanol (0% -
30%) M solution at 308.15K is reported in Table1. The
values of adiabatic compressibility (β), apparent molal
compressibility (ϕk), apparent molal volume (ϕv), limiting
apparent molal compressibility (ϕ°k), limiting apparent
molal volume (ϕ°v) their constants (Sk, Sv), are reported in
Table 2, 3. The volumetric, compressibility and transport
parameter have been calculated using the standard relations,
Adiabatic compressibility
β = (1)
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 1 | Jan-2015, Available @ http://www.ijret.org 97
The apparent molar compressibility
φk = ( o - ) +
(2)
where, M is the molal concentration of the solute and Mw
the molecular weight of the solute. φk is the function of M as
obtained by Gucker (1993) [5] from Debye Huckel [6] and
is given by
φk = φo
k + Sk M 1/2
(3)
where, φo
k is the limiting apparent molar compressibility and
Sk is a constant.
The apparent molar volume φv
φv = -
(4)
The apparent molar volume φv in according to
empirical relation as:
φv = φo
v + Sv M 1/2
(5)
where, φo
v is the limiting apparent molar volume and Sv is a
constant. The constant values have been evaluated by least
square method.
The viscosity A and B coefficients has been calculated from
the Jones - Dole equation [7].
= 1+ AM 1/2
+BM (6)
where, η and ηo are the viscosities of the solution and
solvent respectively.
Transfer adiabatic compressibility (Δφo
k) and transfer
volume (Δφo
v) have been calculated as:
Δφo
y = φo
y (in aqueous n-propanol solution) - φo
y
(in water) (7)
Where, φo
y denotes limiting apparent molar compressibility
φo
k, limiting apparent molar volume φo
v.
Table – 1: Density (), viscosity () and ultrasonic velocity ( U) of the amino acids in aqueous solutions of n-propanol
at 308.15 K
M
(mol.dm–3
)
/(kg.m–3
) /(×10–3
Nsm–2
) U/(x10-10
m.s–1
)
Water + n-Propanol + L-valine
0% 10% 20% 30% 0% 10% 20% 30% 0% 10% 20% 30%
0.00 994.0 980.1 966.2 952.9 0.7190 0.9614 1.0576 1.2861 1519.5 1537.6 1555.2 1575.7
0.02 994.7 981.0 967.3 954.2 0.8060 0.9926 1.0760 1.3062 1520.6 1540.2 1558.0 1579.2
0.04 995.5 982.2 968.8 955.2 0.8296 1.0001 1.0870 1.3322 1524.7 1542.6 1560.5 1584.2
0.06 996.5 983.6 970.4 957.2 0.8578 1.0128 1.1005 1.3516 1527.4 1545.0 1562.8 1586.2
0.08 997.8 985.1 971.9 959.0 0.8827 1.0255 1.1251 1.3878 1530.8 1547.8 1565.3 1590.3
0.10 999.2 986.8 973.6 960.8 0.9113 1.0360 1.1595 1.4044 1535.2 1552.3 1570.1 1594.2
Water + n-Propanol + L-Leucine
0.00 994.0 980.1 966.2 952.9 0.7190 0.9614 1.0576 1.2861 1519.5 1537.6 1555.2 1575.7
0.02 996.7 983.4 971.0 958.7 0.7943 0.9711 1.1208 1.3292 1523.9 1540.9 1559.6 1579.1
0.04 998.2 985.4 973.0 960.6 0.8046 0.99s45 1.1372 1.3713 1526.6 1543.7 1562.2 1585.3
0.06 999.9 987.0 974.8 962.6 0.8122 1.0050 1.1530 1.3873 1529.1 1546.7 1565.0 1588.9
0.08 1001.6 989.2 976.8 964.4 0.8301 1.0274 1.1705 1.4059 1530.8 1549.7 1567.6 1593.2
0.10 1002.9 990.6 978.3 966.0 0.8360 1.0581 1.1839 1.4440 1533.9 1552.4 1570.9 1594.5
Water + n-Propanol + L-Glutamine
0.00 994.0 980.1 966.2 952.9 0.7190 0.9614 1.0576 1.2861 1519.5 1537.6 1555.2 1575.7
0.02 997.2 984.6 972.0 959.4 0.7996 0.9711 1.2765 1.5215 1523.5 1542.3 1559.9 1579.8
0.04 998.3 985.8 973.3 960.8 0.8061 0.9842 1.3012 1.5423 1526.3 1545.0 1563.7 1586.2
0.06 1000.3 987.6 975.4 963.2 0.8161 1.0006 1.3068 1.5623 1529.6 1548.3 1567.0 1589.4
0.08 1002.2 990.0 977.8 965.6 0.8343 1.0156 1.3197 1.5754 1532.3 1551.9 1570.4 1592.2
0.10 1003.1 991.3 979.5 967.7 0.8537 1.0289 1.3397 1.5948 1535.2 1554.3 1573.4 1594.3
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 1 | Jan-2015, Available @ http://www.ijret.org 98
The density (ρ) increases with increase of molal
concentration of amino acids and decreases with increase of
concentration of n-propanol (Table 1), the values of
ultrasonic velocity increase with increase in molal
concentration of amino acids and also with n-propanol
content. The observed results suggest a moderate strong
electrolytic nature in which the solutes tend to attract the
solvent molecules in the aqueous solution.
When amino acids are dissolved the water structure
is disturbed initially, followed by a structural reorganization
leaving the molecules in closely fitting helical cavities [8].
This will increase the density structure of water. Hence the
density of medium is affected. The increase in the ultrasonic
velocity may be attributed to the cohesion brought about by
the hydration. When the amino acids are dissolved in
aqueous alcohol, the cations NH3
+
and anions COO-
are
formed. The water molecules are attached to the ions
strongly by the electrostatic forces which introduce a greater
cohesion in the solution. The cohesion effect of medium
generally increases with the increase of amino acid
concentration. The increased associations observed in these
solutions, may also be due to water structure enhancement
brought by the increase of electrostriction in the presence of
n-propanol.
The adiabatic compressibility (β) (Table-2)
decreases with increase in the concentration of amino acids
and also with the n-propanol content.
The decrease in adiabatic compressibility is
attributed to the influence of the electrostatic field of ions
(NH3
+
and COO-
) on the surrounding solvent molecules
(C3H7
+
, OH-
).
The other observed results are on (ϕk) and (ϕv) (Table 2) of
L-valine, L-leucine and L-glutamine in aqueous n-propanol
solutions at 308.15K has been summarized as follows.
(i) All (ϕk) and (ϕv) values are negative over the entire
system.
(ii) With increase in concentration of amino acids as
well as n-propanol in system-I the values of (ϕk)
and (ϕv) decreases. For system II and II the
values of (ϕk) and (ϕv) increases with increase in
concentration of amino acid but decreases with
the increase in concentration of n-propanol.
(iii) For (ϕk) and (ϕv) values the magnitude are in the
order L-valine > L-leucine > L-glutamine.
Table - 2 : Values of adiabatic compressibility ( β ), apparent molar compressibility ( φk ) and apparent molar
volume ( φv) of amino acids in aqueous n-propanol solutions at 308.15 K.
M
(mol.
dm–3
)
β / ( x 10-10
m2
N-1
) -φk / (x 10-7
m2
N-1
) - φv / ( x 10-3
m3
mol-1
)
0% 10% 20% 30% 0% 10% 20% 30% 0% 10% 20% 30%
System - I Water + n-Propanol + L-valine
0.00 4.3572 4.3156 4.2791 4.2267 -- -- -- -- -- --
0.02 4.3474 4.3012 4.2589 4.2023 0.6653 0.9621 1.2535 1.3546 35.28 46.68 58.72 71.36
0.04 4.3206 4.2785 4.2387 4.1714 1.0903 1.1586 1.2978 1.5266 37.78 54.41 69.31 76.74
0.06 4.3013 4.2591 4.2193 4.1522 1.1362 1.1985 1.3066 1.6006 41.95 60.39 71.53 78.44
0.08 4.2766 4.2369 4.1993 4.1226 1.2102 1.2424 1.3130 1.6394 47.78 64.61 75.75 83.31
0.10 4.2461 4.2050 4.1660 4.0950 1.2293 1.3570 1.4321 1.6407 52.23 69.15 78.55 86.16
System - II Water + n-Propanol + L-Leucine
0.00 4.3572 4.3156 4.2791 4.2267 -- -- -- -- -- --
0.02 4.3203 4.2827 4.2340 4.1828 2.0595 2.3715 3.3179 3.4813 136.13 171.05 255.67 317.30
0.04 4.2986 4.2585 4.2112 4.1422 1.9252 2.0109 2.4503 2.9665 105.69 131.06 180.69 210.16
0.06 4.2773 4.2351 4.1884 4.1148 1.7627 1.8480 2.1464 2.5820 98.80 118.74 152.04 176.11
0.08 4.2601 4.2094 4.1660 4.0850 1.6301 1.8283 2.0005 2.4088 95.28 117.19 140.25 156.28
0.10 4.2378 4.1888 4.1421 4.0712 1.5841 1.7303 1.9058 2.1360 89.14 108.01 127.87 142.17
System - III Water + n-Propanol + L-Glutamine
0.00 4.3572 4.3156 4.2791 4.2267 -- -- -- -- -- --
0.02 4.3204 4.2697 4.2280 4.1763 2.4513 3.2857 3.5430 3.9615 161.27 233.01 308.64 355.34
0.04 4.2999 4.2496 4.2019 4.1365 1.9037 2.2774 2.7161 3.1310 108.18 147.33 188.57 215.56
0.06 4.2761 4.2238 4.1752 4.1102 1.8119 2.0804 2.4107 2.7031 105.45 128.99 162.54 186.88
0.08 4.2493 4.1940 4.1469 4.0850 1.7980 2.0648 2.2946 2.4754 102.74 127.39 153.33 172.38
0.10 4.2298 4.1756 4.1239 4.0652 1.6728 1.8931 2.1410 2.2714 91.12 115.12 140.38 160.34
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 1 | Jan-2015, Available @ http://www.ijret.org 99
The negative values of (ϕk) and (ϕv) indicates ionic and
hydrophilic interactions occurring in these systems [10]. The
magnitude of (ϕk) strongly supports our earlier view of the
ultrasonic velocity and adiabatic compressibility. The
negative values of (ϕv) indicate electrostrictive solvation of
ions [11]. The value of (ϕv) shows that stronger molecular
association has been found in L-valine.
Hence L-valine is a more effective structure maker
than other two amino acids.
From Table 3, the changes observed in (ϕ°k) and (Sk) values
with increase of amino acids concentration may be due to
ion-solvent interaction and ion-ion interactions in the
solution. The values of (ϕ°k) are negative and it decreases
with increasing concentration of n-propanol in all the
systems studied. It confirms the existence of ion-solvent
interaction in the mixtures.
The magnitude of (ϕ°k) is in the order L-valine >
L-leucine > L-glutamine. The values of (Sk) is negative for
L-valine (Table 3), but it is positive for other two amino
acids. The negative values of (Sk) Indicate weakening of
ion-ion interaction and suggest the structure breaking effect
of the amino acids.
It is well known that solutes causing
electrostriction lead to decrease in compressibility of the
solution. This is reflected by the negative values of the (ϕk)
values of amino acids.
The volume behavior of the solute at infinite
dilution is satisfactorily represented by (ϕ°v), which is
independent of
the ion-ion interactions and provides information concerning
ion-solvent interactions. Table 3 reveals that the values of
(ϕ°v) are negative in all the three amino acids. From table 3,
(Sv) values are negative for L-valine and positive for the
other two amino acids. The negative (Sv) values for L-valine
suggest the presence of weak ion-ion interactions [12].
Therefore it causes the complex ion formation in the
systems. The values of transfer adiabatic compressibility
(Δϕ°k) and transfer volume (Δϕ°v) (Table 3) are negative and
it decreases with increasing concentration of n-propanol in
all the three amino acid systems. It suggests that the
existence of ion-solvent interaction in the mixtures.
Table - 3 Values of limiting apparent molal compressibility ( ), limiting apparent molal volume ( ), their constants
Sk and Sv, transfer adiabatic compressibility (Δ ) and transfer volume (Δ ) of the amino acids in aqueous
n-propanol solutions at 308.15 K
Amino
Acid
M/
(mol. Kg–1
)
– /
(×10-7
m2
N-1
)
– /
(×10-3
m3
mol-1
)
Sk /
(×10-7
N-1
m-1
mol-1
)
Sv / (×10-3
m3
L1/2
mol-3/2
)
Δ
/(×10-7
m2
N-1
)
Δ
/ (×10-3
m3
mol-1
)
A /
(dm3/2
.
mol-1/2
)
B / (dm3/2
.
mol-1
)
L-Valine
0% 0.3522 20.46 -3.0117 -95.06 - - 0.8210 -0.0349
10% 0.7044 29.11 -2.0216 -126.25 -0.3522 -8.65 0.1982 0.1168
20% 1.1286 45.41 -0.8096 -106.97 -0.7764 -24.95 -0.0384 0.9700
30% 1.1663 59.85 -1.6285 -81.62 -0.8141 -39.39 -0.0357 1.0517
L-Leucine
0% 2.4107 164.68 2.6080 251.72 - - 0.8746 -1.2209
10% 2.7867 209.04 3.4966 336.75 -0.376 -44.36 -0.1051 1.2781
20% 4.2240 338.96 7.8453 707.24 -1.8133 -174.28 0.4427 -0.2459
30% 4.5015 429.68 7.5367 969.18 -2.0908 -265.00 -0.1546 0.6913
L-Glutamine
0% 3.0022 197.5 4.4574 0.3534 - - 0.8882 -1.1238
10% 4.0460 297.7 7.2800 0.6226 -1.0438 -0.1002 -0.0500 0.8670
20% 4.4470 404.3 7.7035 0.9013 -1.4448 -0.2068 1.9129 -3.6004
30% 5.1630 467.1 9.5105 1.0505 -2.1608 -0.2696 1.6619 -3.0269
In the case of amino acids + n-propanol + water, when the
solute-cosolute molecules come close enough, their
cospheres overlaps and the following types of interactions
are possible:
(1) Ion-hydrophilic interactions occurring between
zwitterionic centers of amino acids and the –OH group
of n-propanol,
(2) Hydrophobic - hydrophilic interactions between
nonpolar parts of amino acids or n-propanol and –OH
group of n-propanol or zwitterionic centers of amino
acids, and
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
_______________________________________________________________________________________
Volume: 04 Issue: 1 | Jan-2015, Available @ http://www.ijret.org 100
(3) hydrophobic-hydrophobic interactions occurring
between the nonpolar parts of amino acids and the
nonpolar parts of n-propanol.
Anwar Ali [13] was also suggested the similar types of
interactions in the study of some amino acids with salts in
aqueous medium.
On the basis of co-sphere overlap model [14] the (Δϕ°v)
values can also be explained in terms of solute-cosolute
(ion-ion) interactions. According to this model, ion-ion
group interactions contribute positively whereas ion-non-
polar and non-polar-non-polar interactions contribute
negatively to the (Δϕ°v) values.
Therefore the negative values of (Δϕ°k) and (Δϕ°v) observed
in all the three amino acids showed that the interaction
contribution of type (ii) is stronger than that of type (i).
The study of Viscosity (η), helps to understand the
structure as well as molecular interactions occurring in the
solutions. It is observed that the values of viscosity increases
with increasing in solute concentration. This increasing
effect indicates the existence of ion-solvent interaction
occurring in these systems (Table 1).
Further to confirm the effect, the role of viscosity
(B) coefficient has been obtained from Jones-Dole equations
[15]. The (A) coefficient is negative and (B) coefficient is
positive for L-valine whereas a reverse trend is observed for
the other two amino acids (Table 3). Since there is a weak
ion-ion interaction is occurred in L-valine, because (A) is a
measure of ionic interaction, which is indicated by the
negative and smaller magnitude of (A) values [16] for L-
valine and vice-versa for the other two amino acids.
The viscosity (B) coefficient [17] gives the effect
of ion-solvent interactions on the solution viscosity. The
positive (B) values suggest the presence of strong ion-
solvent interactions vice-versa. The magnitude of (B) is in
the order L-valine > L-leucine > L-glutamine. The larger
value of (B) shows structure making capacity of the solute.
4. CONCLUSION
In summary, from the magnitudes of β, ϕk, ϕv and
viscosity B coefficient, it can be concluded that L-valine in
aqueous n-propanol solution possesses the strong ion-
solvent interaction than the other two amino acids. The
transfer volume (Δϕ°v) suggests an ionic hydrophobic group
interaction which predominates over the ionic hydrophilic
interactions and hydrophobic – hydrophobic interactions.
From the co-sphere overlap model it can be concluded that
ionic-hydrophobic interactions are dominating over the ion-
ion and hydrophobic – hydrophilic interactions.
REFERENCES
[1]. Hedwig G.R., HoilandH., J. Chem. Thermodyn., 23
(1999), 1029.
[2]. Lin Q., HuX., Lin L., SangW., LiS., J. Chem. Eng.
Data, 46 522 (2001).
[3]. Hackel M., HinzH., HeduringG. R., J. Mol. Bio. 66
429 (1999).
[4]. Kumar P., Kumar S., SinghS., GangwarR. S.,
Oriental J. of Chem. 2011. 27 No:2, 639 – 644.
[5]. Gucker, F.T., Chem.Rev.,13 (1993) 111
[6]. Debye, P., and Huckel, E., Z.Phys.,24 (1923) 305
[7]. Jones, A., and Dole, M., J.Am.Chem. Soc.,51(1929)
2950
[8]. Falkenhagen, H., and Vernon, E.L., Z.Phys.,33
(1932) 140
[9]. Kavanou J., water and solute water interactions
(Holden-Day Amsterdam) (1964).
[10]. Sandu J.S& Gurbis singh, J Ind. Chem. Soc., 65,
135 (1992).
[11]. Dhanalakshmi & Jasmin E, J. Pure. Appl.
Ultrasonics., 21, 79 (1999).
[12]. Biswajit Sinha, Bipulkumar Sarkar and
Mahendranath Roy. J. Chem. Thermodyn., 40, 394
(2008).
[13]. Anwar Ali, Shahla Khan, Soghra Hyder & Mohd
Tariq, J. Chem. Thermodyn, 39, 613 (2007).
[14]. Gurney R.W., Ionic process in solution chapter-I
(McGraw – Hill, New York) 1953.
[15]. Jones G., Dole M., J. Am. Chem. Soc., 51, 2950
(1929).
[16]. Man Singh, Maneesha Pandey, Rajeshkumar
Yadav., Verma H.S., J. Mol. Liq., 135. 188 (2007).
[17]. Millero F. J., LosurdoA., ShinC., J. Phys. Chem.,
82, 784 (1978).

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Investigation of molecular interaction of amino acids in aqueous n propanol solutions at 308.15 k

  • 1. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 1 | Jan-2015, Available @ http://www.ijret.org 96 INVESTIGATION OF MOLECULAR INTERACTION OF AMINO ACIDS IN AQUEOUS n-PROPANOL SOLUTIONS AT 308.15 K Richard D’ Souza1 G. Meenakshi2 1 Research Scholar, Department of Physics, Bharathiyar University, Coimbatore, Tamil Nadu, India. 2 Associate Professor (Rtd), Department of Physics, Kanchimamunivar Center for PG Studies, Pondicherry, India Abstract The physical properties that has been investigated are, density (ρ),viscosity (η), and ultrasonic velocity (U) of L-valine, L- leucine and L-glutamine in aqueous n-propanol solution (0%-30%) in steps of 10% at 308.15K have been measured. The derived acoustical parameters namely adiabatic compressibility (β), apparent molal compressibility (ϕK), apparent molal volume (ϕV), limiting apparent molal compressibility(ϕ°K), limiting apparent molal volume(ϕ°V) and their constants (sk, sv), transfer adiabatic compressibility (Δϕ°K), transfer volume(Δϕ°V) , and viscosity B-coefficient are calculated using the experimental data. The change that has been observed in the parameter with respect to molality of the solute has been interpreted in terms of ion-ion and ion- solvent interactions. Key words: Molecular interaction, solute-solvent interaction, ion-ion interaction, ion-solvent interaction. --------------------------------------------------------------------***---------------------------------------------------------------------- 1. INTRODUCTION In recent years, the Physicist wished to understand the structure of liquid molecules. The only means they had of investigating these structures were by chemical reaction that led to the changes which themselves were known. The liquids and liquid mixtures help chemical physicist to explore the “dynamic behavior” of rigid molecules, using both physical and chemical methods. Denaturation of globular proteins in aqueous solutions is a fundamental biological process which till date is not completely understood and continues to be a subject of extensive investigations [1]. Knowledge of various solute-solute and solute-solvent interactions is very important to understand various fundamental phenomena like stability of proteins, folding/unfolding processes, denaturation of proteins etc., in aqueous solutions [2]. It is rather difficult to study the interaction of protein molecules because it has got a nature of complex structure. It is quite interesting to study the physio- chemical behavior of the non-electrolyte like propanol with amino acids [3]. The physical properties of dilute aqueous solutions of non- electrolytes depend on the solute and solvent i.e., water whose structure acts as breaker or maker. The influence of small quantity of amino acids over the hydrogen bonded structure of water in the solution may expect to yield good results. It will also help to study the nature of molecular interactions between the organic solute with water which act as a solvent [4]. 2. MATERIALS AND METHODS In the present study, the spectroscopic reagent (SR) and analytical reagent (AR) grades of minimum assay of 99.9% are used and obtained from E-Merck, Germany and Sd Fine chemicals, India. Water used in the experiment was deionized, distilled and are degassed to making solutions. An aqueous solution of n-propanol 0% - 30 % mol. dm-3 in steps of 10 % is prepared by volume and has been used for the present study. The amino acids in the concentration range of 0.02 - 0.1 mol dm-3 has been made by volume on the molality concentration with a precision of ± 1×10-4 g on an electronic digital balance (Model: Shimadzu Ax - 200). The density has been measured by using the relative measurement method with an accuracy of ± 0.01 kg m-3 , and obtained by using a specific gravity bottle. An Ostwald’s viscometer (5ml) has been used for the viscosity measurements. Efflux time has been determined using a digital chronometer within ± 0.01 s. For velocity measurements, Ultrasonic interferometer having a frequency of 3 MHz (Mittal Enterprises, New Delhi, Model: F-18) with an overall accuracy of 0.1% has been used. A digital electronic constant temperature bath has been used for experimental purpose. The accuracy of the temperature measurement is ± 0.1 K. 3. RESULT AND DISCUSSION The values of ultrasonic velocity (U), density (ρ), and viscosity (η), for different molar concentrations of L- valine, L-leucine and L-glutamine in aqueous n-propanol (0% - 30%) M solution at 308.15K is reported in Table1. The values of adiabatic compressibility (β), apparent molal compressibility (ϕk), apparent molal volume (ϕv), limiting apparent molal compressibility (ϕ°k), limiting apparent molal volume (ϕ°v) their constants (Sk, Sv), are reported in Table 2, 3. The volumetric, compressibility and transport parameter have been calculated using the standard relations, Adiabatic compressibility β = (1)
  • 2. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 1 | Jan-2015, Available @ http://www.ijret.org 97 The apparent molar compressibility φk = ( o - ) + (2) where, M is the molal concentration of the solute and Mw the molecular weight of the solute. φk is the function of M as obtained by Gucker (1993) [5] from Debye Huckel [6] and is given by φk = φo k + Sk M 1/2 (3) where, φo k is the limiting apparent molar compressibility and Sk is a constant. The apparent molar volume φv φv = - (4) The apparent molar volume φv in according to empirical relation as: φv = φo v + Sv M 1/2 (5) where, φo v is the limiting apparent molar volume and Sv is a constant. The constant values have been evaluated by least square method. The viscosity A and B coefficients has been calculated from the Jones - Dole equation [7]. = 1+ AM 1/2 +BM (6) where, η and ηo are the viscosities of the solution and solvent respectively. Transfer adiabatic compressibility (Δφo k) and transfer volume (Δφo v) have been calculated as: Δφo y = φo y (in aqueous n-propanol solution) - φo y (in water) (7) Where, φo y denotes limiting apparent molar compressibility φo k, limiting apparent molar volume φo v. Table – 1: Density (), viscosity () and ultrasonic velocity ( U) of the amino acids in aqueous solutions of n-propanol at 308.15 K M (mol.dm–3 ) /(kg.m–3 ) /(×10–3 Nsm–2 ) U/(x10-10 m.s–1 ) Water + n-Propanol + L-valine 0% 10% 20% 30% 0% 10% 20% 30% 0% 10% 20% 30% 0.00 994.0 980.1 966.2 952.9 0.7190 0.9614 1.0576 1.2861 1519.5 1537.6 1555.2 1575.7 0.02 994.7 981.0 967.3 954.2 0.8060 0.9926 1.0760 1.3062 1520.6 1540.2 1558.0 1579.2 0.04 995.5 982.2 968.8 955.2 0.8296 1.0001 1.0870 1.3322 1524.7 1542.6 1560.5 1584.2 0.06 996.5 983.6 970.4 957.2 0.8578 1.0128 1.1005 1.3516 1527.4 1545.0 1562.8 1586.2 0.08 997.8 985.1 971.9 959.0 0.8827 1.0255 1.1251 1.3878 1530.8 1547.8 1565.3 1590.3 0.10 999.2 986.8 973.6 960.8 0.9113 1.0360 1.1595 1.4044 1535.2 1552.3 1570.1 1594.2 Water + n-Propanol + L-Leucine 0.00 994.0 980.1 966.2 952.9 0.7190 0.9614 1.0576 1.2861 1519.5 1537.6 1555.2 1575.7 0.02 996.7 983.4 971.0 958.7 0.7943 0.9711 1.1208 1.3292 1523.9 1540.9 1559.6 1579.1 0.04 998.2 985.4 973.0 960.6 0.8046 0.99s45 1.1372 1.3713 1526.6 1543.7 1562.2 1585.3 0.06 999.9 987.0 974.8 962.6 0.8122 1.0050 1.1530 1.3873 1529.1 1546.7 1565.0 1588.9 0.08 1001.6 989.2 976.8 964.4 0.8301 1.0274 1.1705 1.4059 1530.8 1549.7 1567.6 1593.2 0.10 1002.9 990.6 978.3 966.0 0.8360 1.0581 1.1839 1.4440 1533.9 1552.4 1570.9 1594.5 Water + n-Propanol + L-Glutamine 0.00 994.0 980.1 966.2 952.9 0.7190 0.9614 1.0576 1.2861 1519.5 1537.6 1555.2 1575.7 0.02 997.2 984.6 972.0 959.4 0.7996 0.9711 1.2765 1.5215 1523.5 1542.3 1559.9 1579.8 0.04 998.3 985.8 973.3 960.8 0.8061 0.9842 1.3012 1.5423 1526.3 1545.0 1563.7 1586.2 0.06 1000.3 987.6 975.4 963.2 0.8161 1.0006 1.3068 1.5623 1529.6 1548.3 1567.0 1589.4 0.08 1002.2 990.0 977.8 965.6 0.8343 1.0156 1.3197 1.5754 1532.3 1551.9 1570.4 1592.2 0.10 1003.1 991.3 979.5 967.7 0.8537 1.0289 1.3397 1.5948 1535.2 1554.3 1573.4 1594.3
  • 3. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 1 | Jan-2015, Available @ http://www.ijret.org 98 The density (ρ) increases with increase of molal concentration of amino acids and decreases with increase of concentration of n-propanol (Table 1), the values of ultrasonic velocity increase with increase in molal concentration of amino acids and also with n-propanol content. The observed results suggest a moderate strong electrolytic nature in which the solutes tend to attract the solvent molecules in the aqueous solution. When amino acids are dissolved the water structure is disturbed initially, followed by a structural reorganization leaving the molecules in closely fitting helical cavities [8]. This will increase the density structure of water. Hence the density of medium is affected. The increase in the ultrasonic velocity may be attributed to the cohesion brought about by the hydration. When the amino acids are dissolved in aqueous alcohol, the cations NH3 + and anions COO- are formed. The water molecules are attached to the ions strongly by the electrostatic forces which introduce a greater cohesion in the solution. The cohesion effect of medium generally increases with the increase of amino acid concentration. The increased associations observed in these solutions, may also be due to water structure enhancement brought by the increase of electrostriction in the presence of n-propanol. The adiabatic compressibility (β) (Table-2) decreases with increase in the concentration of amino acids and also with the n-propanol content. The decrease in adiabatic compressibility is attributed to the influence of the electrostatic field of ions (NH3 + and COO- ) on the surrounding solvent molecules (C3H7 + , OH- ). The other observed results are on (ϕk) and (ϕv) (Table 2) of L-valine, L-leucine and L-glutamine in aqueous n-propanol solutions at 308.15K has been summarized as follows. (i) All (ϕk) and (ϕv) values are negative over the entire system. (ii) With increase in concentration of amino acids as well as n-propanol in system-I the values of (ϕk) and (ϕv) decreases. For system II and II the values of (ϕk) and (ϕv) increases with increase in concentration of amino acid but decreases with the increase in concentration of n-propanol. (iii) For (ϕk) and (ϕv) values the magnitude are in the order L-valine > L-leucine > L-glutamine. Table - 2 : Values of adiabatic compressibility ( β ), apparent molar compressibility ( φk ) and apparent molar volume ( φv) of amino acids in aqueous n-propanol solutions at 308.15 K. M (mol. dm–3 ) β / ( x 10-10 m2 N-1 ) -φk / (x 10-7 m2 N-1 ) - φv / ( x 10-3 m3 mol-1 ) 0% 10% 20% 30% 0% 10% 20% 30% 0% 10% 20% 30% System - I Water + n-Propanol + L-valine 0.00 4.3572 4.3156 4.2791 4.2267 -- -- -- -- -- -- 0.02 4.3474 4.3012 4.2589 4.2023 0.6653 0.9621 1.2535 1.3546 35.28 46.68 58.72 71.36 0.04 4.3206 4.2785 4.2387 4.1714 1.0903 1.1586 1.2978 1.5266 37.78 54.41 69.31 76.74 0.06 4.3013 4.2591 4.2193 4.1522 1.1362 1.1985 1.3066 1.6006 41.95 60.39 71.53 78.44 0.08 4.2766 4.2369 4.1993 4.1226 1.2102 1.2424 1.3130 1.6394 47.78 64.61 75.75 83.31 0.10 4.2461 4.2050 4.1660 4.0950 1.2293 1.3570 1.4321 1.6407 52.23 69.15 78.55 86.16 System - II Water + n-Propanol + L-Leucine 0.00 4.3572 4.3156 4.2791 4.2267 -- -- -- -- -- -- 0.02 4.3203 4.2827 4.2340 4.1828 2.0595 2.3715 3.3179 3.4813 136.13 171.05 255.67 317.30 0.04 4.2986 4.2585 4.2112 4.1422 1.9252 2.0109 2.4503 2.9665 105.69 131.06 180.69 210.16 0.06 4.2773 4.2351 4.1884 4.1148 1.7627 1.8480 2.1464 2.5820 98.80 118.74 152.04 176.11 0.08 4.2601 4.2094 4.1660 4.0850 1.6301 1.8283 2.0005 2.4088 95.28 117.19 140.25 156.28 0.10 4.2378 4.1888 4.1421 4.0712 1.5841 1.7303 1.9058 2.1360 89.14 108.01 127.87 142.17 System - III Water + n-Propanol + L-Glutamine 0.00 4.3572 4.3156 4.2791 4.2267 -- -- -- -- -- -- 0.02 4.3204 4.2697 4.2280 4.1763 2.4513 3.2857 3.5430 3.9615 161.27 233.01 308.64 355.34 0.04 4.2999 4.2496 4.2019 4.1365 1.9037 2.2774 2.7161 3.1310 108.18 147.33 188.57 215.56 0.06 4.2761 4.2238 4.1752 4.1102 1.8119 2.0804 2.4107 2.7031 105.45 128.99 162.54 186.88 0.08 4.2493 4.1940 4.1469 4.0850 1.7980 2.0648 2.2946 2.4754 102.74 127.39 153.33 172.38 0.10 4.2298 4.1756 4.1239 4.0652 1.6728 1.8931 2.1410 2.2714 91.12 115.12 140.38 160.34
  • 4. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 1 | Jan-2015, Available @ http://www.ijret.org 99 The negative values of (ϕk) and (ϕv) indicates ionic and hydrophilic interactions occurring in these systems [10]. The magnitude of (ϕk) strongly supports our earlier view of the ultrasonic velocity and adiabatic compressibility. The negative values of (ϕv) indicate electrostrictive solvation of ions [11]. The value of (ϕv) shows that stronger molecular association has been found in L-valine. Hence L-valine is a more effective structure maker than other two amino acids. From Table 3, the changes observed in (ϕ°k) and (Sk) values with increase of amino acids concentration may be due to ion-solvent interaction and ion-ion interactions in the solution. The values of (ϕ°k) are negative and it decreases with increasing concentration of n-propanol in all the systems studied. It confirms the existence of ion-solvent interaction in the mixtures. The magnitude of (ϕ°k) is in the order L-valine > L-leucine > L-glutamine. The values of (Sk) is negative for L-valine (Table 3), but it is positive for other two amino acids. The negative values of (Sk) Indicate weakening of ion-ion interaction and suggest the structure breaking effect of the amino acids. It is well known that solutes causing electrostriction lead to decrease in compressibility of the solution. This is reflected by the negative values of the (ϕk) values of amino acids. The volume behavior of the solute at infinite dilution is satisfactorily represented by (ϕ°v), which is independent of the ion-ion interactions and provides information concerning ion-solvent interactions. Table 3 reveals that the values of (ϕ°v) are negative in all the three amino acids. From table 3, (Sv) values are negative for L-valine and positive for the other two amino acids. The negative (Sv) values for L-valine suggest the presence of weak ion-ion interactions [12]. Therefore it causes the complex ion formation in the systems. The values of transfer adiabatic compressibility (Δϕ°k) and transfer volume (Δϕ°v) (Table 3) are negative and it decreases with increasing concentration of n-propanol in all the three amino acid systems. It suggests that the existence of ion-solvent interaction in the mixtures. Table - 3 Values of limiting apparent molal compressibility ( ), limiting apparent molal volume ( ), their constants Sk and Sv, transfer adiabatic compressibility (Δ ) and transfer volume (Δ ) of the amino acids in aqueous n-propanol solutions at 308.15 K Amino Acid M/ (mol. Kg–1 ) – / (×10-7 m2 N-1 ) – / (×10-3 m3 mol-1 ) Sk / (×10-7 N-1 m-1 mol-1 ) Sv / (×10-3 m3 L1/2 mol-3/2 ) Δ /(×10-7 m2 N-1 ) Δ / (×10-3 m3 mol-1 ) A / (dm3/2 . mol-1/2 ) B / (dm3/2 . mol-1 ) L-Valine 0% 0.3522 20.46 -3.0117 -95.06 - - 0.8210 -0.0349 10% 0.7044 29.11 -2.0216 -126.25 -0.3522 -8.65 0.1982 0.1168 20% 1.1286 45.41 -0.8096 -106.97 -0.7764 -24.95 -0.0384 0.9700 30% 1.1663 59.85 -1.6285 -81.62 -0.8141 -39.39 -0.0357 1.0517 L-Leucine 0% 2.4107 164.68 2.6080 251.72 - - 0.8746 -1.2209 10% 2.7867 209.04 3.4966 336.75 -0.376 -44.36 -0.1051 1.2781 20% 4.2240 338.96 7.8453 707.24 -1.8133 -174.28 0.4427 -0.2459 30% 4.5015 429.68 7.5367 969.18 -2.0908 -265.00 -0.1546 0.6913 L-Glutamine 0% 3.0022 197.5 4.4574 0.3534 - - 0.8882 -1.1238 10% 4.0460 297.7 7.2800 0.6226 -1.0438 -0.1002 -0.0500 0.8670 20% 4.4470 404.3 7.7035 0.9013 -1.4448 -0.2068 1.9129 -3.6004 30% 5.1630 467.1 9.5105 1.0505 -2.1608 -0.2696 1.6619 -3.0269 In the case of amino acids + n-propanol + water, when the solute-cosolute molecules come close enough, their cospheres overlaps and the following types of interactions are possible: (1) Ion-hydrophilic interactions occurring between zwitterionic centers of amino acids and the –OH group of n-propanol, (2) Hydrophobic - hydrophilic interactions between nonpolar parts of amino acids or n-propanol and –OH group of n-propanol or zwitterionic centers of amino acids, and
  • 5. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 _______________________________________________________________________________________ Volume: 04 Issue: 1 | Jan-2015, Available @ http://www.ijret.org 100 (3) hydrophobic-hydrophobic interactions occurring between the nonpolar parts of amino acids and the nonpolar parts of n-propanol. Anwar Ali [13] was also suggested the similar types of interactions in the study of some amino acids with salts in aqueous medium. On the basis of co-sphere overlap model [14] the (Δϕ°v) values can also be explained in terms of solute-cosolute (ion-ion) interactions. According to this model, ion-ion group interactions contribute positively whereas ion-non- polar and non-polar-non-polar interactions contribute negatively to the (Δϕ°v) values. Therefore the negative values of (Δϕ°k) and (Δϕ°v) observed in all the three amino acids showed that the interaction contribution of type (ii) is stronger than that of type (i). The study of Viscosity (η), helps to understand the structure as well as molecular interactions occurring in the solutions. It is observed that the values of viscosity increases with increasing in solute concentration. This increasing effect indicates the existence of ion-solvent interaction occurring in these systems (Table 1). Further to confirm the effect, the role of viscosity (B) coefficient has been obtained from Jones-Dole equations [15]. The (A) coefficient is negative and (B) coefficient is positive for L-valine whereas a reverse trend is observed for the other two amino acids (Table 3). Since there is a weak ion-ion interaction is occurred in L-valine, because (A) is a measure of ionic interaction, which is indicated by the negative and smaller magnitude of (A) values [16] for L- valine and vice-versa for the other two amino acids. The viscosity (B) coefficient [17] gives the effect of ion-solvent interactions on the solution viscosity. The positive (B) values suggest the presence of strong ion- solvent interactions vice-versa. The magnitude of (B) is in the order L-valine > L-leucine > L-glutamine. The larger value of (B) shows structure making capacity of the solute. 4. CONCLUSION In summary, from the magnitudes of β, ϕk, ϕv and viscosity B coefficient, it can be concluded that L-valine in aqueous n-propanol solution possesses the strong ion- solvent interaction than the other two amino acids. The transfer volume (Δϕ°v) suggests an ionic hydrophobic group interaction which predominates over the ionic hydrophilic interactions and hydrophobic – hydrophobic interactions. From the co-sphere overlap model it can be concluded that ionic-hydrophobic interactions are dominating over the ion- ion and hydrophobic – hydrophilic interactions. REFERENCES [1]. Hedwig G.R., HoilandH., J. Chem. Thermodyn., 23 (1999), 1029. [2]. Lin Q., HuX., Lin L., SangW., LiS., J. Chem. Eng. Data, 46 522 (2001). [3]. Hackel M., HinzH., HeduringG. R., J. Mol. Bio. 66 429 (1999). [4]. Kumar P., Kumar S., SinghS., GangwarR. S., Oriental J. of Chem. 2011. 27 No:2, 639 – 644. [5]. Gucker, F.T., Chem.Rev.,13 (1993) 111 [6]. Debye, P., and Huckel, E., Z.Phys.,24 (1923) 305 [7]. Jones, A., and Dole, M., J.Am.Chem. Soc.,51(1929) 2950 [8]. Falkenhagen, H., and Vernon, E.L., Z.Phys.,33 (1932) 140 [9]. Kavanou J., water and solute water interactions (Holden-Day Amsterdam) (1964). [10]. Sandu J.S& Gurbis singh, J Ind. Chem. Soc., 65, 135 (1992). [11]. Dhanalakshmi & Jasmin E, J. Pure. Appl. Ultrasonics., 21, 79 (1999). [12]. Biswajit Sinha, Bipulkumar Sarkar and Mahendranath Roy. J. Chem. Thermodyn., 40, 394 (2008). [13]. Anwar Ali, Shahla Khan, Soghra Hyder & Mohd Tariq, J. Chem. Thermodyn, 39, 613 (2007). [14]. Gurney R.W., Ionic process in solution chapter-I (McGraw – Hill, New York) 1953. [15]. Jones G., Dole M., J. Am. Chem. Soc., 51, 2950 (1929). [16]. Man Singh, Maneesha Pandey, Rajeshkumar Yadav., Verma H.S., J. Mol. Liq., 135. 188 (2007). [17]. Millero F. J., LosurdoA., ShinC., J. Phys. Chem., 82, 784 (1978).