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Chemistry and Materials Research                                                                 www.iiste.org
ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online)
Vol 2, No.1, 2012


Study the Rheological and Mechanical Properties of PVA/CuCl2
                                              by Ultrasonic
                                        1
                                            Abdul-Kareem Jawad Rashid
                                              2
                                                  Burak Yahya Kadem
                                                   3
                                                       Lamis F.Naser
   1. University of Babylon, College of Science, Physics Department, Babylon, Hilla -Najif Street, Iraq
   2. University of Babylon, College of Science, Physics Department, Babylon, Hilla -Najif Street, Iraq
   3. University of Babylon, College of Science, Physics Department, Babylon, Hilla -Najif Street, Iraq
                                                                           2
     * E-mail of the corresponding author: 1dr.abdulkaream@yahoo.com & burakwh@yahoo.com
Abstract
Some of physical properties of polyvinyl alcohol dissolves in distilled water had been studied before and after
adding different weights of copper (II) chloride (CuCl2), the Rheological properties shows that the densities
variation are intangible and shear viscosity are responsible for reducing velocity, bulk modulus and
transmittance the absorption coefficient of ultrasonic waves and relaxation amplitude are increasing with
adding copper (II) chloride because there will be more molecules in solution and this lead to more
attenuation against wave propagation
Keywords: PVA solution, mechanical properties, rheological properties, ultrasound technique.


1. Introduction
PVA is a water-soluble synthetic polymer, due to the characteristics of easy preparation, good
biodegradability, excellent chemical resistance, and good mechanical properties, polyvinyl alcohol is used
mainly as a solution in water but its solubility in water depends on its degree of polymerization and degree of
hydrolysis of its precursor (poly vinyl acetate), In PVA solutions in water, very complicated and strong
physical interactions between solvent and polymer would be present.
The rheological properties of the PVA solutions are affected by effectiveness of the physical bonding solvent
systems the physical state of water is very important to rheological responses because free water forms
hydro-gel structure (Song and Byoung 2004) solvent effects might therefore be expected to influence the
ultrasonic relation behavior, the absorption of ultrasonic in liquid polymer systems is governed by local
modes of motion and cooperative whole molecule movement because of the strong intermolecular
interaction within the polymer it should be possible to observe cooperative motion in the ultrasonic range
(Jayanta   et. al. 2004).
Polyvinyl alcohol has high tensile strength and flexibility, as well as high oxygen and aroma barrier
properties. However these properties are dependent on humidity, in other words, with higher humidity more
water is absorbed, the water which acts as a plasticizer, will then reduce its tensile strength, but increase its
elongation and tear strength. PVA is fully degradable and dissolves quickly. (Fromageau et. al.           2003).
Acoustic relaxation measurements on other polymers have been reported by several workers (Hasun S.K.
1989, Tomasz et. al. 2010, Hassun,S.K. and Rahman,K.1990, Khalida 2004), ultrasonic technique is good
method for studying the structural changes associated with the information of mixture assist in the study of
molecular interaction between two species; some of mechanical properties of different polymers were

                                                           19
Chemistry and Materials Research                                                                 www.iiste.org
ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online)
Vol 2, No.1, 2012
carried by some workers using ultrasonic technique (Al-Bermany E.2004, B. Boro 2009). Aqueous solution
prepared from copper (II) chloride contains a range of copper (II) complexes depending on concentration,
temperature and the presence of additional chloride ions (Greenwood and Earnshaw 1997, ).




     (Fig. 1) The molecular structure of CuCl2.2H2O             (Fig. 2) The molecular structure of PVA.


2. Experimental
2.1 Preparation of Solutions:
The solution was prepared by soluble (0.5 gm PVA) in (400 ml) distilled water under stirring at 80oC for (1
hour) the resulting solution was stirred continuously until the solution mixture became a homogeneous, the
copper (II) chloride weights were (0.01, 0.02, 0.03, 0.04, 0.05) gm added to the PVA solution to study the
addition affect on some of the rheological and mechanical properties.


2.2 Ultrasonic measurements:
 Ultrasonic measurements were made by pulse technique of sender-receiver type (SV-DH-7A/SVX-7
velocity of sound instrument) with different frequencies (25, 30,35,40,45 and 50 kHz) in our study the
frequency fixed at (25 KHz), the receiver quartz crystal mounted on a digital vernier scale of slow motion, the
receiver crystal could be displaced parallel to the sender and the samples were put between sender and
receiver. The sender and receiver pulses (waves) were displaced as two traces of cathode ray oscilloscope,
and the digital delay time (t) of receiver pulses were recorded with respect to the thickness of the samples (x).
The pulses height on oscilloscope (CH1) represents incident ultrasonic wave’s amplitude (A0) and the pulses
height on oscilloscope (CH2) represents the receiver ultrasonic wave’s amplitude (A).


3.    Results and Discussion
The densities of the solutions (ρ) were determined by density bottle method, the change in densities is
almost intangible when we add copper (II) chloride as shown in (Fig.3) their viscosities measured before
and after adding copper chloride for all samples using Ostwald viscometer with accuracy of ± 1.05%, the
method of measurement has been described by (Al-Bermany E.2004), elsewhere the shear viscosity were
determined before and after the adding of copper (II) chloride by the following equation (Illiger         et. al.
2008, Subhi     et. al.1990) (ηs /ηo = t ρ /to ρo) where (ηs) is the solution viscosity, (ρo) and (ηo) are the
distilled water density and viscosity respectively, the shear viscosity is increasing with adding copper (II)
chloride as shown in (Fig.4) since the viscosity describes a fluid's internal resistance between molecules so
when we add the copper (II) chloride there will be more molecules, the additional forces between molecules
leads to an additional contribution to the shear stress and this lead to reduce velocity as shown in (Fig.3),
the associated state of water in the solvent systems had a significant effect on the physical properties of
PVA solutions such as rheological responses and molecular relaxation behavior (Song and Byoung 2004).
Ultrasonic wave velocity (v) shown in (Fig.5) was calculated using the following equation (Boutouyrie et.

                                                       20
Chemistry and Materials Research                                                                www.iiste.org
ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online)
Vol 2, No.1, 2012
al. 2009) (v = x / t ) where (t) is the time that the waves need to cross the samples (digital obtained from the
instrument), the velocity is decreasing this because structural or volume relaxation it occurs in associated
liquids such as polymers, a liquid when at rest has a lattice structure similar to that possessed by solid when
waves are propagated through it, the resultant periodic     changes of    wave pressure causes molecules to
flow into vacancies in the lattice during compression phase and to return to their original positions in the
lattice during rarefaction, because of this and because of viscosity the ratio of the change in pressure to the
fractional volume compression is decrease with adding copper (II) chloride, this called the bulk modulus of
the material (B) as shown in (Fig.6) and it is calculated by Laplace equation (B = ρ v 2) (Abdul-Kareem
et.al .2011). (Fig.7) shows the solutions compressibility (K) which is calculated from this equation (R.
Palani and S. Kalavathy 2011) (K =1/ ρ v 2) the compressibility appears to be increasing with increase in
copper (II) chloride molecules, this behavior indicates significant interaction between solute and solvent
molecules due to which the structural arrangement in the neighborhoods of constituent solutes is
considerably affected. The transmittance (T) is the fraction of incident wave at a specified wavelength that
passes through the sample was calculated from the following equation (Dipak Basu 2001) (T = I / Io) where
(Io) is the initially intensity of the ultrasonic waves and (I) is the received intensity, it is decreasing with
adding copper (II) chloride as shown in (Fig.8) this attributed that the polymer molecules absorbed the sound
waves according to Lambert-Beer Law (Ingle and        Crouch 1988) (A/A0 = e- α x ) where (α) is the absorption
coefficient,   (A0) is the initially amplitude of the ultrasonic waves, (A) is the wave amplitude after
absorption and (x) is the thickness of the sample and because the viscosity increasing the absorption
coefficient is increasing as shown in (Fig.9) which is biased on concentration (Dipak Basu 2001, Ingle and
Crouch 1988), this attributed to the fact that when adding copper (II) chloride there will be more molecules
in solution this lead to more attenuation against wave propagation, the attenuation can be attributed to the
friction and heat exchange between the particles and the surrounding medium as well as to the decay of the
acoustic wave in the forward direction due to scattering by the Particles (Tomasz et. al. 2010) so there will be
increasing in absorption and this lead to increase the relaxation amplitude as shown in (Fig.10), the
Attenuation is generally proportional to the square of sound frequency, the relaxation amplitude (D) was
calculated from the following equation (D = α/ f2) (Josef and Herbert 1990) where (f) is the ultrasonic
frequency and this attributed to the fact that ultrasonic energy depends on viscosity thermal conductivity,
scattering and intermolecular processes , thermal conductivity and scattering effects are known to be
negligible (Boutouyrie et.al. 2009, Josef and Herbert 1990) so viscosity is responsible for the increase of
relaxation amplitude for this reason absorption coefficient commonly known as visco –absorption.
1.   Conclusion
This study shows that intermolecular processes and the associated state of water in the solvent systems had a
significant effect on the physical properties of PVA solutions such as rheological responses and molecular
relaxation behavior, and indicating increase in the size of molecules in bath of ultrasonic waves, when
concentration increases there will be complexes molecules formed in the solution by the effect of peroxide
and roots that rebounded to formations between polymer chains when adding copper chloride, the affect of
adding copper chloride on densities is intangible so the viscosities of solutions which were increasing are
responsible for reducing velocity of ultrasound then reducing the bulk modulus and transmittance, this lead to
increase the absorption coefficient with adding copper chloride because molecules absorbed the sound waves
according to Lambert-Beer Law then increase the relaxation amplitude.

                                                      21
Chemistry and Materials Research                                                             www.iiste.org
ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online)
Vol 2, No.1, 2012

References
Abdul-Kareem Jawad Rashid , Rawaa Mizher Obiad, Burak Yahya Kadem, “Study the Rheological and
Mechanical Properties of PVA/NH4Cl by Ultrasonic” Chemistry and Materials Research, iiste., Vol 1, No.1,
2011.

Al-Bermany E.(2004),”Gamma radiation effect in some physical properties of polymer zanthan cellulose
“M.Sc. thesis, Baghdad university.


B. Boro Djordjevi (2009), “Ultrasonic characterization of advanced composite materials” the 10th
International Conference of the Slovenian Society for Non- Destructive Testing (Application of
Contemporary Non-Destructive Testing in Engineering), Ljubljana, Slovenia, pp. 47-57.


Boutouyrie P, Briet M, Collin C, Vermeersch S, Pannier B Artery Research,3(1): 3–8(2009).


Dipak Basu (2001) Dictionary of Material Science and High Energy Physics, CRC Press, Chapter 26


Fromageau, J.; Brusseau, E.; Vray, D.; Gimenez, G.; Delachartre, P.; IEEE Transactions on Ultrasonics,
Ferroelectrics and Frequency Control, Volume: 50, Issue: 10. 2003, Page(s): 1318 - 1324.


Greenwood, N. N. and Earnshaw, A. (1997). Chemistry of the Elements (2nd Edn.), Oxford:Butterworth-
Heinemann.


Hassun,S.K., Rahman,K.(1990), Ultrasonic Study of Molecular Association of High Impact Polystyrene
Solutions in Toluene, Iraqi Journal of Science, 31,3,24.


Hasun S.K. ,”Ultrasonic study and visco-relaxation of       PVA”, British polymer Journal, (1989) vol.21,
333-338.


Illiger S R, Rao K.P. and Demappa, T.(2008), Miscibility Studies of HPMC/PVA Blends in Water by
Viscosity, Density, Refractive Index and Ultrasonic Velocity Method, Carbohydrate Polymer, 74,779-782.


Jayanta Chakraborty, Jayashri Sarkar, Ravi Kumar and Giridhar Madra (2004) “Ultrasonic Degradation of
Polybutadiene and Isotactic Polypropylene”, Polymer Degradation and Stability, Elsevier,85(1),555-558.
J. D. J. Ingle and S. R. Crouch, Spectrochemical Analysis, Prentice Hall, N.J. (1988)]


Krautkramer, Josef and Herbert, “Ultrasonic testing of materials” 4th edition, Springer. (1990).


Khalida,H.H., Study of Structural and Visco-Relaxation of Polycarbonates Solutions by Ultrasonic
Technique, Journal of Al-Qadisiya of Pure Sciences, (2004) 9,3,188-122.



                                                     22
Chemistry and Materials Research                                                              www.iiste.org
ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online)
Vol 2, No.1, 2012
R. Palani and S. Kalavathy      2011, Volumetric compressibility and transport studies on molecular
interactions of mono, di and tri saccharine in aqueous sodium butyrate mixtures at 303.15 K, Advances in
Applied Science Research, 2011, 2 (2): 146-155


Subhi K. Hassun, Kadhim H. Hussain and Najiba A. Hassan (1990), Visco- Relaxation Studies of
Polystyrene Solutions in Different Solvents by Ultrasonic , Acta Polymerica, 41(8),438-441.


Song Ie Song, Byoung Chul Kim 2004, Characteristic rheological features of PVA solutions in water-
containing solvents with different hydration states, Polymer (45) Elsevier, p. 2381–2386


Tomasz Hornowski, Arkadiusz Józefczak ,Andrzej Skumiel and Mikołaj Łabowski ,” Effect of
Poly(Ethylene Glycol) Coating on the Acoustic Properties of Biocompatible Magnetic Fluid”, Int J Thermo
phys. , (2010), 31:70–76.




       (Fig.3) Density due toCuCl2 addition              (Fig.4) Shear viscoscity due to concentration




                                                    23
Chemistry and Materials Research                                                             www.iiste.org
ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online)
Vol 2, No.1, 2012




  (Fig.5) Ultrasonic velocity due to concentration          (Fig.6) Bulk modules due to concentration




  (Fig.7) Compressibility due to concentration            (Fig.8) Transmittance due to concentration




  (Fig.9) Absorption coefficient due to concentration (Fig.10) Relaxation amplitude due to concentration




                                                     24

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Study the rheological and mechanical properties of pva cu cl2 by ultrasonic

  • 1. Chemistry and Materials Research www.iiste.org ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) Vol 2, No.1, 2012 Study the Rheological and Mechanical Properties of PVA/CuCl2 by Ultrasonic 1 Abdul-Kareem Jawad Rashid 2 Burak Yahya Kadem 3 Lamis F.Naser 1. University of Babylon, College of Science, Physics Department, Babylon, Hilla -Najif Street, Iraq 2. University of Babylon, College of Science, Physics Department, Babylon, Hilla -Najif Street, Iraq 3. University of Babylon, College of Science, Physics Department, Babylon, Hilla -Najif Street, Iraq 2 * E-mail of the corresponding author: 1dr.abdulkaream@yahoo.com & burakwh@yahoo.com Abstract Some of physical properties of polyvinyl alcohol dissolves in distilled water had been studied before and after adding different weights of copper (II) chloride (CuCl2), the Rheological properties shows that the densities variation are intangible and shear viscosity are responsible for reducing velocity, bulk modulus and transmittance the absorption coefficient of ultrasonic waves and relaxation amplitude are increasing with adding copper (II) chloride because there will be more molecules in solution and this lead to more attenuation against wave propagation Keywords: PVA solution, mechanical properties, rheological properties, ultrasound technique. 1. Introduction PVA is a water-soluble synthetic polymer, due to the characteristics of easy preparation, good biodegradability, excellent chemical resistance, and good mechanical properties, polyvinyl alcohol is used mainly as a solution in water but its solubility in water depends on its degree of polymerization and degree of hydrolysis of its precursor (poly vinyl acetate), In PVA solutions in water, very complicated and strong physical interactions between solvent and polymer would be present. The rheological properties of the PVA solutions are affected by effectiveness of the physical bonding solvent systems the physical state of water is very important to rheological responses because free water forms hydro-gel structure (Song and Byoung 2004) solvent effects might therefore be expected to influence the ultrasonic relation behavior, the absorption of ultrasonic in liquid polymer systems is governed by local modes of motion and cooperative whole molecule movement because of the strong intermolecular interaction within the polymer it should be possible to observe cooperative motion in the ultrasonic range (Jayanta et. al. 2004). Polyvinyl alcohol has high tensile strength and flexibility, as well as high oxygen and aroma barrier properties. However these properties are dependent on humidity, in other words, with higher humidity more water is absorbed, the water which acts as a plasticizer, will then reduce its tensile strength, but increase its elongation and tear strength. PVA is fully degradable and dissolves quickly. (Fromageau et. al. 2003). Acoustic relaxation measurements on other polymers have been reported by several workers (Hasun S.K. 1989, Tomasz et. al. 2010, Hassun,S.K. and Rahman,K.1990, Khalida 2004), ultrasonic technique is good method for studying the structural changes associated with the information of mixture assist in the study of molecular interaction between two species; some of mechanical properties of different polymers were 19
  • 2. Chemistry and Materials Research www.iiste.org ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) Vol 2, No.1, 2012 carried by some workers using ultrasonic technique (Al-Bermany E.2004, B. Boro 2009). Aqueous solution prepared from copper (II) chloride contains a range of copper (II) complexes depending on concentration, temperature and the presence of additional chloride ions (Greenwood and Earnshaw 1997, ). (Fig. 1) The molecular structure of CuCl2.2H2O (Fig. 2) The molecular structure of PVA. 2. Experimental 2.1 Preparation of Solutions: The solution was prepared by soluble (0.5 gm PVA) in (400 ml) distilled water under stirring at 80oC for (1 hour) the resulting solution was stirred continuously until the solution mixture became a homogeneous, the copper (II) chloride weights were (0.01, 0.02, 0.03, 0.04, 0.05) gm added to the PVA solution to study the addition affect on some of the rheological and mechanical properties. 2.2 Ultrasonic measurements: Ultrasonic measurements were made by pulse technique of sender-receiver type (SV-DH-7A/SVX-7 velocity of sound instrument) with different frequencies (25, 30,35,40,45 and 50 kHz) in our study the frequency fixed at (25 KHz), the receiver quartz crystal mounted on a digital vernier scale of slow motion, the receiver crystal could be displaced parallel to the sender and the samples were put between sender and receiver. The sender and receiver pulses (waves) were displaced as two traces of cathode ray oscilloscope, and the digital delay time (t) of receiver pulses were recorded with respect to the thickness of the samples (x). The pulses height on oscilloscope (CH1) represents incident ultrasonic wave’s amplitude (A0) and the pulses height on oscilloscope (CH2) represents the receiver ultrasonic wave’s amplitude (A). 3. Results and Discussion The densities of the solutions (ρ) were determined by density bottle method, the change in densities is almost intangible when we add copper (II) chloride as shown in (Fig.3) their viscosities measured before and after adding copper chloride for all samples using Ostwald viscometer with accuracy of ± 1.05%, the method of measurement has been described by (Al-Bermany E.2004), elsewhere the shear viscosity were determined before and after the adding of copper (II) chloride by the following equation (Illiger et. al. 2008, Subhi et. al.1990) (ηs /ηo = t ρ /to ρo) where (ηs) is the solution viscosity, (ρo) and (ηo) are the distilled water density and viscosity respectively, the shear viscosity is increasing with adding copper (II) chloride as shown in (Fig.4) since the viscosity describes a fluid's internal resistance between molecules so when we add the copper (II) chloride there will be more molecules, the additional forces between molecules leads to an additional contribution to the shear stress and this lead to reduce velocity as shown in (Fig.3), the associated state of water in the solvent systems had a significant effect on the physical properties of PVA solutions such as rheological responses and molecular relaxation behavior (Song and Byoung 2004). Ultrasonic wave velocity (v) shown in (Fig.5) was calculated using the following equation (Boutouyrie et. 20
  • 3. Chemistry and Materials Research www.iiste.org ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) Vol 2, No.1, 2012 al. 2009) (v = x / t ) where (t) is the time that the waves need to cross the samples (digital obtained from the instrument), the velocity is decreasing this because structural or volume relaxation it occurs in associated liquids such as polymers, a liquid when at rest has a lattice structure similar to that possessed by solid when waves are propagated through it, the resultant periodic changes of wave pressure causes molecules to flow into vacancies in the lattice during compression phase and to return to their original positions in the lattice during rarefaction, because of this and because of viscosity the ratio of the change in pressure to the fractional volume compression is decrease with adding copper (II) chloride, this called the bulk modulus of the material (B) as shown in (Fig.6) and it is calculated by Laplace equation (B = ρ v 2) (Abdul-Kareem et.al .2011). (Fig.7) shows the solutions compressibility (K) which is calculated from this equation (R. Palani and S. Kalavathy 2011) (K =1/ ρ v 2) the compressibility appears to be increasing with increase in copper (II) chloride molecules, this behavior indicates significant interaction between solute and solvent molecules due to which the structural arrangement in the neighborhoods of constituent solutes is considerably affected. The transmittance (T) is the fraction of incident wave at a specified wavelength that passes through the sample was calculated from the following equation (Dipak Basu 2001) (T = I / Io) where (Io) is the initially intensity of the ultrasonic waves and (I) is the received intensity, it is decreasing with adding copper (II) chloride as shown in (Fig.8) this attributed that the polymer molecules absorbed the sound waves according to Lambert-Beer Law (Ingle and Crouch 1988) (A/A0 = e- α x ) where (α) is the absorption coefficient, (A0) is the initially amplitude of the ultrasonic waves, (A) is the wave amplitude after absorption and (x) is the thickness of the sample and because the viscosity increasing the absorption coefficient is increasing as shown in (Fig.9) which is biased on concentration (Dipak Basu 2001, Ingle and Crouch 1988), this attributed to the fact that when adding copper (II) chloride there will be more molecules in solution this lead to more attenuation against wave propagation, the attenuation can be attributed to the friction and heat exchange between the particles and the surrounding medium as well as to the decay of the acoustic wave in the forward direction due to scattering by the Particles (Tomasz et. al. 2010) so there will be increasing in absorption and this lead to increase the relaxation amplitude as shown in (Fig.10), the Attenuation is generally proportional to the square of sound frequency, the relaxation amplitude (D) was calculated from the following equation (D = α/ f2) (Josef and Herbert 1990) where (f) is the ultrasonic frequency and this attributed to the fact that ultrasonic energy depends on viscosity thermal conductivity, scattering and intermolecular processes , thermal conductivity and scattering effects are known to be negligible (Boutouyrie et.al. 2009, Josef and Herbert 1990) so viscosity is responsible for the increase of relaxation amplitude for this reason absorption coefficient commonly known as visco –absorption. 1. Conclusion This study shows that intermolecular processes and the associated state of water in the solvent systems had a significant effect on the physical properties of PVA solutions such as rheological responses and molecular relaxation behavior, and indicating increase in the size of molecules in bath of ultrasonic waves, when concentration increases there will be complexes molecules formed in the solution by the effect of peroxide and roots that rebounded to formations between polymer chains when adding copper chloride, the affect of adding copper chloride on densities is intangible so the viscosities of solutions which were increasing are responsible for reducing velocity of ultrasound then reducing the bulk modulus and transmittance, this lead to increase the absorption coefficient with adding copper chloride because molecules absorbed the sound waves according to Lambert-Beer Law then increase the relaxation amplitude. 21
  • 4. Chemistry and Materials Research www.iiste.org ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) Vol 2, No.1, 2012 References Abdul-Kareem Jawad Rashid , Rawaa Mizher Obiad, Burak Yahya Kadem, “Study the Rheological and Mechanical Properties of PVA/NH4Cl by Ultrasonic” Chemistry and Materials Research, iiste., Vol 1, No.1, 2011. Al-Bermany E.(2004),”Gamma radiation effect in some physical properties of polymer zanthan cellulose “M.Sc. thesis, Baghdad university. B. Boro Djordjevi (2009), “Ultrasonic characterization of advanced composite materials” the 10th International Conference of the Slovenian Society for Non- Destructive Testing (Application of Contemporary Non-Destructive Testing in Engineering), Ljubljana, Slovenia, pp. 47-57. Boutouyrie P, Briet M, Collin C, Vermeersch S, Pannier B Artery Research,3(1): 3–8(2009). Dipak Basu (2001) Dictionary of Material Science and High Energy Physics, CRC Press, Chapter 26 Fromageau, J.; Brusseau, E.; Vray, D.; Gimenez, G.; Delachartre, P.; IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control, Volume: 50, Issue: 10. 2003, Page(s): 1318 - 1324. Greenwood, N. N. and Earnshaw, A. (1997). Chemistry of the Elements (2nd Edn.), Oxford:Butterworth- Heinemann. Hassun,S.K., Rahman,K.(1990), Ultrasonic Study of Molecular Association of High Impact Polystyrene Solutions in Toluene, Iraqi Journal of Science, 31,3,24. Hasun S.K. ,”Ultrasonic study and visco-relaxation of PVA”, British polymer Journal, (1989) vol.21, 333-338. Illiger S R, Rao K.P. and Demappa, T.(2008), Miscibility Studies of HPMC/PVA Blends in Water by Viscosity, Density, Refractive Index and Ultrasonic Velocity Method, Carbohydrate Polymer, 74,779-782. Jayanta Chakraborty, Jayashri Sarkar, Ravi Kumar and Giridhar Madra (2004) “Ultrasonic Degradation of Polybutadiene and Isotactic Polypropylene”, Polymer Degradation and Stability, Elsevier,85(1),555-558. J. D. J. Ingle and S. R. Crouch, Spectrochemical Analysis, Prentice Hall, N.J. (1988)] Krautkramer, Josef and Herbert, “Ultrasonic testing of materials” 4th edition, Springer. (1990). Khalida,H.H., Study of Structural and Visco-Relaxation of Polycarbonates Solutions by Ultrasonic Technique, Journal of Al-Qadisiya of Pure Sciences, (2004) 9,3,188-122. 22
  • 5. Chemistry and Materials Research www.iiste.org ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) Vol 2, No.1, 2012 R. Palani and S. Kalavathy 2011, Volumetric compressibility and transport studies on molecular interactions of mono, di and tri saccharine in aqueous sodium butyrate mixtures at 303.15 K, Advances in Applied Science Research, 2011, 2 (2): 146-155 Subhi K. Hassun, Kadhim H. Hussain and Najiba A. Hassan (1990), Visco- Relaxation Studies of Polystyrene Solutions in Different Solvents by Ultrasonic , Acta Polymerica, 41(8),438-441. Song Ie Song, Byoung Chul Kim 2004, Characteristic rheological features of PVA solutions in water- containing solvents with different hydration states, Polymer (45) Elsevier, p. 2381–2386 Tomasz Hornowski, Arkadiusz Józefczak ,Andrzej Skumiel and Mikołaj Łabowski ,” Effect of Poly(Ethylene Glycol) Coating on the Acoustic Properties of Biocompatible Magnetic Fluid”, Int J Thermo phys. , (2010), 31:70–76. (Fig.3) Density due toCuCl2 addition (Fig.4) Shear viscoscity due to concentration 23
  • 6. Chemistry and Materials Research www.iiste.org ISSN 2224- 3224 (Print) ISSN 2225- 0956 (Online) Vol 2, No.1, 2012 (Fig.5) Ultrasonic velocity due to concentration (Fig.6) Bulk modules due to concentration (Fig.7) Compressibility due to concentration (Fig.8) Transmittance due to concentration (Fig.9) Absorption coefficient due to concentration (Fig.10) Relaxation amplitude due to concentration 24