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Advances in Physics Theories and Applications www.iiste.org
ISSN 2224-719X (Paper) ISSN 2225-0638 (Online)
Vol.20, 2013
134
Enhancement Mechanical Properties of Barium Chloride by
Adding Copper Chloride using Ultrasonic Technique
Prof.Dr.Abdul-Kareem J. Al-Bermany(Corresponding author)
Babylon University / Facility of Science /Physics Department /Advanced polymer laboratory
E-Mail: dr.abdulkaream@yahoo.com
Burak Yahya Kadem
E-Mail burakwh@yahoo.com
Lamis Faaz Naser
Babylon University / Facility of Science /Physics Department /Advanced polymer laboratory
SShh-Phy@yahoo.com
Abstract:
Some of physical properties of BaCl2 dissolves in distilled water had been studied at different concentrations
(0.05%, 0.1%, 0.15%, 0.2%, 0.25% and 0.3%) (gm./ml) before and after adding (0.3)gm of CuCl2 for all
concentrations , the mechanical properties such as ultrasonic velocity had been measured by ultrasonic waves
system at frequency 25 KHz, other mechanical properties had been calculated such as absorption coefficient of
ultrasonic waves, relaxation time, relaxation amplitude, specific acoustic impedance, compressibility and bulk
modules. The results show that all these properties are increasing with the increase of the polymer concentration
except compressibility is decreasing with the increase of the concentration; results show that when adding CuCl2
these properties are increasing except compressibility is decreasing. Results also shows that adding CuCl2 to
BaCl2 enhances the ultrasonic absorption coefficient as a result of high values after addition.
Keywords: BaCl2 solution, CuCl2 solution, mechanical properties, ultrasound technique.
1. Introduction
TheBaCl2 is a water-soluble synthetic polymer, due to the characteristics of easy preparation, good
biodegradability, excellent chemical resistance, and good mechanical properties, BaCl2 is used mainly as a
solution in water but its solubility in water depends on temperature, [1]. BaCl2 is available as colorless crystals
and salt barium is the most important and has high degradation in water .An improved understanding of the
excited state structure and dynamics in conjugated polymers should aid in the design of more efficient materials
for such applications. The prevailing view is that these materials can be thought of as collections of chain
segments with varying conjugation lengths, whose proximity to each other does not affect their fundamental
electronic structure, but whose intramolecular excision states interact via weak, Forster-type interactions [2]
Copper(II) chloride is the chemical compound with the formula CuCl2. This is a light brown solid, which slowly
absorbs moisture to form a blue-green dihydrate. The copper(II) chlorides are some of the most common
copper(II) compounds, after copper sulfate. Anhydrous CuCl2 adopts a distorted cadmium iodide structure. In
this motif, the copper centers are octahedral. Most copper(II) compounds exhibit distortions from idealized
octahedral geometry due to the Jahn-Teller effect, which in this case describes the localization of one d-electron
into a molecular orbital that is strongly antibonding with respect to a pair of chloride ligands. In CuCl2·2H2O, the
copper again adopts a highly distorted octahedral geometry, the Cu(II) centers being surrounded by two water
ligands and four chloride ligands, which bridge asymmetrically to other Cu centers solvent effects might
therefore be expected to influence the ultrasonic relation behavior, the absorption of ultrasonic in liquid systems
is governed by local modes of motion and cooperative whole molecule movement because of the strong
intermolecular interaction it should be possible to observe cooperative motion in the ultrasonic range.. 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.
Acoustic relaxation measurements on other solutions have been reported by several workers[8,9], 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 solutions
were carried by some workers using ultrasonic technique[10]. The purpose of this research was to investigate the
physical properties of BaCl2 with CuCl2 as aqueous solutions by ultrasound wave at fixed frequency (25 KHZ)
and study the effect of adding CuCl2 on the physical properties of BaCl2 to enhance its different applications.
2. Experimental:
2.1 Preparation of Solutions:
BaCl2 (Gerhard Buchman –Germany) with assay (99%) and CuCl2 (Messina) with assay (99.8%) [11] .The
BaCl2 solutions were prepared by dissolving a known weights of BaCl2 powder in a fixed volume (400 ml) of
Advances in Physics Theories and Applications www.iiste.org
ISSN 2224-719X (Paper) ISSN 2225-0638 (Online)
Vol.20, 2013
135
distilled water under stirring at 70oC for ( 30 min). The BaCl2 concentrations were (0.05%, 0.1%, 0.15 %, 0.2%,
0.25% and 0.3%) gm./ ml ; then CuCl2 was added with weight (0.3 gm.) to all BaCl2 Concentrations. The
resulting solution was stirred continuously for (30 min) until the solution mixture became a homogeneous.
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 constant frequency (25 KHz),as shown in Fig. below the receiver quartz crystal mounted
on a digital venire 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).
The instruments of ultrasonic system
2.3 Theoretical calculations:
The absorption coefficient (α ) was calculated from Lambert – Beer law[12]:
)1(/ )(
0 LLLx
eAA α−
=
Where ( 0A ) is the initially amplitude of the ultrasonic waves,( A ) is the wave amplitude after absorption and
( x ) is the thickness of the sample.
The ultrasonic wave velocity (V ) was calculated using the following equation[13]:
)2(/ LLLtxV =
Where (t ) is time that the waves need to cross the samples (digital obtained from the instrument). Attenuation
is generally proportional to the square of sound frequency so the relaxation amplitude ( D ) was calculated from
the following equation[14] where ( f ) is the ultrasonic frequency:
)3(2
LLL
f
D
α
=
The acoustic impedance of a medium ( Z ), it was calculated by equation[15]:
)4(LLLVZ ρ=
Bulk modulus ( K ) is the substance's resistance to uniform compression, it is defined as the pressure increase
needed to decrease the volume; it was calculated by Laplace equation[16] :
)5(2
LLLVK ρ=
Compressibility ( B ) is a measure of the relative volume change of a fluid or solid as a response to a pressure (or
mean stress) change, it was calculated by the following equation[17]:
)6()( 12
LLL−
= VB ρ
The relaxation time (τ ) was calculated from the equation[18]:
)7(34 2
LLLVS ρητ =
Advances in Physics Theories and Applications www.iiste.org
ISSN 2224-719X (Paper) ISSN 2225-0638 (Online)
Vol.20, 2013
136
3. Results and Discussion:
(Fig.2) shows that absorption coefficient is increasing with concentration this attributed to the fact that when
polymer concentration increase 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 [15], this behavior same to that give by [19] for other polymers, adding CuCl2 enhances absorption
coefficient by increasing its values. This attributed that there were more flexibility for these polymer chains in
solution as a result of adding CuCl2 molecules, and because ultrasonic waves propagate as compression and
rarefaction in a medium so there are variation in density medium and there were more attenuation to energy of
ultrasound waves when adding CuCl2[20]. Ultrasonic velocity is increasing with increasing CuCl2 as shown in
(Fig.1) 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 so when adding CuCl2
the vacancies were accupied by these molecules lead to increases the velocity [21].. The compressibility is
decreasing with the increase of concentration (Fig.3) and attributed to the fact that in Laplace equation no. (6)
There are inverse proportionality between compressibility and ultrasonic velocity [23, 24]. Ultrasonic relaxation
time was calculated by using equation no. (7) Shown in (Fig.4) and the relaxation amplitude shown in (Fig.5)
calculated from equation no.(3) their values are increasing with concentration, this behavior same to that give by
[19] for other polymers, also (Fig.4) Shows that relaxation time decreased when adding CuCl2 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 and since CuCl2 increase velocity so
relaxation time must decrease [18] Specific acoustic impedance shown in (Fig.6) is increasing with
concentrations this behavior same to that given by [25] for other polymers and attributed to the equation no. (4)
has only one variable parameter which is velocity and density has very small variations with respect to that of
velocity. And the bulk modulus is increasing with concentration (Fig.7) ; this behavior same to that give by
[26].(Fig.6) shows that adding CuCl2 increased acoustic impedance because CuCl2 chains fills the valances by
swallowing water molecules and be closer to BaCl2 macromolecules that increasing Specific acoustic
impedance[27].
4. Conclusion
1. Adding CuCl2 polymer to BaCl2 enhances the ultrasonic absorption coefficient as a result of high values
after addition so it can be used as coated materials for moving bodies in order to detect its by ultrasonic
technique .
2.Adding CuCl2 increases the ultrasonic velocity so it can be used as good medium for transforming ultrasonic
waves in such medical instruments.
3. Adding CuCl2 reduced compressibility this lead to increase interaction between polymer molecules this
cause enhancement for mechanical properties against environments .
References
1.Greenwood, N. N. and Earnshaw, A. (1997). Chemistry of the Elements (2nd Edn.), Oxford:Butterworth-
Heineman.
2. Jayanta Chakraborty, Jayashri Sarkar, Ravi Kumar and Giridhar Madra (2004) “Ultrasonic Degradation of
Poly butadiene and Isotactic Polypropylene”, Polymer Degradation and Stability, Elsevier, 85(1).
3. Krishna, Palakodety Radha; G. Dayaker (2007). "A stereoselective total synthesis of (-)-andrachcinidine via
an olefin cross-metathesis protocol". Tetrahedron Letters (Elsevier) 48 (41): 7279–7282.
doi:10.1016/j.tetlet.2007.08.053.
4. Chapman , A. Hallp E “Thickening and Gelling Agents for food” , 2002.
5. Anon, "Society of Petroleum Eng. of AIME J.". Pub. by Soc. of Pc. Eng. of AIME. USA, P. 482, 1985.
6. Biswal DR, Singh RP (2004) “Characterization of Carboxy methyl cellulose and poly acryl amide graft
copolymer”, Carbo hyd. Polymer, 57:379-387.
7. Edgar181, Source: "Own work by uploader " , 14:36, 16 October 2008 (UTC).
8. Poly (Ethylene Glycol) Coating on the Acoustic Properties of Biocompatible Magnetic Fluid”, International
Journal of Thermo physics. Springer link, 31(1), 70–76.
9. Khalida,H.H. (2004) “Study of Structural and Visco-Relaxation of Polycarbonates Solutions by Ultrasonic
Technique”, Journal of Al-Qadisiya of Pure Sciences, 9(3),188-122.
10. B. Boro Djordjevi (2009) “Ultrasonic characterization of advanced composite materials” the
10thInternational Conference of the Slovenian Society for Non- Destructive Testing (Application of
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Vol.20, 2013
137
Contemporary Non-Destructive Testing in Engineering), Ljubljana, Slovenia, 47-57.
11. Messina incorporated “product data”, Travis suite 520 Data, Texas. p. 22,1998.
12. Zong fang Wu1 and Dong C. Liu (2011) “Method of improved scattered size estimation without Attenuation
known a priori” Bioinformatics and Biomedical Engineering (ICBBE), 4th International Conference, IEEE,
8(10).1- 4.
13. Boutouyrie P, Briet M, Collin C, Vermeersch S and Pannier B (2009) “Assessment of pulse wave velocity”,
ArteryResearch, 3 (1), 3–8..
14. Josef and Herbert Krautkramer (1990) “Ultrasonic testing of materials” 4th
edition, Springer.
15. Jarth Mc-Hugh (2008). a thesis PhD Bundesanstalt fur Material for schung und - prufung (BAM), Germany.
16. Siddhartha Roy ,Alexander Winner ,Tillman Beck Thomas Studnitzky and Gunter Stephanie (2011)
“Mechanical properties of cellular solids produced from hollow stainless steel spheres” J Mater Sci ,46:5519–
5526.
17. 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.
18. Curi E.,Campana S. (2006), Journal of Macromolecules science chem.A431,4.
19. Ehssan D.J, a thesis M.Sc (2004) “Gamma relaxation effect on some physical properties of polymer xanzan
cellulose” university of Babylon.
20. Alaa J. Kadham Algidsawi, Ahmed Hashim and Hayder J. Kadham Algidsawi (2011) “The Effect of
(LiFCuCl2.2H2O) on Mechanical Properties of Poly-Vinyl Alcohol”, European Journal of Scientific Research,
65 (1) , 74-78.
21. Oudry J, Bastard C, Miette V, Willinger R and Sandrin L(2009) ”Ultrasound Medical Biolology”,1185-97
22. T.G. Lazareva and E.V. Shingareva (2002) ʻʻ Rheological and Electrophysical Characteristics of polyvinyl
Alcohol and water- soluble Carboxymethyl Celluloseˮ, Russian Journal of Applied Chemistry, 75, (10), 1688-
1691.
23. Oudry J, Bastard C, Miette V, Willinger R and Sandrin L(2009) ”Ultrasound Medical Biolology”,1185-97.
24. Al-Bermany K.J. (2010) “Enhancement of mechanical properties using gamma radiation for HEC Polymer”,
Journal of college of Education, Babylon University, 1(5), 10-15.
25. Ahmed Hashim, Alaa J. Kadham Algidsawi, Hayder J. Kadham Algidsawi and Shaymaa Hadi (2011)ʻʻ
Mechanical Properties of (PVA-CoNO3, BaSO4.5H2O) Compositesˮ, European Journal of Scientific Research,
65(2) , 163-167.
26. Abdul-Kareem J. Rashid, Ehssan Dhiaa Jawad and Burak Y. Kadem (2011) “A Study of Some Mechanical
Properties of Iraqi Palm Fiber-PVA Composite by Ultrasonic” European Journal of Scientific Research, 61 (2).
203-209.
27. Martin F.D and Kuntamukula M, “polymeric Material science and Engineering” v.72,pub. , 2001.
0
500
1000
1500
2000
2500
3000
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35
UltrasonicVelocity(m/sec)
Concentration(gm/ml)%
BaCl2
BaCl2+0.3gmCuCl2
Fig.1. Ultrasonic Velocity due to concentration
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ISSN 2224-719X (Paper) ISSN 2225-0638 (Online)
Vol.20, 2013
138
0
50
100
150
200
250
0 0.05 0.1 0.15 0.2 0.25 0.3
UltrasonicAbsorption
Coefficient(m-1)
Concentration(gm/ml)%
BaCl2
BaCl2+0.3gm CuCl
Fig.2. Absorption coefficient due to concentration
0
0.5
1
1.5
2
2.5
3
3.5
4
0 0.1 0.2 0.3
Compressibility*10-6
(m.sec2/kg)
Concentration(gm/ml)%
BaCl2
BaCl2+0.3gm CuCl
Fig.3. Compressibility due to concentration
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ISSN 2224-719X (Paper) ISSN 2225-0638 (Online)
Vol.20, 2013
139
0
1
2
3
4
5
6
0 0.1 0.2 0.3 0.4
Relaxationtime*10-11
(sec)
Concentration(gm/ml)%
BaCl2
BaCl2+0.3gmCuCL2
Fig.4. Relaxation time due to concentration
0
5
10
15
20
25
30
35
0 0.1 0.2 0.3 0.4
RelaxationAmplitude*10-8
(sec2/m)
Concentration(gm/ml)%
BaCl2
BaCl2+0.3gmCuCl2
Fig.5. Relaxation amplitude due to concentration
Advances in Physics Theories and Applications www.iiste.org
ISSN 2224-719X (Paper) ISSN 2225-0638 (Online)
Vol.20, 2013
140
0
5
10
15
20
25
30
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35
SpecificAcousticImpedance*105
(kg/m2.sec)
Concentration(gm/ml)%
BaCl2
BaCl2+0.3gmCuCl2
Fig. 6.Acoustic impedance due to concentration
0
10
20
30
40
50
60
70
0 0.1 0.2 0.3
BulkModulus*108
(kg/m.sec2)
Concentration(gm/ml)%
BaCl2
BaCl2+0.3gm CuCl
Fig.7. Bulk Modulus due to concentration
This academic article was published by The International Institute for Science,
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Enhancement mechanical properties of barium chloride by adding copper chloride using ultrasonic technique

  • 1. Advances in Physics Theories and Applications www.iiste.org ISSN 2224-719X (Paper) ISSN 2225-0638 (Online) Vol.20, 2013 134 Enhancement Mechanical Properties of Barium Chloride by Adding Copper Chloride using Ultrasonic Technique Prof.Dr.Abdul-Kareem J. Al-Bermany(Corresponding author) Babylon University / Facility of Science /Physics Department /Advanced polymer laboratory E-Mail: dr.abdulkaream@yahoo.com Burak Yahya Kadem E-Mail burakwh@yahoo.com Lamis Faaz Naser Babylon University / Facility of Science /Physics Department /Advanced polymer laboratory SShh-Phy@yahoo.com Abstract: Some of physical properties of BaCl2 dissolves in distilled water had been studied at different concentrations (0.05%, 0.1%, 0.15%, 0.2%, 0.25% and 0.3%) (gm./ml) before and after adding (0.3)gm of CuCl2 for all concentrations , the mechanical properties such as ultrasonic velocity had been measured by ultrasonic waves system at frequency 25 KHz, other mechanical properties had been calculated such as absorption coefficient of ultrasonic waves, relaxation time, relaxation amplitude, specific acoustic impedance, compressibility and bulk modules. The results show that all these properties are increasing with the increase of the polymer concentration except compressibility is decreasing with the increase of the concentration; results show that when adding CuCl2 these properties are increasing except compressibility is decreasing. Results also shows that adding CuCl2 to BaCl2 enhances the ultrasonic absorption coefficient as a result of high values after addition. Keywords: BaCl2 solution, CuCl2 solution, mechanical properties, ultrasound technique. 1. Introduction TheBaCl2 is a water-soluble synthetic polymer, due to the characteristics of easy preparation, good biodegradability, excellent chemical resistance, and good mechanical properties, BaCl2 is used mainly as a solution in water but its solubility in water depends on temperature, [1]. BaCl2 is available as colorless crystals and salt barium is the most important and has high degradation in water .An improved understanding of the excited state structure and dynamics in conjugated polymers should aid in the design of more efficient materials for such applications. The prevailing view is that these materials can be thought of as collections of chain segments with varying conjugation lengths, whose proximity to each other does not affect their fundamental electronic structure, but whose intramolecular excision states interact via weak, Forster-type interactions [2] Copper(II) chloride is the chemical compound with the formula CuCl2. This is a light brown solid, which slowly absorbs moisture to form a blue-green dihydrate. The copper(II) chlorides are some of the most common copper(II) compounds, after copper sulfate. Anhydrous CuCl2 adopts a distorted cadmium iodide structure. In this motif, the copper centers are octahedral. Most copper(II) compounds exhibit distortions from idealized octahedral geometry due to the Jahn-Teller effect, which in this case describes the localization of one d-electron into a molecular orbital that is strongly antibonding with respect to a pair of chloride ligands. In CuCl2·2H2O, the copper again adopts a highly distorted octahedral geometry, the Cu(II) centers being surrounded by two water ligands and four chloride ligands, which bridge asymmetrically to other Cu centers solvent effects might therefore be expected to influence the ultrasonic relation behavior, the absorption of ultrasonic in liquid systems is governed by local modes of motion and cooperative whole molecule movement because of the strong intermolecular interaction it should be possible to observe cooperative motion in the ultrasonic range.. 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. Acoustic relaxation measurements on other solutions have been reported by several workers[8,9], 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 solutions were carried by some workers using ultrasonic technique[10]. The purpose of this research was to investigate the physical properties of BaCl2 with CuCl2 as aqueous solutions by ultrasound wave at fixed frequency (25 KHZ) and study the effect of adding CuCl2 on the physical properties of BaCl2 to enhance its different applications. 2. Experimental: 2.1 Preparation of Solutions: BaCl2 (Gerhard Buchman –Germany) with assay (99%) and CuCl2 (Messina) with assay (99.8%) [11] .The BaCl2 solutions were prepared by dissolving a known weights of BaCl2 powder in a fixed volume (400 ml) of
  • 2. Advances in Physics Theories and Applications www.iiste.org ISSN 2224-719X (Paper) ISSN 2225-0638 (Online) Vol.20, 2013 135 distilled water under stirring at 70oC for ( 30 min). The BaCl2 concentrations were (0.05%, 0.1%, 0.15 %, 0.2%, 0.25% and 0.3%) gm./ ml ; then CuCl2 was added with weight (0.3 gm.) to all BaCl2 Concentrations. The resulting solution was stirred continuously for (30 min) until the solution mixture became a homogeneous. 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 constant frequency (25 KHz),as shown in Fig. below the receiver quartz crystal mounted on a digital venire 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). The instruments of ultrasonic system 2.3 Theoretical calculations: The absorption coefficient (α ) was calculated from Lambert – Beer law[12]: )1(/ )( 0 LLLx eAA α− = Where ( 0A ) is the initially amplitude of the ultrasonic waves,( A ) is the wave amplitude after absorption and ( x ) is the thickness of the sample. The ultrasonic wave velocity (V ) was calculated using the following equation[13]: )2(/ LLLtxV = Where (t ) is time that the waves need to cross the samples (digital obtained from the instrument). Attenuation is generally proportional to the square of sound frequency so the relaxation amplitude ( D ) was calculated from the following equation[14] where ( f ) is the ultrasonic frequency: )3(2 LLL f D α = The acoustic impedance of a medium ( Z ), it was calculated by equation[15]: )4(LLLVZ ρ= Bulk modulus ( K ) is the substance's resistance to uniform compression, it is defined as the pressure increase needed to decrease the volume; it was calculated by Laplace equation[16] : )5(2 LLLVK ρ= Compressibility ( B ) is a measure of the relative volume change of a fluid or solid as a response to a pressure (or mean stress) change, it was calculated by the following equation[17]: )6()( 12 LLL− = VB ρ The relaxation time (τ ) was calculated from the equation[18]: )7(34 2 LLLVS ρητ =
  • 3. Advances in Physics Theories and Applications www.iiste.org ISSN 2224-719X (Paper) ISSN 2225-0638 (Online) Vol.20, 2013 136 3. Results and Discussion: (Fig.2) shows that absorption coefficient is increasing with concentration this attributed to the fact that when polymer concentration increase 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 [15], this behavior same to that give by [19] for other polymers, adding CuCl2 enhances absorption coefficient by increasing its values. This attributed that there were more flexibility for these polymer chains in solution as a result of adding CuCl2 molecules, and because ultrasonic waves propagate as compression and rarefaction in a medium so there are variation in density medium and there were more attenuation to energy of ultrasound waves when adding CuCl2[20]. Ultrasonic velocity is increasing with increasing CuCl2 as shown in (Fig.1) 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 so when adding CuCl2 the vacancies were accupied by these molecules lead to increases the velocity [21].. The compressibility is decreasing with the increase of concentration (Fig.3) and attributed to the fact that in Laplace equation no. (6) There are inverse proportionality between compressibility and ultrasonic velocity [23, 24]. Ultrasonic relaxation time was calculated by using equation no. (7) Shown in (Fig.4) and the relaxation amplitude shown in (Fig.5) calculated from equation no.(3) their values are increasing with concentration, this behavior same to that give by [19] for other polymers, also (Fig.4) Shows that relaxation time decreased when adding CuCl2 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 and since CuCl2 increase velocity so relaxation time must decrease [18] Specific acoustic impedance shown in (Fig.6) is increasing with concentrations this behavior same to that given by [25] for other polymers and attributed to the equation no. (4) has only one variable parameter which is velocity and density has very small variations with respect to that of velocity. And the bulk modulus is increasing with concentration (Fig.7) ; this behavior same to that give by [26].(Fig.6) shows that adding CuCl2 increased acoustic impedance because CuCl2 chains fills the valances by swallowing water molecules and be closer to BaCl2 macromolecules that increasing Specific acoustic impedance[27]. 4. Conclusion 1. Adding CuCl2 polymer to BaCl2 enhances the ultrasonic absorption coefficient as a result of high values after addition so it can be used as coated materials for moving bodies in order to detect its by ultrasonic technique . 2.Adding CuCl2 increases the ultrasonic velocity so it can be used as good medium for transforming ultrasonic waves in such medical instruments. 3. Adding CuCl2 reduced compressibility this lead to increase interaction between polymer molecules this cause enhancement for mechanical properties against environments . References 1.Greenwood, N. N. and Earnshaw, A. (1997). Chemistry of the Elements (2nd Edn.), Oxford:Butterworth- Heineman. 2. Jayanta Chakraborty, Jayashri Sarkar, Ravi Kumar and Giridhar Madra (2004) “Ultrasonic Degradation of Poly butadiene and Isotactic Polypropylene”, Polymer Degradation and Stability, Elsevier, 85(1). 3. Krishna, Palakodety Radha; G. Dayaker (2007). "A stereoselective total synthesis of (-)-andrachcinidine via an olefin cross-metathesis protocol". Tetrahedron Letters (Elsevier) 48 (41): 7279–7282. doi:10.1016/j.tetlet.2007.08.053. 4. Chapman , A. Hallp E “Thickening and Gelling Agents for food” , 2002. 5. Anon, "Society of Petroleum Eng. of AIME J.". Pub. by Soc. of Pc. Eng. of AIME. USA, P. 482, 1985. 6. Biswal DR, Singh RP (2004) “Characterization of Carboxy methyl cellulose and poly acryl amide graft copolymer”, Carbo hyd. Polymer, 57:379-387. 7. Edgar181, Source: "Own work by uploader " , 14:36, 16 October 2008 (UTC). 8. 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  • 4. Advances in Physics Theories and Applications www.iiste.org ISSN 2224-719X (Paper) ISSN 2225-0638 (Online) Vol.20, 2013 137 Contemporary Non-Destructive Testing in Engineering), Ljubljana, Slovenia, 47-57. 11. Messina incorporated “product data”, Travis suite 520 Data, Texas. p. 22,1998. 12. Zong fang Wu1 and Dong C. Liu (2011) “Method of improved scattered size estimation without Attenuation known a priori” Bioinformatics and Biomedical Engineering (ICBBE), 4th International Conference, IEEE, 8(10).1- 4. 13. Boutouyrie P, Briet M, Collin C, Vermeersch S and Pannier B (2009) “Assessment of pulse wave velocity”, ArteryResearch, 3 (1), 3–8.. 14. Josef and Herbert Krautkramer (1990) “Ultrasonic testing of materials” 4th edition, Springer. 15. Jarth Mc-Hugh (2008). a thesis PhD Bundesanstalt fur Material for schung und - prufung (BAM), Germany. 16. Siddhartha Roy ,Alexander Winner ,Tillman Beck Thomas Studnitzky and Gunter Stephanie (2011) “Mechanical properties of cellular solids produced from hollow stainless steel spheres” J Mater Sci ,46:5519– 5526. 17. 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. 18. Curi E.,Campana S. (2006), Journal of Macromolecules science chem.A431,4. 19. Ehssan D.J, a thesis M.Sc (2004) “Gamma relaxation effect on some physical properties of polymer xanzan cellulose” university of Babylon. 20. Alaa J. Kadham Algidsawi, Ahmed Hashim and Hayder J. Kadham Algidsawi (2011) “The Effect of (LiFCuCl2.2H2O) on Mechanical Properties of Poly-Vinyl Alcohol”, European Journal of Scientific Research, 65 (1) , 74-78. 21. Oudry J, Bastard C, Miette V, Willinger R and Sandrin L(2009) ”Ultrasound Medical Biolology”,1185-97 22. T.G. Lazareva and E.V. Shingareva (2002) ʻʻ Rheological and Electrophysical Characteristics of polyvinyl Alcohol and water- soluble Carboxymethyl Celluloseˮ, Russian Journal of Applied Chemistry, 75, (10), 1688- 1691. 23. Oudry J, Bastard C, Miette V, Willinger R and Sandrin L(2009) ”Ultrasound Medical Biolology”,1185-97. 24. Al-Bermany K.J. (2010) “Enhancement of mechanical properties using gamma radiation for HEC Polymer”, Journal of college of Education, Babylon University, 1(5), 10-15. 25. Ahmed Hashim, Alaa J. Kadham Algidsawi, Hayder J. Kadham Algidsawi and Shaymaa Hadi (2011)ʻʻ Mechanical Properties of (PVA-CoNO3, BaSO4.5H2O) Compositesˮ, European Journal of Scientific Research, 65(2) , 163-167. 26. Abdul-Kareem J. Rashid, Ehssan Dhiaa Jawad and Burak Y. Kadem (2011) “A Study of Some Mechanical Properties of Iraqi Palm Fiber-PVA Composite by Ultrasonic” European Journal of Scientific Research, 61 (2). 203-209. 27. Martin F.D and Kuntamukula M, “polymeric Material science and Engineering” v.72,pub. , 2001. 0 500 1000 1500 2000 2500 3000 0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 UltrasonicVelocity(m/sec) Concentration(gm/ml)% BaCl2 BaCl2+0.3gmCuCl2 Fig.1. Ultrasonic Velocity due to concentration
  • 5. Advances in Physics Theories and Applications www.iiste.org ISSN 2224-719X (Paper) ISSN 2225-0638 (Online) Vol.20, 2013 138 0 50 100 150 200 250 0 0.05 0.1 0.15 0.2 0.25 0.3 UltrasonicAbsorption Coefficient(m-1) Concentration(gm/ml)% BaCl2 BaCl2+0.3gm CuCl Fig.2. Absorption coefficient due to concentration 0 0.5 1 1.5 2 2.5 3 3.5 4 0 0.1 0.2 0.3 Compressibility*10-6 (m.sec2/kg) Concentration(gm/ml)% BaCl2 BaCl2+0.3gm CuCl Fig.3. Compressibility due to concentration
  • 6. Advances in Physics Theories and Applications www.iiste.org ISSN 2224-719X (Paper) ISSN 2225-0638 (Online) Vol.20, 2013 139 0 1 2 3 4 5 6 0 0.1 0.2 0.3 0.4 Relaxationtime*10-11 (sec) Concentration(gm/ml)% BaCl2 BaCl2+0.3gmCuCL2 Fig.4. Relaxation time due to concentration 0 5 10 15 20 25 30 35 0 0.1 0.2 0.3 0.4 RelaxationAmplitude*10-8 (sec2/m) Concentration(gm/ml)% BaCl2 BaCl2+0.3gmCuCl2 Fig.5. Relaxation amplitude due to concentration
  • 7. Advances in Physics Theories and Applications www.iiste.org ISSN 2224-719X (Paper) ISSN 2225-0638 (Online) Vol.20, 2013 140 0 5 10 15 20 25 30 0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 SpecificAcousticImpedance*105 (kg/m2.sec) Concentration(gm/ml)% BaCl2 BaCl2+0.3gmCuCl2 Fig. 6.Acoustic impedance due to concentration 0 10 20 30 40 50 60 70 0 0.1 0.2 0.3 BulkModulus*108 (kg/m.sec2) Concentration(gm/ml)% BaCl2 BaCl2+0.3gm CuCl Fig.7. Bulk Modulus due to concentration
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