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Original article
9 (
1_suppl
); S373-S378
doi:
10.1016/j.arabjc.2011.05.007

Metallic and non-metallic anionic interaction activities estimated with sound velocity and refractive index

School of Chemical Sciences, Central University of Gujarat, Gandhinagar 382030, India

⁎Corresponding author. Tel.: +91 079 23260210; fax: +91 079 23260076. mansingh50@hotmail.com (Man Singh),

Disclaimer:
This article was originally published by Elsevier and was migrated to Scientific Scholar after the change of Publisher.

Peer review under responsibility of King Saud University.

Abstract

Density (ρ ± 10−3 kg m−3), sound velocity (VS ± 10−2 ms−1) as acoustic property and refractive index (μri ± 10−4) for 0.01–0.1 m K2Cr2O7, K2HPO4, KMnO4, KH2PO4, KCl, and KOH aqueous salts with compressibility attained with ion–solvent interaction (ISI) are reported at 0.01 interval and 293.15 K. Ionic internal pressure generated with ISI is expressed as adiabatic compressibility (β, pa−1) with relative change (Δβ/β0) and apparent molal compressibility (ϕk, m2N−1) with specific ionic activities for metallic and non-metallic anions. Linear regression generated V S 0 , μ ri 0 , ϕk0, and β0 as limiting data for analysis of speed of light and sound. The V S 0 as KH2PO4 > K2HPO4 > KOH > K2Cr2O7 > KCl > KMnO4 denoted a minimum V S 0 metallic anions. With concentrations, the sound velocity and refractive index are noted as ISI functions where the sound and light waves were in opposite trends. The Mn0 and Cr0 transitional metals with anions of the K2Cr2O7 and KMnO4 have affected the compressibility as K2Cr2O7 > KMnO4 due to 2Cr+6. The V S 0 , μ ri 0 , ϕk0, and β0 analyzed their ionic strengths in comparison to HPO 4 - , H 2 PO 4 - , Cl, and OH as non-metallic anions considering the interactions as sensors. A molionic model of ion–water interaction was proposed to generalize ion-molecular interactions in industrial mixtures.

Keywords

Sound velocity
Light velocity
Refractive index
Solute solvent interaction
Adiabatic compressibility
Apparent molal compressibility
1

1 Introduction

The VS of ionic liquids (ILs) as a physicochemical indicator does analyze several internal properties, such as residual stress, hardness, grain size micro structure, elastic constant, medicinal engineering, and agriculture (Sumathi and Varalakshmi, 2010). Conceptually, the sound as energy travels through a medium such as air or water, as a compressed phase, where pressure variations bring changes and its waves travel through particles of interacting species within fixed interfaces. The ionic or internal activities significantly cause interruptions in travel due to ISI, where a cycle of wave varies with the compressibility. The compressibility as function of the type and nature of bonds critically furnish useful information about ionic–molecular interactions. Recently, the VS data are used to elucidate an interpreted ISI in liquid medium (Baluja and Oza, 2005; Rawat and Sangeeta, 2008; Ali and Nain, 1996; Ogawa and Murakami, 1987) as the salts disrupt hydrogen bonding forming new structural reorientation. Thus the data infer ion–solvent configurations with different ionic pressure due to intrinsic hydration structures. Therefore, the ionic interactions exerted internal pressure which is also studied with Debye–Hückel ionic theory (Debye and Hückel, 1923), and fitted in present study. For understanding a role of ion polar interaction force, several parameters, such as β, Δβ, Δβ/β0, and ϕk were studied to find structural arrangements with relative strength of various types of intermolecular or inter ionic interactions. Thus, the ISI created a compressed medium for traveling velocities.

The μri is an optical in nature for analyzing optical properties of materials whose values are often required to interpret spectroscopic data (Singh, 2002). Light absorbing capacity as characteristic feature develops a mediate light accepter device to design physically, biologically and chemically stability of the compounds or solutions. The μri is a most authentic optical data plays key role in various areas of material science for designing thin film technology and others. Similarly, the μri data are widely used for determination of solution concentrations (Subedi et al., 2006). Thus the μri study exhibits efficient optical functions for developing an optical device with such liquids which are studied in the present work. The present study showed that the ISI increased the μri and decreased the speed of light in water due to compressibility. The VS and μri in the present study for salts solution offered understanding the behavior of AIL. Knowledge of the VS and μri of electrolyte solutions is extremely important to identify their internal and external properties. Such structural ionic activities with corresponding state of hydrogen bonding could be studied with the VS and μri. For example, observed V S 0 values as KH2PO4 > K2HPO4 > KOH > K2Cr2O7 > KCl > KMnO4 and μ ri 0 as KMnO4 > KH2PO4 > KOH > K2HPO4 > KCl > K2Cr2O7 inferred comparative analysis of the ionic interactions in our study. The VS and μri parameters on HPO 4 - , H 2 PO 4 - , Cl, OH, and Cr 2 O 7 - MnO 4 - , and similar others could act as authentic non-metallic and metallic anionic interaction sensors, respectively. The study predicted that the number of anionic metals with oxidation states plays an effective role to produce internal pressure and affected the VS which is less than μri. An interesting property of solution as wave conservation is studied. Thus the metallic and non-metallic anionic studies are highly significant but are not reported yet. Interestingly more and more ionic liquid systems if are subjected to such studies then their data trends and magnitudes do illustrate the nature and size of the ions with respect to medium and polarity. Thus the K2Cr2O7, K2HPO4, KMnO4, KH2PO4, KCl, and KOH aqueous mixtures were chosen to exactly investigate the effect of metallic and nonmetallic ions on water structures vis-a-vis the acoustic property of the mixtures.

2

2 Experimental methods

2.1

2.1 Chemicals and solvents

Chemicals (99.99%, AR, K2Cr2O7, K2HPO4, KMnO4, KH2PO4, KCl, KOH, Ranbaxy, India) were used as received. Milli-Q water was used as a solvent.

2.2

2.2 Analytical conditions

The experiment was done at 293.15 K. Solutions w/w were prepared with Milli-Q water of 10−6 μ S cm−1 conductance with electronic Kern ABS 220-4 model balance with ±0.01 mg accuracy. The ρ and VS data with 10−3kg m−3 and 10−2 ms−1, respectively, were measured with density and sound velocity meter DSA 5000M whose quartz U tube was cleaned with acetone after each measurement. The equipment works on a theory of oscillation periods of U tube for air, solvent and solutions (Pal et al., 2010). The μri was measured with ±10−4 using Rudolph Research analytical J series Refractometer model 57. Its sample plate was properly cleaned and dried each time with acetone. The measurements for water values were repeated several times to ensure calibration and reproducibility of the equipment. The μri literature value of the water was 1.3328 which very closely matched with experimental values of water. The precision and reproducibility of measured data along with 95.5% confidence variance were noted with highly reproducibility. Similarly the VS experimental value was 1482.69 ms−1 for water and had shown striking agreements with literature values.

3

3 Calculations

Densities were applied for adiabatic compressibility (Mason, 1929) calculation with Eq. (1).

(1)
β = 1 / V S × ρ 0

The VS and ρ0 are sound velocity and density of solution and solvent, respectively. A variation in compressibility and relative change in adiabatic compressibility were calculated with Eqs. 2 and 3, respectively.

(2)
Δ β = β - β 0
(3)
Δ β / β 0

The β0 a water adiabatic compressibility = 4.56 × 107 pa−1 was calculated with Eq. (1). The apparent molal compressibility was calculated with Eq. (4).

(4)
Φ k = 1000 / m · ρ 0 ( ρ 0 β - β 0 ρ ) + β 0 · M / ρ

The ρ0 and ρ are densities of solvent and solution, respectively, m is molality and M is molecular mass. The velocity of light (VL) is calculated with μri = VL (vacuum)/VL (medium) as the VL = 2.99 × 108 = 3.00 × 108 m/s in vacuum (Newcomb, 1886) was used.

4

4 Results and discussion

4.1

4.1 The VS, VL, and V S 0 , μ ri 0 and concentration study for comparative ionic interactions

The concentration effect on VS and μri was analyzed from data given in Table 1 and showed increases in VS and μri with increase in concentration and VL was decreased. The VS and μri directly determined internal pressure and ionic hydration with salt’s interactions which formed a high compact continuous medium through which the sound and light waves traveled. Thus the ISI forces developed a denser medium that manifolded the sound speed with a decrease in light velocity. The ISI created anion-hydration and partly the unengaged water with the similar molecules as a homogeneous medium. Thus a pattern of ion-hydration is different with each salt and inferred interaction as important information about a medium characterization that increased VS and decreased VL. It is observed that an increase in concentration is accompanied with an increase in internal pressure. For example, VS is 343.2 m/s in air and 1482.69 m/s with water while VL is 3 × 108 m/s in vacuum but VL in water is 2.5209 m/s. Thus, the K2Cr2O7, K2HPO4, KMnO4, KH2PO4, KCl, and KOH interactions have increased and decreased VS and VL, respectively (Table 1). It inferred that the ISI enhanced and exerted a higher internal pressure where an increase in VS is accompanied with a decrease in VL, depicted in Fig. 1. Both VS and VL are mutually inversely proportional due to an additional resistance and compressibility, respectively, with concentration. With salts Table 1 shows a percentage increase in VS with approximately equal decrease in VL. It is similar to energy conservation as partly the energy is consumed and the same amount of energy is appeared in another form. Thereby it seems an interesting property of solution that inferred absorption of a certain amount of a particular wave and the same amount of another form is exhibited as wave conservation.

Table 1 Molality (m), density (ρ ± 10−3 kg m−3), sound velocity (VS ± 10−2 ms−1), %VS ± 102, adiabatic compressibility (β ± 10−4 pa−1), change in adiabatic compressibility (Δβ ± 10−4 pa−1), relative change in adiabatic compressibility (Δβ/β0 ± 10−4), apparent molal compressibility (ϕk ± m2N−1), refractive index (μri ± 104), velocity of light (VL ± 103 ms−1), % of light velocity (%VL ± 102).
m ρ VS %VS β× 107 −Δβ × 109 −Δβ/β0 −ϕk × 105 μri VL × 108 %VL
K2Cr2O7
0.01 1.000141 1483.10 0.03 4.5457 1.1200 0.0025 6.5305 1.3333 2.250 0.03
0.02 1.002287 1483.80 0.07 4.5317 2.5212 0.0055 8.4544 1.3339 2.249 0.08
0.03 1.004207 1484.50 0.12 4.5187 3.8140 0.0084 8.3909 1.3344 2.248 0.12
0.04 1.006180 1485.20 0.17 4.5056 5.1251 0.0112 8.4651 1.3349 2.247 0.15
0.05 1.008154 1485.70 0.20 4.4938 6.3100 0.0138 8.2581 1.3354 2.247 0.19
0.06 1.010119 1486.41 0.25 4.4807 7.6125 0.0167 8.3094 1.3360 2.246 0.24
0.07 1.012228 1487.12 0.30 4.4671 8.9729 0.0197 8.5226 1.3365 2.245 0.27
0.08 1.014140 1487.73 0.34 4.4551 1.0181 0.0223 8.3793 1.3370 2.244 0.31
0.09 1.016366 1488.39 0.38 4.4414 1.1551 0.0253 8.6073 1.3375 2.243 0.35
0.10 1.018346 1489.07 0.43 4.4287 1.2819 0.0281 8.5757 1.3380 2.242 0.38
K2HPO4
0.01 0.999689 1484.16 0.10 4.5412 1.5639 0.0034 14.384 1.3332 2.250 0.03
0.02 1.001121 1485.90 0.22 4.5241 3.2748 0.0072 15.04 1.3334 2.250 0.04
0.03 1.002710 1487.66 0.34 4.5063 5.0599 0.0111 15.744 1.3338 2.249 0.07
0.04 1.004105 1489.03 0.43 4.4917 6.5137 0.0143 15.047 1.3340 2.249 0.09
0.05 1.005566 1490.79 0.55 4.4746 8.2247 0.0180 15.203 1.3342 2.249 0.10
0.06 1.007164 1492.62 0.67 4.4566 1.0029 0.0220 15.568 1.3345 2.248 0.12
0.07 1.008591 1493.92 0.76 4.4425 1.1434 0.0251 15.145 1.3348 2.248 0.15
0.08 1.010258 1495.85 0.89 4.4238 1.3311 0.0292 15.555 1.3351 2.247 0.17
0.09 1.011613 1497.44 0.99 4.4085 1.4841 0.0326 15.331 1.3353 2.247 0.18
0.10 1.012980 1498.68 1.08 4.3952 1.6164 0.0355 14.95 1.3356 2.246 0.21
KMnO4
0.01 0.999230 1482.76 0.00 4.5519 4.9826 0.0011 2.3833 1.3332 2.250 0.03
0.02 1.000350 1482.99 0.02 4.5454 1.1466 0.0025 3.3713 1.3336 2.250 0.06
0.03 1.001440 1483.23 0.04 4.539 1.7910 0.0039 3.6584 1.3339 2.249 0.08
0.04 1.002620 1483.73 0.07 4.5306 2.6294 0.0058 4.3793 1.3342 2.249 0.10
0.05 1.003560 1483.90 0.08 4.5253 3.1574 0.0069 3.9749 1.3346 2.248 0.13
0.06 1.005220 1484.10 0.10 4.5166 4.0274 0.0088 4.8244 1.3349 2.247 0.15
0.07 1.007310 1484.58 0.13 4.5043 5.2528 0.0115 6.2135 1.3351 2.247 0.17
0.08 1.008820 1484.98 0.15 4.4951 6.1724 0.0135 6.5502 1.3353 2.247 0.18
0.09 1.009120 1485.06 0.16 4.4933 6.3540 0.0139 5.3742 1.3357 2.246 0.21
0.10 1.011110 1485.52 0.19 4.4817 7.5160 0.0165 6.1858 1.3359 2.246 0.23
KH2PO4
0.01 0.999230 1483.62 0.06 4.5466 1.0249 0.0022 8.6427 1.3331 2.250 0.02
0.02 1.000200 1484.60 0.13 4.5362 2.0662 0.0045 8.6403 1.3333 2.250 0.03
0.03 1.001170 1485.57 0.19 4.5259 3.0955 0.0068 8.5903 1.3335 2.250 0.05
0.04 1.002100 1486.50 0.26 4.5161 4.0798 0.0090 8.4082 1.3336 2.250 0.06
0.05 1.003060 1487.49 0.32 4.5057 5.1146 0.0112 8.4348 1.3338 2.249 0.07
0.06 1.004050 1488.47 0.39 4.4953 6.1528 0.0135 8.4793 1.3339 2.249 0.08
0.07 1.004840 1489.26 0.44 4.4871 6.9799 0.0153 8.0734 1.3341 2.249 0.09
0.08 1.005900 1490.35 0.52 4.4758 8.1091 0.0178 8.3051 1.3343 2.248 0.11
0.09 1.007000 1491.41 0.59 4.4646 9.2315 0.0203 8.4951 1.3344 2.248 0.12
0.10 1.007950 1492.36 0.65 4.4547 1.0222 0.0224 8.4501 1.3346 2.248 0.13
KCl
0.01 0.998680 1483.09 0.03 4.5524 4.4750 0.0010 3.1484 1.3330 2.251 0.01
0.02 0.999120 1483.71 0.07 4.5466 1.0305 0.0023 3.803 1.3331 2.250 0.02
0.03 0.999610 1484.34 0.11 4.5405 1.6386 0.0036 4.1718 1.3332 2.250 0.03
0.04 1.000090 1484.96 0.15 4.5345 2.2349 0.0049 4.3155 1.3333 2.250 0.03
0.05 1.000500 1485.41 0.18 4.5299 2.6940 0.0059 4.0613 1.3334 2.250 0.04
0.06 1.001050 1486.24 0.24 4.5224 3.4493 0.0076 4.496 1.3335 2.250 0.05
0.07 1.001660 1486.79 0.28 4.5163 4.0581 0.0089 4.6338 1.3336 2.250 0.06
0.08 1.001970 1487.12 0.30 4.5129 4.3982 0.0097 4.2311 1.3337 2.249 0.06
0.09 1.002460 1487.70 0.34 4.5072 4.9709 0.0109 4.2681 1.3338 2.249 0.07
0.10 1.003570 1489.03 0.43 4.4941 6.2747 0.0138 5.3128 1.3340 2.249 0.09
KOH
0.01 0.998580 1483.50 0.05 4.5503 6.5536 0.0014 5.631 1.3330 2.251 0.01
0.02 0.999070 1484.19 0.10 4.5439 1.3013 0.0029 5.883 1.3331 2.250 0.02
0.03 0.999490 1484.94 0.15 4.5374 1.9496 0.0043 5.8636 1.3332 2.250 0.03
0.04 0.999890 1485.63 0.20 4.5314 2.5518 0.0056 5.7184 1.3333 2.250 0.03
0.05 1.000320 1486.48 0.26 4.5242 3.2654 0.0072 5.8839 1.3334 2.250 0.04
0.06 1.000740 1487.13 0.30 4.5184 3.8505 0.0084 5.7711 1.3335 2.250 0.05
0.07 1.001220 1488.03 0.36 4.5108 4.6119 0.0101 5.9795 1.3336 2.250 0.06
0.08 1.001650 1488.86 0.42 4.5038 5.3104 0.0117 6.0332 1.3337 2.249 0.06
0.09 1.002110 1489.56 0.46 4.4975 5.9392 0.0130 6.0093 1.3337 2.249 0.06
0.10 1.002580 1490.43 0.52 4.4901 6.6765 0.0147 6.1059 1.3338 2.249 0.07
Relation between sound and light velocity.
Figure 1
Relation between sound and light velocity.

The V S 0 with KH2PO4 > K2HPO4 > KOH > K2Cr2O7 > KCl > KMnO4 sequence inferred higher internal pressure with the KH2PO4 and lowest for KMnO4 (Table 2). It is explained with pressure p = 1/volume v (Boyle’s law) relation where the density ρ = mass m/v. It marked the KH2PO4 with higher density that caused stronger ionic interactions and the KMnO4 with lower density due to weaker ionic interactions. Such observation inferred that a metallic anion weakened the ionic interactions and the non-metallic anion strengthened the same. Similarly, the μ ri 0 as KMnO4 > KH2PO4 > KOH > K2HPO4 > KCl > K2Cr2O7, with highest values with KMnO4 and lowest with K2Cr2O7 (Table 2) inferred that the MnO 4 - a metallic anion with weaker internal pressure and also the Cr 2 O 7 - with two metallic anion with variable valence inferred weaker shear stress and strain due to moderately weaker ionic interaction. The V S 0 values of the K2Cr2O7, K2HPO4, KH2PO4, KCl and KOH are rationalized w.r.t. those of the KMnO4 with the 1.000067, 1.000169, 1.000175, 1.000040, and 1.000162 times higher than of the KMnO4, respectively. Similarly, the μ ri 0 of the K2HPO4, KMnO4, KH2PO4, KCl, and KOH are rationalized w.r.t. the K2Cr2O7 and noted 1.000068, 1.000135, 1.000105, 1.000038 and 1.000075 times higher than of the K2Cr2O7, respectively (Table 3). In comparison to the K2HPO4 and KH2PO4, there is no specific effect of 1 and 2 K+ on VS and μri while the PO 4 3 - anions are the same because both VS and μri for the KH2PO4 are higher than of the K2HPO4. However, in comparison to K2Cr2O7 and KMnO4 the VS are higher with K2Cr2O7 and μri with KMnO4 due to an effect of anionic metals on VS and μri. The two anionic metallic atoms such as Cr in the K2Cr2O7 has increased VS more than single anionic metallic atom such as Mn in the KMnO4 that decreased the μri. The Mn and Cr are in +7 and +6 oxidation states in KMnO4 and K2Cr2O7, respectively, so another information is also important that the metal having high oxidation number decreased VS and increased μri while the metal having low oxidation number increased VS and decreased μri. In comparison of K2Cr2O7 and KCl, the effect of ionic size and symmetrical arrangement of the ISI existed. The metallic anion such as K2Cr2O7 increased VS more than of the KCl where the K+ and Cl have the same sizes due to the same electronic configuration such as 1s2, 2s2, 2p6, 3s2, 3p6. These variations could be due to the same sizes of the ions which might have created symmetrical arrangement of the ISI while the different size of the ions such as the K+ and Cr 2 O 7 2 - with metallic anionic property developed unsymmetrical ISI which increased the compressibility. This effect is opposite for the μri such as the KCl increased μri higher than of K2Cr2O7.

Table 2 Linear regression data for sound velocity V S 0  ± 10−2 s−1, S V S  ± 10−2 ms−1 kg mol−1, refractive index μ ri 0  ± 10−4, S μ ri  ± 10−4 kg mol−1, adiabatic compressibility β0 ± 104 pa−1, Sβ ± 104 pa−1 kg mol−1, and apparent molal compressibility ϕk0 ± m2N−1, Sϕk ± m2N−1 kg mol−1.
V S 0 S V S μ ri 0 S μ ri −ϕk0 × 105 Sϕk × 10−4 β0 × 107 Sβ × 107
K2Cr2O7 1482.49 65.75 1.33283 0.0520 7.5946 11.905 4.5579 −1.2919
K2HPO4 1482.64 162.98 1.33292 0.0267 14.969 4.1485 4.5565 −1.6400
KMnO4 1482.39 30.81 1.33301 0.0296 2.3897 41.851 4.5618 −0.7901
KH2PO4 1482.65 96.66 1.33297 0.0162 8.6231 −3.1125 4.5567 −1.0159
KCl 1482.45 61.58 1.33288 0.0105 3.4301 14.801 4.5590 −0.6064
KOH 1482.63 72.22 1.33293 0.0090 5.6653 4.0465 4.5575 −0.6680
Table 3 Rationalized V S 0 and μ ri 0 .
K2Cr2O7 K2HPO4 KMnO4 KH2PO4 KCl KOH
V S 0 ratio 1.000067 1.000169 1.000000 1.000175 1.000040 1.000162
μ ri 0 ratio 1.000000 1.000068 1.000135 1.000105 1.000038 1.000075

4.2

4.2 Adiabatic (β) and apparent molal compressibilities (ϕk)

The negative values of the ϕk, Δβ, and Δβ/β0 (Sumathi and Varalakshmi, 2010; Anwar, 1998; Anwar and Anil Kumar, 2002) given in Table 1 which is due to ISI, where the Δβ and Δβ/β0 values increased with increase in salts concentration. It may be attributed to an overall increase in the cohesive forces in the solution (Sumathi and Varalakshmi, 2010; Pandey and Akhatar, 1996). These cohesive forces may result into interaction between water–water, salt–water and salt–water adjacent molecules, where the β values decreased with increase in concentration (Table 1). The β0 are as KMnO4 > KCl > K2Cr2O7 > KOH > KH2PO4 > K2HPO4 (Table 2) shows that KMnO4 has the highest and K2HPO4 has the lowest β0 value with 0.0053 pa−1 difference in their values due to creating high adiabatic compress medium (ACM). A decrease in β0 is due to an increase in ion-dipolicstriction where the salts caused a compression with the decrease in the compressibility (Riyazudden and Khan, 2009). A comparison of KH2PO4 and K2HPO4 salts inferred that a replacement of an H+ from K2HPO4 caused a weaker ISI with contribution of K+ for creating ACM. Thus the cations matter a lot toward an ACM effect on the water structure. Thus KH2PO4 with only single K+ created a stronger ACM while K2HPO4 with 2K+ caused a weaker ACM. Thus the K2HPO4 interaction is two times weaker effective for ACM than of the KH2PO4. The difference of their β0 values are very low with 0.0002 pa−1 which has obtained from (KH2PO4–K2HPO4) that inferred the more cation numbers had partially caused ACM effect. Similarly the KMnO4 has created stronger ACM than of the K2Cr2O7 due to the number of cation and number of transitional metal in their anions. It inferred that the low number of a metal such as Mn (+7) in MnO4- caused stronger ACM than of the high number of a metal such as Cr (+6). Thus extensively and explicitly constituted a concept of molionic mixtures where nature of salts had caused structural impacts on the water structure with variable resultants values of VS, β and ϕk. The ratio of their β0 values is 1.0008 pa−1 derived from (KMnO4/K2Cr2O7) had inferred the partially affected ACM by less number of anionic metals. A linear fitting of the ϕk0 with the composition are found as K2HPO4 > KH2PO4 > K2Cr2O7 > KOH > KCl > KMnO4 (Table 2) due to a reverse relation of ϕk0 with β0 except KOH and K2Cr2O7. It inferred that those factors which are accountable for strong β0 or ACM such as numbers of cation or anionic metals are weaker for ϕk. The similar trend of VS and ϕk with opposite trends of the β0 showed a special relationship among VS, β, and ϕk as VS = ϕk/β as such as relation among the density = mass/volume.

5

5 Conclusion

The study distinguished concentration effect on VS and μri with ISI and even when the MnO 4 - , Cr 2 O 7 - anions with transitional metals were present with potassium in salts. The VS and μri are increased and VL is decreased for aqueous potassium salts solution. The opposite relation of VS and VL is found with increasing internal pressure generated with ISI. The study concluded that the salts contribution with metallic anions (Cr+6 and Mn+7) as ISI did decrease sound velocity in a certain proportion then it increased the light velocity with a similar proportion for the same solution. It is exactly fitted in natural trends of first law of thermodynamics as energy conservation because the light and sound velocities are forms of energy.

Acknowledgment

The authors are highly thankful to Central university of Gujarat, Gandhinagar, for providing financial, infrastructural support and experimental facilities.

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