Volumetric, Acoustic and Viscometric Studies on the Behaviour of Homoeopathic Formulations of Ammonium Causticum at Different Temperatures

OMCIJ.MS.ID.555835

Experimental

Ethanol control and homoeopathic formulations of various potencies of ammonium causticum used in the study were procured from Dr. Wilmer Schwabe India Pvt. Limited, India, which were prepared in accordance with Homoeopathic Pharmacopoeia of India [27]. The densities and ultrasonic speeds of the samples were measured by using high precision digital vibrating tube Density and Sound Analyzer (DSA 5000M, Anton Paar, Austria). The principle used in density measurement is based upon oscillating U-tube principle while the speed of sound is measured using a propagation time technique. This instrument is equipped with both density and ultrasonic cells, with reproducibility of ±1 × 10-3 kg·m-3 and ±1 × 10-2 m·s-1 for density and ultrasonic speed, respectively. The temperature for both cells was kept constant by using built in peltier thermostat within ±0.01 K. The equipment was calibrated with triply distilled degassed water and with dry air at atmospheric pressure [9,10]. The operating working frequency used for ultrasonic speed measurements is 3 MHz. The standard uncertainties related to the measurements of density, ultrasonic speed and temperature were found within ±0.05 kg·m-3, ±0.5 m·s-1 and ±0.01 K, respectively.

The viscosity measurements were done by using microviscometer (Lovis 2000M, Anton Paar, Austria) at temperatures, (293.15 -318.15) K, and atmospheric pressure p = 101 kPa. The temperature was controlled to ±0.02 K by an automatic build in Peltier technique. The rolling ball principle was used in the measurement of viscosity, having a calibrated glass capillary with a steel ball as supplied by manufacturer. The calibration of capillary was accomplished by using viscosity standard fluids. The standard uncertainties for viscosity measurements and temperature were estimated to be within ±0.5% and ±0.02 K.

  • Research Article
  • Keywords
  • Introduction
  • i>
  • Experimental
  • Results
  • Discussion
  • Conclusion
  • Acknowledgement
  • References
  • Results

    The values of densities, ρ, ultrasonic speeds, u, and viscosities, η of homoeopathic formulations of ammonium causticum as function of potency (in centesimal) at different temperatures are listed in Tables 1-3 and are presented graphically in Figures 1-3 respectively. The values of the isentropic compressibility, κs , intermolecular free length, Lf , acoustic impedance, Z have been calculated by using the following relations

    where K’ is temperature dependent constant [= (93.875 + 0.375T) × 10−8]; T is the absolute temperature, The values of, κs , Lf and Z are given in Tables 4-6.

    The deviations in, s κ , Lf , Z and η due to addition of ammonium causticum with dilution and succussion are represented by deviations of these properties from ethanol control properties. The deviations in isentropic compressibility, Δκs , deviations in intermolecular free length, ΔLf , deviations in acoustic impedance, ΔZ and deviations in viscosity, Δη have been calculated by using the following standard relations

    where the superscript ‘o’ represents the values for pure ethanol control (91% ethanol in water). The variations of, Δκs , ΔLf , ΔZ ,and Δη with potency, C of ammonium causticum and temperature are presented graphically in Figure 4-7, respectively.

  • Research Article
  • Keywords
  • Introduction
  • i>
  • Experimental
  • Results
  • Discussion
  • Conclusion
  • Acknowledgement
  • References
  • Discussion

    A close examination of Tables 1-3 and Figure 1-3 indicates that the values of ρ and u and η of ammonium causticum in ethanol are greater than those of ethanol control for all the potencies (1C to 200C) at each investigated temperature and these values decrease with increase in temperature. The values of ρ and u are maximum at 1C and then decrease significantly in presence of ammonium causticum for simple successive dilution to the potency 2C and after that these values increase to maxima at 4C. Thereafter, these values decrease till 6C, then these values remain nearly constant up to 30C, and again increase till 40C and thereafter, these values decrease regularly up to 200C (Figure 1 and 2) with successive dilutions. The values of values of η are maximum at 1C and then decrease significantly in presence of ammonium causticum for simple successive dilution to the potency 2C and after that these values increase to maxima at 4C. Thereafter, these values decrease till 6C, then these values remain nearly constant up to 26C, and again increase till 30C and thereafter, these values decrease regularly up to 200C with successive dilutions. (Figure 3). The observed anomalous trends in ρ, u and η at certain potencies indicates that these potencies exhibit different solution structure from that of ethanol control.

    A close perusal of Tables 4 and 5 indicate that the values of κs and Lf for all the ammonium causticum potencies are less than those of ethanol controls at each investigated temperature and these values increase with increase in temperature, which indicates significant interaction between ammonium causticum and ethanol molecules. The values of κs and Lf are minimum at 1C and then increase significantly in presence of ammonium causticum for simple successive dilution to the potency 2C and after that these values decrease to minima at 4C. Thereafter, these values increase till 6C, then these values remain nearly constant up to 30C, and again decrease till 40C and thereafter, these values increase slightly regularly up to 200C (Figure 1 and 2) with successive dilutions (Tables 4 and 5). These variations in κs and Lf are expressed in terms of deviations in isentropic compressibility, Δκs and deviations in intermolecular free length, ΔLf and are shown graphically in Figure 4 and 5. Figures 4 and 5 indicate that the values of Δκs and ΔLf are negative for all the ammonium causticum potencies are less than those of ethanol controls at each investigated temperature, indicating that the solutions are more compressible in presence of ammonium causticum than ethanol controls. This may be due to the formation of stronger interactions between ammonium causticum and ethanol-water molecules than the hydrogen bonding interactions present in ethanol control.

    The s Δκ and ΔLf are minimum at 1C and then increase significantly in presence of ammonium causticum for simple successive dilution to the potency 2C and after that these values decrease to minima at 4C. Thereafter, these values increase till 6C, then these values remain nearly constant up to 30C, and again decrease till 40C and thereafter, these values increase slightly regularly up to 200C (Figure 4 and 5) with successive dilutions (Tables 4 and 5). This indicates that the potencies 1C, 4C and 40C are less compressible and 2C, 6C to 30C are more compressible than the other potencies, indicating that the potencies 1C, 4C and 40C exhibit more compact solution structure and the potencies 2C, 6C to 30C exhibit less compact solution structure as compared to other potencies and ethanol control. The minimum in Δκs and ΔLf values at potencies 1C, 4C and 40C indicate that these have most compact solution structure as compared to other potencies, hence, these potencies may show different behaviour in terms of efficacy when used in practice.

    A close perusal of Table 6 indicates that the acoustic impedances, Z of potencies of ammonium causticum are more than those of ethanol control for all the potencies at each investigated temperature and the values decrease with increase in temperature, which indicates significant interaction between ammonium causticum and ethanol/water molecules. The values of Z are maximum at 1C and then decrease significantly in presence of ammonium causticum for simple successive dilution to the potency 2C and after that these values increase to maximum at 4C. Thereafter, these values decrease till 6C, then these values remain nearly constant up to 30C, and again increase till 40C and thereafter, these values decrease regularly up to 200C (Table 6) with successive dilutions. These variations in Z are expressed in terms of deviations in acoustic impedance, ΔZ and are shown in Figure 6. Figure 6 indicates that values are positive, i.e., Z values for potencies of ammonium causticum are more than those of ethanol control. These values are maximum at 1C and then decrease significantly in presence of ammonium causticum for simple successive dilution to the potency 2C and after that these values increase to maximum at 4C. Thereafter, these values decrease till 6C, then these values remain nearly constant up to 30C, and again increase till 40C and thereafter, these values decrease regularly up to 200C (Figure 6). This indicates that the potencies 1C, 4C and 40C possess more compact solution structure and 2C, 6C to 30C possess less compact structure than the other potencies and ethanol control. The variations in values of Z and ΔZ of these potencies may be due to interaction between ammonium causticum and ethanol/water molecules.

    The variations in η are expressed in terms of deviations in viscosity, Δη and are shown in Figure 7. Figure 7 indicates that Δη values are positive, i.e., η values for ammonium causticum are more than those of ethanol control. These Δη values are maximum at 1C and then decrease significantly in presence of ammonium causticum for simple successive dilution to the potency 2C and after that these values increase to maxima at 4C. Thereafter, these values decrease till 6C, then these values remain nearly constant up to 26C, and again increase till 30C and thereafter, these values decrease regularly up to 200C with successive dilutions (Figure 7).

    The variations in values of η and Δη of these potencies may be due interaction between ammonium causticum and ethanol/ water molecules. It is observed that the variations observed in the values of measured properties, ρ and u and η; and calculated parameters, κs,Lf,Δκs , ΔLf , ΔZ and Δη support each other. Similar anomalous trends in these properties have also been reported earlier for different potencies of ammonium aceticum [28] and acidum salicylicum [25].

  • Research Article
  • Keywords
  • Introduction
  • i>
  • Experimental
  • Results
  • Discussion
  • Conclusion
  • Acknowledgement
  • References
  • Conclusion

    The densities, ultrasonic speeds, and viscosities of ethanol control, 33 formulations of ammonium causticum in ethanol control are measured for potencies from 1C to 200C (with an interval of 2C up to 30C and then of 10C up to 200C) at six different temperatures and atmospheric pressure. From these experimental data, various physicochemical parameters, viz., s κ , Lf Z , Δκs , ΔLf, ΔZ and Δη were calculated. The results have been qualitatively discussed in terms of interactions/physicochemical behaviour of these extremely dilute homoeopathic formulations of ammonium causticum in ethanol. This indicates that the potencies 1C, 4C and 40C possess more compact solution structure and 2C, 6C to 30C possess less compact structure as compared to other potencies and ethanol control. Hence, these potencies may have different behaviour in terms of efficacy when used in practice. It can be qualitatively concluded that even in extreme dilutions the molecules of ammonium causticum may be present in these homoeopathic formulations, however it needs to be confirmed from other techniques.

  • Research Article
  • Keywords
  • Introduction
  • i>
  • Experimental
  • Results
  • Discussion
  • Conclusion
  • Acknowledgement
  • References
  • Acknowledgement

    The authors are thankful to Central Council for Research in Homeopathy (CCRH), Ministry of AYUSH, Govt. of India for providing financial assistance to carry out this collaborative study.

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