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Molecular dynamics study of perchloric acid using the extended Madrid-2019 force field

M. Cruz-Sánchez, S. Blazquez, C. Vega, V. M. Trejos

Abstract

Perchloric acid (HClO$_4$) is widely used to prepare perchlorate salts with applications in propellants, industry, environmental chemistry, and biology. In this work, we used the intermolecular parameters from the extended Madrid-2019 force field for the perchlorate anion (ClO$_4^-$) and the oxonium cation (H$_3$O$^+$) together with TIP4P/2005 water to model perchloric acid solutions. The force field uses scaled charges of $\pm0.85e$ for monovalent ions and has been widely applied for aqueous ionic systems. We used the model to predict thermodynamic properties [densities and temperatures of maximum in density (TMD)], structural features (ion-water correlations: ion-hydrogen and ion-oxygen), and transport properties (self-diffusion coefficients and viscosity) of perchloric acid solutions at several concentrations. Experimental densities are predicted in excellent agreement up to 10 $m$. We also performed molecular simulations over a wide range of temperatures in order to determine the TMD of perchloric acid at different molalities. Predicted viscosities at 298.15 K and 1 bar are in good agreement with experimental data for concentrations below 4 $m$. Results are discussed in terms of model strengths and limitations.

Molecular dynamics study of perchloric acid using the extended Madrid-2019 force field

Abstract

Perchloric acid (HClO) is widely used to prepare perchlorate salts with applications in propellants, industry, environmental chemistry, and biology. In this work, we used the intermolecular parameters from the extended Madrid-2019 force field for the perchlorate anion (ClO) and the oxonium cation (HO) together with TIP4P/2005 water to model perchloric acid solutions. The force field uses scaled charges of for monovalent ions and has been widely applied for aqueous ionic systems. We used the model to predict thermodynamic properties [densities and temperatures of maximum in density (TMD)], structural features (ion-water correlations: ion-hydrogen and ion-oxygen), and transport properties (self-diffusion coefficients and viscosity) of perchloric acid solutions at several concentrations. Experimental densities are predicted in excellent agreement up to 10 . We also performed molecular simulations over a wide range of temperatures in order to determine the TMD of perchloric acid at different molalities. Predicted viscosities at 298.15 K and 1 bar are in good agreement with experimental data for concentrations below 4 . Results are discussed in terms of model strengths and limitations.
Paper Structure (13 sections, 6 equations, 5 figures, 3 tables)

This paper contains 13 sections, 6 equations, 5 figures, 3 tables.

Figures (5)

  • Figure 1: (Colour online) Density as a function of molality for aqueous solutions of perchloric acid (HClO$_4$) at three temperatures (namely 298.15, 283.15, and 323.15 K) and 1 bar. Solid symbols represent the MD results, while the continuous line corresponds to the experimental data. Experimental data are taken from reference Brickwedde1949properties. The MD simulations were performed using the Madrid-2019 force field ($q = \pm0.85e$) Blazquez2025perchlorateGamez2025_H3O. For better visualization, the densities of perchloric acid at 298.15 K and 283.15 K are shifted upward by 100 and 200 units, respectively.
  • Figure 2: (Colour online) Panel (a): number-density profiles of ClO$_4^-$ and H$_3$O$^+$ ions as a function of the box length along the three Cartesian coordinates ($x$, $y$, and $z$) for the 8.48 $m$ HClO$_4$ solution. The profiles are nearly flat and overlap in all directions, indicating that the system remains homogeneous, with no evidence of aggregation. Only small statistical fluctuations ($\approx 1\%$) are observed across the simulation box. For clarity, the $y$-axis and $x$-axis values in the number density were shifted upward by one and two number density units, respectively. Panel (b): representative snapshot of the system at the highest molality studied in this work (8.48 $m$), showing the spatial distribution of perchlorate (green and yellow) and hydronium (blue and red) ions.
  • Figure 3: (Colour online) Panel (a): density as a function of temperature for aqueous solutions of perchloric acid (HClO$_4$) at 0.30 $m$, 0.49 $m$, 0.69 $m$, and 0.98 $m$ at 1 bar. Solid squares denote MD simulation results, dashed lines represent third-order polynomial fits to the MD data obtained with the extended Madrid-2019 model Blazquez2025perchlorateGamez2025_H3O, and stars indicate the temperature of maximum density. Panel (b): variation of $\Delta$ as a function of $m$ for perchloric acid solutions. The dashed line corresponds to a linear fit to the MD simulation results (filled symbols).
  • Figure 4: (Colour online) Radial distribution functions for aqueous solutions of perchloric acid (HClO$_4$) at low (0.98 $m$, solid black line) and high (5.42 $m$, dotted red line) concentrations at 298.15 K and 1 bar. Panel (a): RDFs for H$_w$--Cl$_p$ and H$_w$--O$_p$ interactions. Panel (b): RDFs for O$_w$--Cl$_p$ and O$_w$--O$_p$ interactions. Panel (c): RDFs for O$_{\text{H}_3 \text{O}^+}$--Cl$_p$ and H$_{\text{H}_3 \text{O}^+}$--O$_p$, interactions. The vertical dotted lines correspond to the experimental values for the position of the first maximum of the RDFs.
  • Figure 5: (Colour online) Panel (a): self-diffusion coefficients of water and perchloric ion (ClO$_4^{-}$) as a function of molality at 298.15 K and 1 bar. Filled squares represent simulation results, while dashed lines are included as visual guides. The experimental was obtained from reference Malhotra1993. Panel (b): shear viscosity as a function of molality for aqueous solutions of perchloric acid (HClO$_4$) at 298.15 K and 1 bar. Filled squares represent simulation results, while continuous lines correspond to experimental data from reference Brickwedde1949properties.