Abstract

Supercritical fluids play a significant role in elucidating fundamental aspects of liquid matter under extreme conditions. They have been extensively studied at pressures and temperatures relevant to various industrial applications. However, much less is known about the structural behaviour of supercritical fluids and no structural crossovers have been observed in static compression experiments in any temperature and pressure ranges beyond the critical point. The structure of supercritical state is currently perceived to be uniform everywhere on the pressure-temperature phase diagram, and to change only in a monotonic way even moving around the critical point, not only along isotherms or isobars. Conversely, we observe structural crossovers for the first time in a deeply supercritical sample through diffraction measurements in a diamond anvil cell and discover a new thermodynamic boundary on the pressure-temperature diagram. We explain the existence of these crossovers in the framework of the phonon theory of liquids using molecular dynamics simulations. The obtained results are of prime importance since they imply a global reconsideration of the mere essence of the supercritical phase. Furthermore, this discovery may pave the way to new unexpected applications and to the exploration of exotic behaviour of confined fluids relevant to geo- and planetary sciences.

Highlights

  • Changes in phonon states[18,19], providing new unexpected connections between elementary collective excitations and the structure[15,16], thermodynamics and scaling laws of supercritical state[17]

  • We report results from a diffraction experiment on supercritical argon in a diamond anvil cell (DAC) which enables the observation of structural transformations upon crossing the Frenkel line

  • These transitions correspond to a new thermodynamic boundary on argon pressure-temperature diagram

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Summary

Results

We introduce the Hamiltonian H = H0 + Hint, where H0 defines a free theory with no interactions between phonons. Q is a multi-index {q1, q2, q3}, ωD is the Debye frequency, and the parameter μ takes values 1 or 0. The parameters g, λ ∈ + are real non-negative couplings, as introduced in the theory of aggregation ( ) states[18]

Qαq and
For a chosen vacuum
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