2023
DOI: 10.1103/physreve.108.024802
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Ultrasonic study of water adsorbed in nanoporous glasses

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Cited by 6 publications
(3 citation statements)
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“…Starting from this simple expression, we derive a microscopic model by accounting for the impact of the n a adsorbed molecules on the speed of sound v ( n a ) and phonon lifetime τ( n a ). For the speed of sound, as a first-order approximation, we assume that the coefficients of the stiffness matrix C and the zeolite volume are independent of n a v ( n normala ) = C / ρ v ( 0 ) / 1 + n a m / m β where v 0 is the speed of sound of empty zeolite, m is the mass of the methane molecule, and m β is the mass of empty zeolite (for more details on the speed of sound in nanoconfined fluids, the reader can refer to the experimental and simulation results of coupled adsorption-ultrasonic measurements , ). For the phonon lifetime, as illustrated in Figure a, we write a simple Matthiessen’s rule in which we consider two relaxation processes that are uncoupled and, hence, independent of each other: (1) phonon–phonon scattering within the solid network and (2) phonon scattering at the interface due to the collision with a fluid molecule.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Starting from this simple expression, we derive a microscopic model by accounting for the impact of the n a adsorbed molecules on the speed of sound v ( n a ) and phonon lifetime τ( n a ). For the speed of sound, as a first-order approximation, we assume that the coefficients of the stiffness matrix C and the zeolite volume are independent of n a v ( n normala ) = C / ρ v ( 0 ) / 1 + n a m / m β where v 0 is the speed of sound of empty zeolite, m is the mass of the methane molecule, and m β is the mass of empty zeolite (for more details on the speed of sound in nanoconfined fluids, the reader can refer to the experimental and simulation results of coupled adsorption-ultrasonic measurements , ). For the phonon lifetime, as illustrated in Figure a, we write a simple Matthiessen’s rule in which we consider two relaxation processes that are uncoupled and, hence, independent of each other: (1) phonon–phonon scattering within the solid network and (2) phonon scattering at the interface due to the collision with a fluid molecule.…”
Section: Resultsmentioning
confidence: 99%
“…where v 0 is the speed of sound of empty zeolite, m is the mass of the methane molecule, and m β is the mass of empty zeolite (for more details on the speed of sound in nanoconfined fluids, the reader can refer to the experimental and simulation results of coupled adsorption-ultrasonic measurements 65,66 ). For the phonon lifetime, as illustrated in Figure 5a, we write a simple Matthiessen's rule in which we consider two relaxation processes that are uncoupled and, hence, independent of each other: (1) phonon−phonon scattering within the solid network and ( 2) phonon scattering at the interface due to the collision with a fluid molecule.…”
Section: ■ Results and Discussionmentioning
confidence: 99%
“…For stimuli-responsive applications, elastic properties of materials are the key. However, elastic properties of nanoporous materials are challenging to quantify even for relatively simple structures . AID can serve as a method to measure the elastic constants of nanoporous samples. , If AID and EID are performed on the same samples, the elastic constants can be derived from AID to help eliminating the number of unknowns in the EID experiments.…”
Section: Moving Forwardmentioning
confidence: 99%