Optical trapping-polarized Raman microspectroscopy of single ethanol (EtOH) microdroplets with a diameter () of 6.1-16.5 μm levitated in an EtOH vapor-saturated air/N gas atmosphere has been explored to elucidate the vibrational and rotational motions of EtOH in the droplets at 22.0 °C. The Raman spectral bandwidth of the C-C stretching vibrational mode observed for an aerosol EtOH microdroplet was narrower than that of bulk EtOH, suggesting that the vibrational/rotational motions of EtOH in the aerosol system were restricted compared to those in the bulk system. In practice, polarized Raman microspectroscopy demonstrated that the rotational relaxation time (τ) of EtOH in an aerosol microdroplet with = 16. 5 μm was slower (2.33 ps) than that in a bulk EtOH (1.65 ps), while the vibrational relaxation times (τ) in the aerosol and bulk EtOH systems were almost comparable with one another: 0.86-0.98 ps. Furthermore, although the τ value of an aerosol EtOH microdroplet was almost unchanged irrespective of as described above, the τ value increased from 2.33 to 3.57 ps with a decrease in from 16.5 to 6.1 μm, which corresponded to the increase in EtOH viscosity (η) from 1.33 to 2.04 cP with the decrease in . The droplet size dependences of τ and η in an aerosol EtOH microdroplet were discussed in terms of the gas/droplet interfacial molecular arrangements of EtOH and Laplace pressure experienced by a spherical EtOH microdroplet in the gas phase.
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http://dx.doi.org/10.1021/acs.analchem.0c05406 | DOI Listing |
Anal Chem
March 2021
Department of Chemistry, Faculty of Science, Hokkaido University, Sapporo 060-0810, Japan.
Optical trapping-polarized Raman microspectroscopy of single ethanol (EtOH) microdroplets with a diameter () of 6.1-16.5 μm levitated in an EtOH vapor-saturated air/N gas atmosphere has been explored to elucidate the vibrational and rotational motions of EtOH in the droplets at 22.
View Article and Find Full Text PDFPhys Rev Lett
June 2012
Division of Physical Sciences and Engineering & Clean Combustion Research Center, King Abdullah University of Science and Technology (KAUST), Thuwal, 23955-6900, Saudi Arabia.
The splashing of a drop impacting onto a liquid pool produces a range of different sized microdroplets. At high impact velocities, the most significant source of these droplets is a thin liquid jet emerging at the start of the impact from the neck that connects the drop to the pool. We use ultrahigh-speed video imaging in combination with high-resolution numerical simulations to show how this ejecta gives way to irregular splashing.
View Article and Find Full Text PDFPhys Rev Lett
January 2011
Division of Physical Sciences and Engineering and Clean Combusion Research Center, King Abdullah University of Science and Technology, Thuwal 23955-6900, Saudi Arabia.
When a drop impacts onto a liquid pool, it ejects a thin horizontal sheet of liquid, which emerges from the neck region connecting the two liquid masses. The leading section of this ejecta bends down to meet the pool liquid. When the sheet touches the pool, at an "elbow," it ruptures and sends off microdroplets by a slingshot mechanism, driven by surface tension.
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