scholarly journals Viscosity and Surface Tension of Benzene at Saturation Conditions from Surface Light Scattering

2021 ◽  
Vol 42 (11) ◽  
Author(s):  
Manuel Kerscher ◽  
Andreas P. Fröba ◽  
Thomas M. Koller

AbstractIn the present study, the liquid viscosity and surface tension of benzene was determined at saturation conditions from surface light scattering (SLS) experiments between (283 and 393) K. Based on the application of the hydrodynamic theory for surface fluctuations at the vapor–liquid phase boundary which was successfully validated by the measurements, a simultaneous determination of liquid viscosity and surface tension with average relative expanded uncertainties (k = 2) of (1.0 and 0.8)% was achieved. Agreement between the measurement data and reference values available in the literature was found for the viscosity and in general also for the surface tension, where benzene constitutes a recommended reference material of relatively moderate surface tension values. All these findings demonstrate for a repeated time that SLS is a suitable method for the investigation of fluids including reference fluids such as benzene, which enables a sound representation of its surface tension, presumably as a result of a rather random molecular orientation at the surface. Overall, the experimental results from this work could contribute to an improved data situation for benzene, in particular with respect to providing viscosities and surface tensions at true saturation conditions.

2017 ◽  
Vol 62 (10) ◽  
pp. 3319-3333 ◽  
Author(s):  
Thomas M. Koller ◽  
Tobias Klein ◽  
Cédric Giraudet ◽  
Jiaqi Chen ◽  
Ahmad Kalantar ◽  
...  

2019 ◽  
Vol 64 (9) ◽  
pp. 4116-4131 ◽  
Author(s):  
Tobias Klein ◽  
Shaomin Yan ◽  
Junwei Cui ◽  
Joseph W. Magee ◽  
Kenneth Kroenlein ◽  
...  

Single, highly charged droplets of dioctylphthalate and sulphuric acid of radius between 1 and 10 μm are suspended in vacuum in a quadrupol trap. As the droplets evaporate their radius is monitored continuously by light scattering and their charge is determined periodically by weight balancing. The droplets break when the electric stress exceeds that of surface tension. The largest fragment remains trapped allowing a determination of the change in volume and charge. The fraction of volume and charge lost is found to be independent of particle size and sign of charge and is variable. The oil drops lose (15.0 ± 3.9)% of their charge on breakup and (2.25 ± 0.96)% of their mass. The acid droplets lose (49.4 ± 8.3)% of their charge and less than 0.1% of their mass. The acid results are compared with those from a model of field emission based upon prolate spheroid deformation and the formation of Taylor cones. For both oil and acid droplets the stability limits are in agreement with those predicted by Lord Rayleigh.


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