Study on freezing phenomenon of supercooled water by electric field applied from outside of thermal storage tube

2018 ◽  
Vol 2018.55 (0) ◽  
pp. D014
Author(s):  
Shota NAKAGAWA ◽  
Masanori FUJIMOTO ◽  
Yoshiro TOCHITANI
Author(s):  
Katherine Carpenter ◽  
Vaibhav Bahadur

The majority of studies on ice formation have attempted to prevent or reduce ice build-up; very few studies have focused on promoting ice nucleation which would have applications in appliances, cryopreservation, and pharmaceutical freeze-drying. Such studies are also relevant to the synthesis of methane hydrates for natural gas transportation. This paper details a fundamental study on the influence of interfacial electric fields on ice nucleation promotion. Electrofreezing, i.e. applying an electric field has been shown to electrically induce nucleation of supercooled water. The freezing temperatures of supercooled water can thus be increased via electrofreezing. However, the mechanisms responsible for elevating the freezing temperature are unclear. Typically, bare electrodes are submerged in water, which creates a volumetric electric field in water. With this type of electric field, the application of a voltage can result in multiple phenomena such as current flows, chemical reactions and gas bubble formation or growth. It is unclear whether electrofreezing is the result of the electric field or the current flow-related secondary phenomena. In the present work, the role of electric fields and surface charge on electrofreezing is isolated by studying electrofreezing of water droplets on a dielectric layer. This dielectric layer blocks current and creates an interfacial electric field with a build-up of electric charge at the solid-fluid interface. Ultra-high electric fields of up to 80 V/μm were applied, which is one order of magnitude higher than in previous studies. Infrared (IR) thermography was used to capture ice nucleation and determine the electrofreezing temperature. The results show that the electric fields alone can elevate the freezing temperature of water by as much as 15 °C; however, this effect saturates at electric fields of approximately 20–40 V/μm. Also, the electrofreezing effect was found to be polarity independent. Therefore, it is hypothesized that the mechanism underlying electrofreezing is a reduction in the Gibbs free energy for ice crystal nucleation. Furthermore, by intentionally creating pinholes in the dielectric layer, which creates current paths, the influence of electric current on electrofreezing was also studied. It was observed that electric currents and/or other secondary effects, such as bubble generation, further increased the electrofreezing temperatures. Overall, this work fills many existing gaps in the current understanding of electrofreezing. It is seen that both the electric field and electric current influence electrofreezing; however, the physical mechanisms are different.


Nature ◽  
1962 ◽  
Vol 196 (4854) ◽  
pp. 568-569 ◽  
Author(s):  
T. W. ZAWIDZKI ◽  
HENRY M. PAPÉE

Author(s):  
G. F. Rempfer

In photoelectron microscopy (PEM), also called photoemission electron microscopy (PEEM), the image is formed by electrons which have been liberated from the specimen by ultraviolet light. The electrons are accelerated by an electric field before being imaged by an electron lens system. The specimen is supported on a planar electrode (or the electrode itself may be the specimen), and the accelerating field is applied between the specimen, which serves as the cathode, and an anode. The accelerating field is essentially uniform except for microfields near the surface of the specimen and a diverging field near the anode aperture. The uniform field forms a virtual image of the specimen (virtual specimen) at unit lateral magnification, approximately twice as far from the anode as is the specimen. The diverging field at the anode aperture in turn forms a virtual image of the virtual specimen at magnification 2/3, at a distance from the anode of 4/3 the specimen distance. This demagnified virtual image is the object for the objective stage of the lens system.


Author(s):  
Patrick P. Camus

The theory of field ion emission is the study of electron tunneling probability enhanced by the application of a high electric field. At subnanometer distances and kilovolt potentials, the probability of tunneling of electrons increases markedly. Field ionization of gas atoms produce atomic resolution images of the surface of the specimen, while field evaporation of surface atoms sections the specimen. Details of emission theory may be found in monographs.Field ionization (FI) is the phenomena whereby an electric field assists in the ionization of gas atoms via tunneling. The tunneling probability is a maximum at a critical distance above the surface,xc, Fig. 1. Energy is required to ionize the gas atom at xc, I, but at a value reduced by the appliedelectric field, xcFe, while energy is recovered by placing the electron in the specimen, φ. The highest ionization probability occurs for those regions on the specimen that have the highest local electric field. Those atoms which protrude from the average surfacehave the smallest radius of curvature, the highest field and therefore produce the highest ionizationprobability and brightest spots on the imaging screen, Fig. 2. This technique is called field ion microscopy (FIM).


1993 ◽  
Vol 3 (8) ◽  
pp. 1201-1225 ◽  
Author(s):  
G. N�ron de Surgy ◽  
J.-P. Chabrerie ◽  
O. Denoux ◽  
J.-E. Wesfreid

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