Controlled generation of droplets using an electric field in a flow focusing paper‐based device

2021 ◽  
Author(s):  
Tianyi Jiang ◽  
Yupan Wu
Keyword(s):  
Author(s):  
Say Hwa Tan ◽  
Benoit Semin ◽  
Jean-Christophe Baret

We report a novel electrical control in droplet microfluidics using an ac electric field. The method can be used to actively control and tune the size of water-in-oil droplets formed in a microfluidic flow focusing device. Electrodes fabricated using microsolidics technique are not in contact with the fluids and hence prevent undesirable electrochemical reactions. The proposed electrical control is able to change the size of the droplets in the order of millisecond and also to manipulate the size of the droplets formed at single droplet level through the change in applied voltages and signal. An electro-mediated droplet formation regime transition from dripping to jetting is also observed due to the changes in the Maxwell stress arising from the application of the ac electric field. At applied frequency of between 50 to 5 kHz, the change in droplet sizes follow similar trend for the case of pure DI water but is different for the case of NaCl solution.


2007 ◽  
Vol 91 (13) ◽  
pp. 133106 ◽  
Author(s):  
Haejune Kim ◽  
Dawei Luo ◽  
Darren Link ◽  
David A. Weitz ◽  
Manuel Marquez ◽  
...  

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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