AI Article Synopsis

  • Droplet impingement in micrometer-sized cavities is crucial for microfabrication processes like inkjet deposition in PLED displays, requiring careful attention to fluid behaviors to achieve quality results.
  • The process involves tiny droplets (several picoliters) ejected from nozzles at high speeds, and their behavior is influenced by factors such as fluid properties, droplet states, and surface characteristics.
  • The impingement process unfolds in four phases: rapid outward stretching due to inertia, recoiling driven by surface tension, gravitational pull towards cavity walls, and stabilization upon contact with the walls, with fluid viscosity playing a key role in whether a stable layer forms.

Article Abstract

The droplet impingement into a cavity at micrometer-scale is one of important fluidic issues for microfabrications, e.g. the inkjet deposition process in the PLED display manufacturing. The related micro-fluidic behaviors in the deposition process should be carefully treated to ensure the desired quality of microfabrication. The droplets generally dispensing from an inkjet head, which contains an array of nozzles, have a volume in several picoliters, while each nozzle responds very quickly and jets the droplets into cavities on substrates with micrometer size. The nature of droplet impingement depends on the fluid properties, the initial state of droplet, the impact parameters and the surface characteristics. The commonly chosen non-dimensional numbers to describe this process are the Weber number, the Reynolds number, the Ohnesorge number, and the Bond number. This paper discusses the influences of fluid properties of a Newtonian fluid, such as surface tension and fluid viscosity, on micro-fluidic characteristics for a certain jetting speed in the deposition process via a numerical approach, which indicates the impingement process consists of four different phases. In the first phase, the droplet stretching outwards rapidly, where inertia force is dominated. In the second phase, the recoiling of droplet is observed, where surface tension becomes the most important force. In the third phase, the gravitational force pulls the droplet surface towards cavity walls. The fourth phase begins when the droplet surface touches cavity walls and ends when the droplet obtains a stable shape. If the fluid viscosity is relatively small, the droplet surface touches cavity walls in the second phase. A stable fluid layer would not form if the viscosity is relatively small.

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Source
http://dx.doi.org/10.1016/j.bios.2003.11.031DOI Listing

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