Search

With the promising potential in non-contact fluid manipulation, the photothermally induced phase change along with the interfacial behaviors have been frequently applied in various microfluidic devices. The property of the working fluid greatly affects the photothermal conversion and thus phase change behaviors. For this reason, the IR laser induced phase change of the NaCl solution in the microchannel was visually studied and compared with distilled water in this work. Experimental results indicated that the NaCl solution exhibited the distinct phase change behaviors. The existence of dissolved ions could weaken the photothermal conversion, leading to lowered temperature rise and evaporation rate as compared to the distilled water. In particular, different from the distilled water, the condensed droplets were formed at the region relatively far away from the evaporating interface due to lower evaporation rate. No coalescence between the condensed droplets and liquid slug was observed. Besides, the effects of the NaCl concentration, laser power and spot position were also investigated. It was found that higher NaCl concentration resulted in lower temperature rise and evaporation rate. With the increase of the input laser power and the decrease of the distance between the laser spot and the interface, the temperature rise and evaporation rate could be improved. The obtained results can be further applied in the design and operation of the microfluidic devices based on the photothermally induced phase change. [ABSTRACT FROM AUTHOR]

The study on cells in vitro usually encounters the signals with oscillatory or periodic temporal profiles, which requires the pulsating flow control. Aiming at this target, a novel approach to generate the pulsating waveform of fluid flow by the photothermally induced phase change in the microchannel with the sawtooth-shaped baffles was developed in this work. It was demonstrated that the periodical immobilization-motion-immobilization flow behavior was formed by the combined photothermally induced interfacial behaviors and the in-channel baffle structures, which successfully generated stable oscillating flow with good response. To further explore the pulsating flow behaviors, effects of the baffle design and input laser power were also investigated. It was shown that increasing the baffle width and interval distance between them could yield large pulse peak flow rate but low frequency, while both the pulse peak flow rate and frequency increased with the input laser power. These results indicate that via the change of the baffle design parameters and laser power, the pulse flow waveform can be well controlled for the in vitro cellular studies. [ABSTRACT FROM AUTHOR]

In this work, the condensation behaviors of distilled water actuated by photothermal effect of the infrared laser with the wavelength of 1550 nm in a microchannel were investigated through the visualization method and image processing technique. The impacts of the laser power and the laser spot position on the interface movement and slug formation were also explored. It is found that the interface tended to be advanced as a result of the photothermally induced evaporation–condensation–coalescence process at lower laser powers while the interface was firstly advanced at the beginning and then moved backward after the liquid slug formation in front of the interface at high laser powers. Experimental results also showed that higher laser power and smaller distance between the initial gas–liquid interface and fixed laser spot yielded faster advancing of the gas–liquid interface. For cases with the liquid slug formation, the growth rate of the liquid slug increased with increasing the laser power and decreasing the distance of the laser spot position away from the initial interface position as a result of a high evaporation rate. [ABSTRACT FROM AUTHOR]

In this work, the characteristics of the meniscus evaporation from a microchannel were studied, which was induced by the photothermal effect of the infrared laser with the wavelength of 1550 nm. The evaporation rate and mass transfer coefficient at the interface were determined by the proposed image process technique coupled with an infrared camera. Experimental results showed that once the infrared laser was applied, the interface temperature was rapidly increased but with non-uniform distribution as a result of such a tiny local heating source. Accompanying with the rapid temperature rise, the meniscus evaporation was also immediately actuated. After a certain laser heating period, the interface temperature was increased to a stable value with relatively uniform distribution. In the meantime, the evaporation rate increased and became steady. Besides, the effects of the laser power and laser spot position on the evaporation rate and mass transfer coefficient at the interface were also explored. It was shown that both the interface temperature and evaporation rate linearly increased with the laser power as a result of more heat generated. Smaller distance between the laser spot and front interface yielded higher interface temperature and evaporation rate because of smaller heat transfer resistance resulting from smaller transport length. Reducing the distance could make the increase of the evaporation rate to become more significant. With respect to the mass transfer coefficient, it is interesting to find that the mass transfer coefficients under all cases were almost the same, about 0.4 m/s. [ABSTRACT FROM AUTHOR]

Thecoalescence between liquid flow and droplets is usually encounteredin liquid filling or some new microdevices; a deep understanding ofits underlying mechanism is required. In this work, therefore, thedynamic behaviors of this atypical phenomenon in microchannels werevisually investigated with droplets generated by photothermally inducedevaporation and condensation. The effects of droplet quantity andposition, inlet pressure, and microchannel size were also explored.Experimental results showed that the coalescence accelerated the liquidmovement as a result of lowered pressure at the interface. Parametricstudies indicated that large droplet quantity and small distance betweenthe inlet and droplets yielded a large velocity increment ratio asa consequence of lowered liquid pressure at the interface and increasedpressure gradient, respectively. A high peak velocity increment butwith low velocity increment ratio was obtained at high inlet pressurebecause of high liquid flow velocity. Moreover, the microchannel witha small size yielded a strong acceleration rate of the liquid movementbecause of more obvious capillary action in the small channel. Resultsobtained will be helpful for the design and operation of those kindsof microdevices that may face this atypical phenomenon. [ABSTRACT FROM AUTHOR]