排序方式: 共有28条查询结果,搜索用时 15 毫秒
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Controlled production of monodisperse double emulsions by two-step droplet breakup in microfluidic devices 总被引:13,自引:0,他引:13
Okushima S Nisisako T Torii T Higuchi T 《Langmuir : the ACS journal of surfaces and colloids》2004,20(23):9905-9908
A microfluidic device having both hydrophobic and hydrophilic components is exploited for production of multiple-phase emulsions. For producing water-in-oil-in-water (W/O/W) dispersions, aqueous droplets ruptured at the upstream hydrophobic junction are enclosed within organic droplets formed at the downstream hydrophilic junction. Droplets produced at each junction could have narrow size distributions with coefficients of variation in diameter of less than 3%. Control of the flow conditions produces variations in internal/external droplet sizes and in the internal droplet number. Both W/O/W emulsions (with two types of internal droplets) and oil-in-water-in-oil emulsions were prepared by varying geometry and wettability in microchannels. 相似文献
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Ichirou Yamaguchi Masayuki Yokota Takasi Ida Mizuki Sunaga Koichi Kobayashi 《Optical Review》2007,14(6):362-364
The state of drying paint is monitored from the dynamic behaviors of the speckle pattern arising from laser illumination of
the region inspected. Temporal variation of the peak height of the cross-correlation function between successive frames taken
with a fixed interval is plotted until the peak maintains a stationary maximum value. We used a speckle pattern in the diffraction
field for monitoring of a single region and that in the image field for simultaneous monitoring of various regions. Both the
normal and the phase-only algorithms were compared for cross-correlation computation. The former showed more distinct variation
of peak height. 相似文献
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This paper is concerned with blowup of positive solutions to a Cauchy problem for a parabolic-elliptic system
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We consider radial solutions blowing up in infinite time to a parabolic–elliptic system in N-dimensional Euclidean space. The system was introduced to describe the gravitational interaction of particles. In the case where N≥2, we can find positive and radial solutions blowing up in finite time. In the present paper, in the case where N≥11, we find positive and radial solutions blowing up in infinite time and investigate those blowup speeds, by using the so-called asymptotic matched expansion techniques and parabolic regularity. 相似文献
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This study describes a microfluidic platform with coaxial annular world-to-chip interfaces for high-throughput production of single and compound emulsion droplets, having controlled sizes and internal compositions. The production module consists of two distinct elements: a planar square chip on which many copies of a microfluidic droplet generator (MFDG) are arranged circularly, and a cubic supporting module with coaxial annular channels for supplying fluids evenly to the inlets of the mounted chip, assembled from blocks with cylinders and holes. Three-dimensional flow was simulated to evaluate the distribution of flow velocity in the coaxial multiple annular channels. By coupling a 1.5 cm × 1.5 cm microfluidic chip with parallelized 144 MFDGs and a supporting module with two annular channels, for example, we could produce simple oil-in-water (O/W) emulsion droplets having a mean diameter of 90.7 μm and a coefficient of variation (CV) of 2.2% at a throughput of 180.0 mL h(-1). Furthermore, we successfully demonstrated high-throughput production of Janus droplets, double emulsions and triple emulsions, by coupling 1.5 cm × 1.5 cm - 4.5 cm × 4.5 cm microfluidic chips with parallelized 32-128 MFDGs of various geometries and supporting modules with 3-4 annular channels. 相似文献
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Droplet formation in a microchannel network 总被引:21,自引:0,他引:21
A method is given for generating droplets in a microchannel network. With oil as the continuous phase and water as the dispersed phase, pico/nanoliter-sized water droplets can be generated in a continuous phase flow at a -junction. The channel for the dispersed phase is 100 microm wide and 100 microm deep, whereas the channel for the continuous phase is 500 microm wide and 100 microm deep. For given experimental parameters, regular-sized droplets are reproducibly formed at a uniform speed. The diameter of these droplets is controllable in the range from 100-380 microm as the flow velocity of the continuous phase is varied from 0.01 m s(-1) to 0.15 m s(-1). 相似文献
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Takasi SenbaTakashi Suzuki 《Journal of Functional Analysis》2002,191(1):17-51
We study a parabolic-elliptic system of partial differential equations, which describes the chemotactic feature of slime molds. It is known that the blowup solution forms singularities such as delta functions, referred to as the collapses. Here, we study the case that the domain is a flat torus and show that the post-blowup continuation of the solution is possible only when those collapses are quantized with the mass 8π. 相似文献