VIDEO GALLERY
|
|
watch movie |
Passive optical separation and enrichment of cells by size difference. Video of yeast cells passing through the intersection. Small and large yeast cells were initially flowing in the bottom channel. When they encounter the line laser, the large yeast cell are stopped and pushed to the upper channel while the small yeast cell passed straight through. As a result, the large cells and small cells were successfully separated. from Passive optical separation and enrichment of cells by size difference, Siew-Kit Hoi, Vuong Hoang Kim, Nguyen Manh Huy, Chorng-Haur Sow, Yueh-Sheng Ow, and Andrew A. Bettiol, Biomicrofluidics 4, 044111 (2010). |
![]() watch movie |
Behavior of a train of droplets in a fluidic network with hydrodynamic traps. This study investigates the dynamics of a train of droplets in a fluidic network with hydrodynamic traps. The movie shows uniform doublet trapping, where the conditions were Rl/Ru = 1.56, Qw/Qo = 0.5, and Qo = 10µl/h. from Behavior of a train of droplets in a fluidic network with hydrodynamic traps, Swastika S. Bithi and Siva A. Vanapalli, Biomicrofluidics 4, 044110 (2010). |
watch movie |
Contraction and extension of Vorticella and its mechanical characterization under flow loading. The flow effect on contraction, extension, and shape of V. convallaria. Zooids were stretched by drag forces, and the lengths of zooids increased. The bell-shaped zooid becomes spherical when it contracted as shown in the videos. The length changes of the zooid during contraction and extension gradually increased to ~20–40 µm for flow rates between 100 and 1100 µl min-1. The zooids completed their contractions within the time frame of 30 or 40 ms. from Contraction and extension of Vorticella and its mechanical characterization under flow loading, Moeto Nagai, Hiroshi Asai, and Hiroyuki Fujita, Biomicrofluidics 4, 034109 (2010). |
watch movie |
Contraction and extension of Vorticella and its mechanical characterization under flow loading. The flow effect on contraction, extension, and shape of V. convallaria. Zooids were stretched by drag forces, and the lengths of zooids increased. The bell-shaped zooid becomes spherical when it contracted as shown in the videos. The length changes of the zooid during contraction and extension gradually increased to ~20–40 µm for flow rates between 100 and 1100 µl min-1. The zooids completed their contractions within the time frame of 30 or 40 ms. from Contraction and extension of Vorticella and its mechanical characterization under flow loading, Moeto Nagai, Hiroshi Asai, and Hiroyuki Fujita, Biomicrofluidics 4, 034109 (2010). |
watch movie |
A method for reducing pressure-induced deformation in silicone microfluidics. Fabrication and Laboratory Methods video showing fabrication of a glass-PDMS-glass device from a 3 inch silicon wafer master. from A method for reducing pressure-induced deformation in silicone microfluidics, David W. Inglis, Biomicrofluidics 4, 026504 (2010). |
watch movie |
Electric charge-mediated coalescence of water droplets for biochemical microreactorsle. Two charged droplets of phenolphthalein solution and NaOH solution are merged by the attractive electrostatic force. from Electric charge-mediated coalescence of water droplets for biochemical microreactorsle, Yong-Mi Jung (정용미) and In Seok Kang (강인석), Biomicrofluidics 4, 024104 (2010). |
watch movie |
Dielectrophoretic cell trapping and parallel one-to-one fusion based on field constriction created by a micro-orifice array. The time lapse observation of the collected fusants was made by loading the PDMS chip to a microscope equipped with on-stage incubator. Synchronized cell division observed on chips with smaller micro-orifice (diameter ~ 2µm). Here we see actual time lapse images of the synchronized cell division. from Dielectrophoretic cell trapping and parallel one-to-one fusion based on field constriction created by a micro-orifice array, Murat Gel, Yuji Kimura, Osamu Kurosawa, Hidehiro Oana, Hidetoshi Kotera, and Masao Washizu , Biomicrofluidics 4, 022808 (2010). |
watch movie |
Dielectrophoretic cell trapping and parallel one-to-one fusion based on field constriction created by a micro-orifice array. The time lapse observation of the collected fusants was made by loading the PDMS chip to a microscope equipped with on-stage incubator. Here, five cell pairs are shown fused on the chip at the beginning of the incubation period, the collected fusants at the beginning of the time lapse imaging, and the actual images during cell division. from Dielectrophoretic cell trapping and parallel one-to-one fusion based on field constriction created by a micro-orifice array, Murat Gel, Yuji Kimura, Osamu Kurosawa, Hidehiro Oana, Hidetoshi Kotera, and Masao Washizu , Biomicrofluidics 4, 022808 (2010). |
watch movie |
Fabrication of microfluidic devices using polydimethylsiloxane.
An article from the journal's newest section: "Fabrication and Laboratory Methods." The embedded multimedia and associated text go step by step through a specific method or procedure.[http://dx.doi.org/10.1063/1.3259624.1] A detailed protocol is provided here for using PDMS in the fabrication of microfluidic devices to aid those interested in using the material in their work, with information on the many potential ways the material may be used for novel devices. from Fabrication of microfluidic devices using polydimethylsiloxane, James Frienda and Leslie Yeo , Biomicrofluidics 4, 026502 (2010). |
watch movie |
Using laser Doppler vibrometry to measure capillary surface waves on fluid-fluid interfaces. An article from the journal's newest section: "Fabrication and Laboratory Methods." The embedded multimedia and associated text go step by step through a specific method or procedure. In this article, the authors show how to use Doppler vibrometry to measure capillary surface waves on a fluid-fluid interface. [http://dx.doi.org/10.1063/1.3353329.1] (a) 30 MHz SAW device with straight electrodes generates acoustic waves (b) propagating across the substrate with a magnitude contour plot, equivalent to generating vibration velocities of several millimeters per second as shown from an oblique view of a measurement performed on a 20 MHz device, (c) without a droplet, (d) with a 5 µl de-ionized water droplet, and (e) a much closer view of a 0.5 µl droplet.
from Using laser Doppler vibrometry to measure capillary surface waves on fluid-fluid interfaces, James Frienda and Leslie Yeo, Biomicrofluidics 4, 026501 (2010). |
watch movie |
Onset of channeling during DNA electrophoresis in a sparse ordered post array. Even at a shorter distance of 10 mm, the videomicroscopy data presented definitively identify the peaks in the electropherogram. The first wave of DNA to enter the viewing window clearly consists of a large number of small, freely moving DNA, corresponding to pUC19. In contrast, the latter images feature a lower number of bright molecules, corresponding to λ-DNA. These large DNAs also occasionally undergo rope-over-pulley collisions at 20 V/cm. [http://dx.doi.org/10.1063/]. from Onset of channeling during DNA electrophoresis in a sparse ordered post array, Jia Ou, Samuel J. Carpenter, and Kevin D. Dorfman, Biomicrofluidics 4, 013203 (2010). |
watch movie |
The normal mobility behavior of the worms without treatment of neurotoxin MPP+. This movie showed the mobility behavior of the individual worms in the absence of MPP+. The untreated worms exhibited free movements with more often sine wave-shape and C-shape movement state within the microchannels. from A programmable microvalve-based microfluidic array for characterization of neurotoxin-induced responses of individual C. elegans, Hui Ma, Lei Jiang, Weiwei Shi, Jianhua Qin, and Bingcheng Lin, Biomicrofluidics 3, 044114 (2009). |
| watch movie |
The slight mobility defects of the worms treated with neurotoxin at lower concentration. The worms exhibited slow stroke frequency without obvious change of their movement state within the microchannels after treated with 0.5mM MPP+. from A programmable microvalve-based microfluidic array for characterization of neurotoxin-induced responses of individual C. elegans, Hui Ma, Lei Jiang, Weiwei Shi, Jianhua Qin, and Bingcheng Lin, Biomicrofluidics 3, 044114 (2009). |
watch movie |
The obvious mobility defects of the worms treated with neurotoxin at higher concentration. The worms exhibited the slow stroke frequency with obvious coiled or titanic state within the microchannels after treated with 1.0mM MPP+. from A programmable microvalve-based microfluidic array for characterization of neurotoxin-induced responses of individual C. elegans, Hui Ma, Lei Jiang, Weiwei Shi, Jianhua Qin, and Bingcheng Lin, Biomicrofluidics 3, 044114 (2009). |
| watch movie |
The movies from this article show the patterns of bubbles in a liquid stream generated by a microfluidic device made of two concentric tapered capillary micropipettes. The inner channel is pumped with air and the outer channel is pumped with 1% alginate solution containing 1% Pluronic F127 surfactant. The first movie shows the pattern changes by reducing the outer liquid flow rate at a constant air pressure. The notation shows pressure (psi)/flow rate (µl/min). (a) shows bubbles travel through a liquid jet with a diameter the same as the outer orifice. The liquid jet becomes thinner liquid thread connecting between bubbles after a certain distance. (b) shows that the liquid thread between bubbles become thinner and shorter. (c) shows bidisperse bubbles are encapsulated in monodisperse liquid droplets. (d) shows liquid droplets alternating between one bubble encapsulated or no bubbles (burst). (e) shows liquid droplets containing no bubbles. from Fabricating scaffolds by microfluidics, Kuo-yuan Chung, Narayan Chandra Mishra, Chen-chi Wang, Feng-hui Lin, and Keng-hui Lin, Biomicrofluidics 3, 022403 (2009). |
| watch movie |
The movies from this article show the patterns of bubbles in a liquid stream generated by a microfluidic device made of two concentric tapered capillary micropipettes. The inner channel is pumped with air and the outer channel is pumped with 1% alginate solution containing 1% Pluronic F127 surfactant. This movie shows more interesting patterns at various gas pressure and liquid flow rate. (a) shows a long train of bubbles in a liquid stream with diameter similar to the diameter of bubbles. (b) shows a shorter train of bubbles in a liquid stream. (c) shows monodisperse bubbles encapsulated in monodisperse liquid droplets. (d) shows bidisperse bubbles encapsulated in monodisperse liquid droplets. (e) shows unstable bubbles encapsulated in liquid droplets. from Fabricating scaffolds by microfluidics, Kuo-yuan Chung, Narayan Chandra Mishra, Chen-chi Wang, Feng-hui Lin, and Keng-hui Lin, Biomicrofluidics 3, 022403 (2009). |
![]() watch animation |
A water droplet immersed in an immiscible fluid under dc electric field can be charged by direct contact to the electrode. The droplet charged from the bottom electrode hops along the arc line of the electric field. It is recharged at the opposite bottom electrode immediately after arriving there. The droplet can be translated according to the intended direction if the signal is moved in the wanted direction at the moment when the drop is in contact with the opposite electrode. The droplet transport is relatively fast: the average velocity is about 10 mm·s−1. Furthermore, it causes less contamination of the chip substrate because a droplet is transported by hopping along the arc of the electric field. Accordingly, surface treatment of the chip substrate is much simpler.
Experimental condition: E = 1.5 kV/cm, V = 2 ml, n = 10 cSt from A novel actuation method of transporting droplets by using electrical charging of droplet in a dielectric fluid, Yong-Mi Jung (정용미) and In Seok Kang (강인석) , Biomicrofluidics 3, 022402 (2009). |
![]() watch movie |
Simulation of the coalescence of two sessile droplets: This video shows the equi-height contours of the droplets as they spread and coalesce on a partially wetting substrate. It illustrates the evolution of the footprint of the droplet system. Following the rapid growth of the neck bridging the two droplets, the resulting droplet slowly relaxes to a spherical cap configuration.
from Modeling the coalescence of sessile droplets, M. Sellier and E. Trelluyer, Biomicrofluidics 3, 022412 (2009). |
![]() watch movie |
Nanocolloids that assemble and disassemble within the nanochannel (width 100 µm and depth 200 nm) into a colloidal closed-packed structure.
from Understanding electrokinetics at the nanoscale: A perspective, Hsueh-Chia Chang and Gilad Yossifon, Biomicrofluidics 3, 012001 (2009). |
![]() watch movie |
Communication between neighboring nanochannels due to overlapping polarized layers at the entrance. The current for a seven-channel array is compared to seven times that for a single-channel array to determine the degree of communication. The single nanochannel dimensions are width w=0.1 mm, height h=200 nm, and length d=0.5 mm. The video shows an array of separate depletion regions emerging from the nanochannel array, just before their merging.
from Understanding electrokinetics at the nanoscale: A perspective, Hsueh-Chia Chang and Gilad Yossifon, Biomicrofluidics 3, 012001 (2009). |
![]() watch movie |
Rectification of a nanoslit with asymmetric entrances: the depletion-enrichment phenomenon when the anode is at the right reservoir. The left entrance is wider (w=2.3 mm) than the right (w =0.1 mm), as seen in the microscopic image (inset of b in the online article), and is obtained by intentional misalignment of the two Pyrex slides. The nanochannel height is h=200 nm and length is d=0.5 mm. The video shows the depletion-enrichment phenomenon when the anode is at the right reservoir. from Understanding electrokinetics at the nanoscale: A perspective, Hsueh-Chia Chang and Gilad Yossifon, Biomicrofluidics 3, 012001 (2009). |
![]() watch movie |
Rubinstein's vortex instability in front of a nanoslit develops beyond a critical voltage to select a thin diffusion layer much shorter than the distance to the electrode. The confocal images are taken at 40 V showing vortices at the depletion layer on the anodic side (left reservoir) for an ionic strength of ~0.1 mM. The diffusion layer is allowed to grow to a certain thickness with a low-frequency ac field and the vortices only appear when the frequency is below 0.1 Hz and when the voltage is beyond ~20 V.
from Understanding electrokinetics at the nanoscale: A perspective, Hsueh-Chia Chang and Gilad Yossifon, Biomicrofluidics 3, 012001 (2009). |
![]() watch movie |
Microflow induced by a pair of orthogonal electrodes at 140 µm separation Fluid conductivity is 20 mS/m. Microflow patterns are delineated by 0.5 µm fluorescent tracer particles. With an ac signal of 500 kHz at 15 VPP, the fluid moves along the pin electrode towards the gap. This microflow pattern is driven by ac electrothermal (ACET) effect. from Investigation of microflow reversal by ac electrokinetics in orthogonal electrodes for micropump design, Kai Yang and Jie Wu, Biomicrofluidics 2, 024101 (2008). |
![]() watch movie |
Microflow induced by an pair of orthogonal electrodes at 140 µm separation Fluid conductivity is 20 mS/m. Microflow patterns are delineated by 0.5 µm fluorescent tracer particles. With an ac signal of 200 Hz at 20 VPP, the fluid shoots from the pin electrode towards the gap. This is caused by Faradaic polarization at the pin electrode. At relatively high voltage, Faradaic polarization takes place and induces co-ions instead of counter-ions from capacitive polarization at lower voltages. Because the mobile ions are of opposite polarity, the flow direction is opposite to those at lower voltages. from Investigation of microflow reversal by ac electrokinetics in orthogonal electrodes for micropump design, Kai Yang and Jie Wu, Biomicrofluidics 2, 024101 (2008). |
![]() watch movie |
Microflow induced by a pair of orthogonal electrodes at 140 µm separation Fluid conductivity is 20 mS/m. Microflow patterns are delineated by 0.5 µm fluorescent tracer particles. Â With an ac signal of 1 kHz at 10 Vpp, fluid moves from the electrode gap up along the pin electrode and forms two vortices in the fluid bulk besides the pin electrode. This flow phenomenon is driven by ac electroosmosis (ACEO) effect, where counter-ions are attracted to the electrode surface and move under the influence of electric field to induce microflows. from Investigation of microflow reversal by ac electrokinetics in orthogonal electrodes for micropump design, Kai Yang and Jie Wu, Biomicrofluidics 2, 024101 (2008). |
![]() watch movie |
Simulation of the generation of an asymmetric chemical gradient field Chemical was fed from an effusion hole located at the center of the chamber while stable lateral medium flow was pumped from left to right. The lateral medium flow provide homogeneous flow field and the central effusion generated a stable (yet variably controllable) chemical gradient. The distribution of the chemical gradient can be easily changed by controlling the relative flow rate between the lateral flow and the effusion flow. Experimental confirmation is described in the main text. from A transparent cell-culture microchamber with a variably controlled concentration gradient generator and flow field rectifier, Ji-Yen Cheng, Meng-Hua Yen, Ching-Te Kuo, and Tai-Horng Young, Biomicrofluidics 2, 024105 (2008). |
![]() watch movie |
Time-lapsed photography of dye replacement inside a modified Hele-Shaw microchamber The dimension of the cell is 14 mm x 26 mm x 105 µm. The flow rate was set at 10 µL/h by a syringe pump. Although parabolic flow front is observed, the flow field is homogeneous. The flow speed is measured by the shape of the flow front edge. The flow fronts were then digitized and the migration distance was measured to estimate flow speed. The result indicates that the difference between the speed at the centerline and that at the wall is about 7%, which is significantly smaller than a parabolic flow. Mammalian cancer cells have been stably cultured inside this chamber for more than 2 weeks. from A transparent cell-culture microchamber with a variably controlled concentration gradient generator and flow field rectifier, Ji-Yen Cheng, Meng-Hua Yen, Ching-Te Kuo, and Tai-Horng Young, Biomicrofluidics 2, 024105 (2008). |
![]() watch movie |
Simulation showing the culture medium replacement inside a modified Hele-Shaw microchamber The dimension of the cell is 14 mm x 26 mm x 105 µm. At a flow rate of 10 µL/h, the flow speed inside the chamber is 0.08 µm/s, resulting in insignificant shear stress on cells to be cultured inside the chamber. The observed parabolic front represents the flow front but not the flow speed. Transversally the flow speed is uniform within 90% of the chamber’s cross-section. The simulation shows that entire medium refreshment is achieved in about 10 hours. Slow and uniform flow field is obtained together with efficient medium replacement. from A transparent cell-culture microchamber with a variably controlled concentration gradient generator and flow field rectifier, Ji-Yen Cheng, Meng-Hua Yen, Ching-Te Kuo, and Tai-Horng Young, Biomicrofluidics 2, 024105 (2008). |
![]() watch movie |
A Dielectrophoretic-Meister for the age of red blood cells The video shows migration of blood cells near a quadrupole electrode as the frequency of the AC field at the electrodes increases. The blood cells start from the negative Dielectrophoretic trap at the middle, migrate to the high field region between the electrodes and migrate back to the center. Such migration pattern indicates that there are two cross-over frequencies for the blood cells. The two values can be easily estimated visually and their values are sensitively dependent on the age of the blood cells. We have also enhanced the sensitivity to age by cross-linking the membrane proteins with glutaldehyde. from Dielectrophoretic discrimination of bovine red blood cell starvation age by buffer selection and membrane cross-linking, J.E. Gordon, Z. Gagnon, and H.-C. Chang, Biomicrofluidics 1, 044102 (2007). |
![]() watch movie |
Trapping rate of fluorescent 5 µm latex particles in the crescent electrode The sorted latex particles are trapped at a trapping gate with electrodes on the top and bottom substrates working in the negative DEP region for the sorted particles. With the symmetric electrode design, a DEP trap exists at the tip of the trapping gate to trap the particles at a very high rate of 100 partilces per second. The number of trapped particles can be estimated from the impedance signal across the electrodes. There is no flow resistance with this trap as there is no electrical force on the liquid. from An integrated dielectrophoretic chip for continuous bioparticle filtering, focusing, sorting, trapping, and detecting, I.F. Cheng, H.C. Chang, D. Hou, and H.-C. Chang, Biomicrofluidics 1, 021503 (2007). |
![]() watch movie |
Sorting latex particles and Lactobacillus based on their negative DEP mobilities The sorter unit with 50-micron wide electrodes fabricated onto the top and bottom substrates and operated at a selected frequency to impart a high field between the two gating electrodes. The liquid goes through the gate unimpeded into a downstream channel and so do 1-micron latex particles suffering from positive DEP. Larger 5 micron latex particles cannot go through the gating electrode and slide along the electrode gate into a different channel. Sorting into different bins by size is hence achieved at about 100 particles per second. from An integrated dielectrophoretic chip for continuous bioparticle filtering, focusing, sorting, trapping, and detecting, I.F. Cheng, H.C. Chang, D. Hou, and H.-C. Chang, Biomicrofluidics 1, 021503 (2007). |
![]() watch movie |
Filtering and focusing stages on a dielectrophoretic (DEP) chip with C. albicans and latex The focusing units on the chip at high frequencies corresponding to negative DEP. The first set of periphery electrodes focus the particles to a 50 micron wide area in the middle of the channel and the second one, with a smaller orifice, line them up into a single queue within a 10 micron wide region. Such focusing allows each colloid to experience the same chemical and electrical environment in the chip and hence can be sorted according to their DEP mobility difference. from An integrated dielectrophoretic chip for continuous bioparticle filtering, focusing, sorting, trapping, and detecting, I.F. Cheng, H.C. Chang, D. Hou, and H.-C. Chang, Biomicrofluidics 1, 021503 (2007). |


































This Publication
Scitation
Google Scholar
PubMed