8 research outputs found
全部國産に依る16ミリ「レ」線映晝 : 第2編
<div><p>Microfluidics is a great enabling technology for biology, biotechnology, chemistry and general life sciences. Despite many promising predictions of its progress, microfluidics has not reached its full potential yet. To unleash this potential, we propose the use of intrinsically active hydrogels, which work as sensors and actuators at the same time, in microfluidic channel networks. These materials transfer a chemical input signal such as a substance concentration into a mechanical output. This way chemical information is processed and analyzed on the spot without the need for an external control unit. Inspired by the development electronics, our approach focuses on the development of single transistor-like components, which have the potential to be used in an integrated circuit technology. Here, we present membrane isolated chemical volume phase transition transistor (MIS-CVPT). The device is characterized in terms of the flow rate from source to drain, depending on the chemical concentration in the control channel, the source-drain pressure drop and the operating temperature.</p></div
Dynamic investigation of the gate switching.
<p>(A), Experimental approach of the investigation. Switch event at t<sub>0</sub> carried out by a change of the input flow in the control channel from c<sub>0</sub> (= 0wt%) to c<sub>1</sub> (= 30wt%), while applying a constant pressure over the chemo-fluidic transistor. The flow rate generated in the flow channel is measured via a flow sensor. (B), Typical measurement of pressure and flow rate data over time, starting from time t<sub>0</sub> (= 0s). (C), Schematic graph with characteristic parameters to quantify the experimental data. (D), Bar graph of the characteristic parameter t<sub>10</sub>, t<sub>90</sub> and Δt for three different dimensions of gel particles.</p
Overview of the fabrication procedure.
<p><b>Master fabrication:</b> (A) Lamination of dry film resist onto substrate. (B) Exposure with UV light through photo mask. (C) Post-exposure bake. (D) Development and rinsing with following hard bake. <b>Chip fabrication</b>: (E) Spin coating of PDMS on control layer master. (F) Moulding of PDMS on flow layer master. <b>Chip assembling</b>: (G) Inhibition of the channel break in the flow layer. (H) Plasma bonding with aligning of the PDMS layers. (I) Incorporation of the hydrogel particle into the control channel. (J) Plasma bonding of the multi-layer chip onto a cover glass.</p
Opening pressure extracted from the measurement data and modeled as a 2nd order 2D polynomial.
<p>Opening pressure extracted from the measurement data and modeled as a 2nd order 2D polynomial.</p
Measured output characteristics (flow rate Q<sub>DS</sub> vs. pressure p<sub>DS</sub>) of the MIS-CVPT with the different ethanol concentrations c<sub><i>Eth</i></sub> 0wt%, 7.5wt%, and 15.0wt% at different temperatures <i>ϑ</i> ranging from 15.0°C to 30.0°C in 5.0K steps.
<p>Measured output characteristics (flow rate Q<sub>DS</sub> vs. pressure p<sub>DS</sub>) of the MIS-CVPT with the different ethanol concentrations c<sub><i>Eth</i></sub> 0wt%, 7.5wt%, and 15.0wt% at different temperatures <i>ϑ</i> ranging from 15.0°C to 30.0°C in 5.0K steps.</p
Transfer characteristic of the MIS-CVPT. Flow rate Q<sub>DS</sub> over ethanol concentration c<sub>Eth</sub> at a constant pressure p<sub>DS</sub> = 100mbar for the temperatures <i>ϑ</i> 22.5°C; 25.0°C; 27.5°C; 30.0°C.
<p>Transfer characteristic of the MIS-CVPT. Flow rate Q<sub>DS</sub> over ethanol concentration c<sub>Eth</sub> at a constant pressure p<sub>DS</sub> = 100mbar for the temperatures <i>ϑ</i> 22.5°C; 25.0°C; 27.5°C; 30.0°C.</p
3D-plot of measured output characteristics (flow rate Q<sub>DS</sub> vs. pressure p<sub>DS</sub> vs. ethanol concentration c<sub>Eth</sub>) of the MIS-CVPT at different temperatures <i>ϑ</i> ranging from 22.5°C to 30.0°C in 2.5K steps.
<p>3D-plot of measured output characteristics (flow rate Q<sub>DS</sub> vs. pressure p<sub>DS</sub> vs. ethanol concentration c<sub>Eth</sub>) of the MIS-CVPT at different temperatures <i>ϑ</i> ranging from 22.5°C to 30.0°C in 2.5K steps.</p
Electrically Tunable Dye Emission via Microcavity Integrated PDMS Gel Actuator
Electrically
tunable microcavities are essential elements for tunable laser sources
indispensable for modern telecommunication and spectroscopy. However,
most device concepts suffer from extensive lithography or etching
for membrane processing. Here, we present an electrically and continuously
tunable, multi-half-wavelength microcavity with a quality factor >
1000 as an easy-to-fabricate platform with potential use for vertical-cavity
surface-emitting lasers. The microcavity has a Fabry–Pérot
structure consisting of ultrasoft PDMS gel with a thickness of 14–15
μm and capped by a distributed Bragg reflector on the bottom
end and a silver layer serving as top mirror and electrode. Additionally,
we have embedded a pyrromethene dye into the PDMS matrix to prove
efficient gain medium integration. By means of an integrated dielectric
elastomer actuator, the microcavity thickness is varied 1.3 μm
(9%) with a driving voltage of 70 V. The subsequent silver mirror
deflection achieves a reversible 40 nm tuning of the cavity resonance
wavelength. The tuning range is limited by the lateral bending of
the electrodes for increasing voltages. This characteristic bending
is confirmed by simulations with finite elements method. The dynamic
behavior of the microcavity is characterized by capacitance measurements
and modeled by viscoelastic theory. Our research provides in-depth
examinations of electrically tunable, PDMS gel-based microcavities
with the future goal of building simple, miniaturized, and cost-efficient
laser sources with high tuning range