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18 protocols using vhx 900

1

Mosquito Proboscis Mechanics and Damping

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The proboscis is modeled as an end-loaded cantilever beam. Three proboscises were excised from the head and affixed to a rigid rod with UV-curable glue and filmed within 10-min of excision. A Keyence VHX-900 digital microscope, which has internal pixel calibration, is used to measure proboscis diameter and cantilevered length at a magnification of 150x. The Keyence VHX-900 also films the accumulation of water produced by an ultrasonic humidifier. All deposited moisture except a single droplet is removed manually before measurement. The deflection of the proboscis under the weight of the single droplet is measured optically by photographic measurements in OSPT. The experiment was replicated twice for each proboscis to achieve an average value. Damping characteristics are determined by using a modified cubic flight arena of characteristic length 37.5 mm to inhibit free flight and ground the mosquitoes. The mosquitoes are vibrated at a fixed frequency of 25 Hz and 50 Hz for a few seconds to establish sinusoidal behavior, and then vibration is ceased. Videos are analyzed with OSPT.
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2

Oscillatory Behavior of Cylindrical Gels

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The cylindrical self-oscillating gels were immersed in a catalyst-free BZ solution containing HNO3 (894 mM), NaBrO3 (100 mM) and malonic acid (64 mM) at 20 °C. The time profiles of the gel diameter during self-oscillation were observed from images recorded by an optical microscope (VHX 900, Keyence, Osaka, Japan ). The images were analyzed by ImageJ software.
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3

Thermally Responsive Gel Swelling Analysis

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The gel samples were equilibrated in water containing 894 mM HNO 3 and 84 mM NaBrO 3 for the oxidized state (Ru(bpy) 3 3+ ) and 894 mM HNO 3 , 64 mM MA, and 84 mM NaCl for the reduced state (Ru(bpy) 3 2+ ). NaCl was added to maintain the ionic strength. Photos of the gels in each redox state were recorded by an optical microscope (Keyence, VHX 900). The acquired images were analyzed with ImageJ software (NIH) to calculate the gel diameters at the various temperature points. The equilibrium swelling ratios were calculated by dividing the measured gel diameters (d) by the inner diameter of the glass capillary (d o , 850 μm) utilized in fabricating the poly(NIPAAm-r-NAPMAm) base gel. The analyzed data were modeled by a Boltzmann sigmoidal equation (Eq. S1).
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4

Imaging and Analysis of PHH/HSC Sheets

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PHH/HSC sheets were imaged on day 11 using digital microscopy (VHX-900, KEYENCE Ltd., Osaka, Japan) and optical coherence tomography (IVS-2000, KEYENCE Ltd.). The area of the PHH/HSC sheets was analyzed using ImageJ ver. 1.53 (NIH, Bethesda, MD, USA). The sheet thickness of was calculated from the cross-sectional area by randomly imaging three different areas in each sheet using optical coherence tomography.
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5

Charpy Impact Behavior of Steel Bars

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The appearance of the samples after the Charpy test was taken through a digital microscope, VHX-900 (Keyence corporation, Osaka, Japan), and digital camera. The microstructures were observed through a scanning electron microscope (SEM), VE-7800 (Keyence Corporation, Osaka, Japan), operated at 15 kV. The electron backscattered diffraction analysis was conducted using a 7001F (JEOL, Tokyo, Japan) equipped with a TSL-OIM analytical system.
For each steel bar, full-size 2 mm V-notched specimens with a notch radius of 0.25 mm were machined along the RD, as shown in Figure 3b, and instrumented Charpy impact tests were conducted under a 500 J capacity using CIEM-500D (Tokyo Koki Testing Machine Co., LTD., Sagamihara, Japan). The P and u during the impact test were recorded every 2.0 μs. The value of DBTT was determined from the Charpy curve, i.e., DBTT denoted the absorbed energy transition temperature corresponding to the half value of the vEu.
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6

Oscillating Hydrogel Dynamics Characterization

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The gels were immersed in a catalyst-free BZ solution containing 894 mM HNO 3 , 84 mM NaBrO 3 , and 64 mM malonic acid at 20 °C. The time profiles of the gel diameter during self-oscillation were observed from images recorded by an optical microscope (Keyence, VHX 900). Based on the gel diameter profiles (Fig. S1), the amplitude, swelling rates, and deswelling rates were calculated and plotted as a function of time. Note that the analysis methods for each component are provided in Fig. S2.
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7

Micro-Nanofluidic Device Fabrication

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To fabricate the micro-nanofluidic device, electron beam lithography (ELS-7500; Elionix, Tokyo, Japan) and the dry etching apparatus (NLD-550; ULVAC Co., Ltd., Kanagawa, Japan) were used. A pH meter (F-72; HORIBA, Kyoto, Japan) and an ultrapure water system (Direct-Q UV3; Merck, Tokyo, Japan) were used to prepare the HEPES and PBS buffers. A digital microscope and a fluorescence microscope equipped with a CCD camera (VHX-900 and VB-7010, respectively; KEYENCE, Osaka, Japan) were used to observe the fluorescence. The constant voltage applied to the sorting device came from a high-voltage power supply (HVS448LC-6000D; LabSmith, CA, USA). A UV/O3 apparatus (Filgen, Aichi, Japan) was used for bonding the silica device and the PDMS reservoir. The particle sizes before and after the proposed sorting were measured using qNano (IZON Science Ltd., Christchurch, New Zealand). A dynamic light scattering (DLS) apparatus (ELSZ-DN2; Otsuka Electronics Co., Ltd., Osaka, Japan) was used to measure the sizes of fluorescent NPs (Figures S2–S5). A tube rotator (TR-350, AS ONE Co., Ltd., Osaka, Japan) and aluminum block bath with a cool-thermo unit (CTU-mini, TAITEC Co., Ltd., Saitama, Japan) were employed for labeling exosomes
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8

Microscopic Observation of Ice Crystal Formation

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1 μL
of the suspension and a 15 μm thick stainless shim ring (Iwata
MFG. Co., Ltd.: RS012016001) were placed between two cover glasses
with thicknesses ranging from 0.012 to 0.017 mm and a diameter of
16 mm. The cover glasses were placed on the cooling stage of a microscope
(Linkam Scientific Instruments: HF95). The temperature of the stage
was cooled to −60 °C at a rate of −90 °C/min,
followed by immediately warming to −10 °C at a rate of
+5 °C/min, which was maintained for 6 h. Images were captured
every 60 min using a digital microscope (KEYENCE Corporation: VHX-900).
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9

RNAi Interference for Pigmentation Study in Ladybugs

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DsRNA synthesis and microinjection into larvae were performed as described previously19 (link). In brief, the cloned cDNA fragments in DNA vectors were amplified by PCR using the primers flanked with the T7 promoter sequence (Supplementary Table 6), and used as templates for dsRNA synthesis. Amplified PCR products were separated by electrophoresis on 1% agarose gels and purified using MagExtractor PCR & Gel Clean up kit (Toyobo). DsRNAs were synthesised using the MEGA script T7 kit (Ambion). Approximately 1.4−2.7 μg and 1.4−2.0 μg of the dsRNAs of Ha-pnr and Cs-pnr were injected into 2-day-old forth (final) instar larvae, respectively. Approximately 2.0−2.7 μg and 1.4–2.7 μg of the EGFP dsRNA were injected into H. axyridis and C. septempunctata larvae as negative controls, respectively. For other genes in the initial small screening, approximately 1 µg of dsRNA was injected into each early last instar larva. Different amount of dsRNA for each gene in this range gave no difference in phenotypic effects. In order to give enough time for the completion of pigmentation, images of adults were captured more than 2 days after eclosion using a digital microscope (VHX-900, Keyence).
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10

Characterization of Shape Memory Polymer Films

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Dynamic mechanical analysis (DMA) was carried out on DMA/SDTA861e (Mettler-Toledo, Greifensee, Switzerland) and DMA Q800/RSA3 (TA Instruments, New Castle, DE, USA) in a tension mold. The pre-designed nanocone arrays images of the PVA films surface were obtained by field emission environmental scanning electron microscopy (SEM, Quanta 200 FEG, FEI, Hillsborough, OR, USA), Atomic Force Microscope (AFM, Dimension Icon, Bruker, Karlsruhe, Germany), and optical microscopy (VHX-900, Keyence, Osaka, Japan). The transmission spectra of the SMP films were obtained using a UV–VIS spectrophotometer (Shimadzu UV-3600, Shimadzu, Kyoto, Japan). The reflectance of the SMP films with and without nanocone structures was recorded by a home-built reflectance measurement set up.
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