3d field simulator Search Results


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ANSYS inc ansys maxwell3d software
Ansys Maxwell3d Software, supplied by ANSYS inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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Ansoft Corporation 3d field simulator software package
3d Field Simulator Software Package, supplied by Ansoft Corporation, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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COMSOL Inc 3d cfd model of the vmd process using comsol multi-physical field simulation software
Illustration of the induction heated <t>(IH)-VMD</t> <t>process.</t> Bottom layer: temperature profile in the feed; Middle layer: composite membrane; Top: vacuum chamber. Right image: enlargement of the Fe-CNTs layer . Reproduced with permission from Elsevier, 2019.
3d Cfd Model Of The Vmd Process Using Comsol Multi Physical Field Simulation Software, supplied by COMSOL Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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COMSOL Inc 3d full-field electromagnetic simulations of the microcylinders
Scanning electron microscope (SEM) images of (a) cleaved Si3N4 <t>microcylinders</t> and (b) lift-off Si3N4 microcylinders. The measured dimensions of these cylinders are shown below each image. The trapped orientations of the microcylinders on an nSWAT device were determined for both (c) cleaved Si3N4 microcylinders and (d) lift-off Si3N4 microcylinders based on their optical images. On an nSWAT device17, a 1064-nm laser is coupled into the TM mode of a Si3N4 waveguide (250 nm high and 750 nm wide) before passing through a 50/50 splitter that creates counter-propagating waves to form a standing wave within a fluidic pool region. The antinodes of the standing wave form trap centers for an array of traps. The entire trap array may also be translocated via a microheater, which changes the phase of one of the counter propagating waves. Bright field microscopy image scale bars in the inserts of (c) and (d) are 1 μm in length.
3d Full Field Electromagnetic Simulations Of The Microcylinders, supplied by COMSOL Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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COMSOL Inc 3d full-field finite element optical simulations comsol multiphysics
Scanning electron microscope (SEM) images of (a) cleaved Si3N4 <t>microcylinders</t> and (b) lift-off Si3N4 microcylinders. The measured dimensions of these cylinders are shown below each image. The trapped orientations of the microcylinders on an nSWAT device were determined for both (c) cleaved Si3N4 microcylinders and (d) lift-off Si3N4 microcylinders based on their optical images. On an nSWAT device17, a 1064-nm laser is coupled into the TM mode of a Si3N4 waveguide (250 nm high and 750 nm wide) before passing through a 50/50 splitter that creates counter-propagating waves to form a standing wave within a fluidic pool region. The antinodes of the standing wave form trap centers for an array of traps. The entire trap array may also be translocated via a microheater, which changes the phase of one of the counter propagating waves. Bright field microscopy image scale bars in the inserts of (c) and (d) are 1 μm in length.
3d Full Field Finite Element Optical Simulations Comsol Multiphysics, supplied by COMSOL Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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ANSYS inc 3d fluctuating wind field simulation
Scanning electron microscope (SEM) images of (a) cleaved Si3N4 <t>microcylinders</t> and (b) lift-off Si3N4 microcylinders. The measured dimensions of these cylinders are shown below each image. The trapped orientations of the microcylinders on an nSWAT device were determined for both (c) cleaved Si3N4 microcylinders and (d) lift-off Si3N4 microcylinders based on their optical images. On an nSWAT device17, a 1064-nm laser is coupled into the TM mode of a Si3N4 waveguide (250 nm high and 750 nm wide) before passing through a 50/50 splitter that creates counter-propagating waves to form a standing wave within a fluidic pool region. The antinodes of the standing wave form trap centers for an array of traps. The entire trap array may also be translocated via a microheater, which changes the phase of one of the counter propagating waves. Bright field microscopy image scale bars in the inserts of (c) and (d) are 1 μm in length.
3d Fluctuating Wind Field Simulation, supplied by ANSYS inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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COMSOL Inc 3d display and multiple physical field simulation
Scanning electron microscope (SEM) images of (a) cleaved Si3N4 <t>microcylinders</t> and (b) lift-off Si3N4 microcylinders. The measured dimensions of these cylinders are shown below each image. The trapped orientations of the microcylinders on an nSWAT device were determined for both (c) cleaved Si3N4 microcylinders and (d) lift-off Si3N4 microcylinders based on their optical images. On an nSWAT device17, a 1064-nm laser is coupled into the TM mode of a Si3N4 waveguide (250 nm high and 750 nm wide) before passing through a 50/50 splitter that creates counter-propagating waves to form a standing wave within a fluidic pool region. The antinodes of the standing wave form trap centers for an array of traps. The entire trap array may also be translocated via a microheater, which changes the phase of one of the counter propagating waves. Bright field microscopy image scale bars in the inserts of (c) and (d) are 1 μm in length.
3d Display And Multiple Physical Field Simulation, supplied by COMSOL Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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COMSOL Inc 3d electrical field simulations
Scanning electron microscope (SEM) images of (a) cleaved Si3N4 <t>microcylinders</t> and (b) lift-off Si3N4 microcylinders. The measured dimensions of these cylinders are shown below each image. The trapped orientations of the microcylinders on an nSWAT device were determined for both (c) cleaved Si3N4 microcylinders and (d) lift-off Si3N4 microcylinders based on their optical images. On an nSWAT device17, a 1064-nm laser is coupled into the TM mode of a Si3N4 waveguide (250 nm high and 750 nm wide) before passing through a 50/50 splitter that creates counter-propagating waves to form a standing wave within a fluidic pool region. The antinodes of the standing wave form trap centers for an array of traps. The entire trap array may also be translocated via a microheater, which changes the phase of one of the counter propagating waves. Bright field microscopy image scale bars in the inserts of (c) and (d) are 1 μm in length.
3d Electrical Field Simulations, supplied by COMSOL Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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3d electrical field simulations - by Bioz Stars, 2026-06
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COMSOL Inc simulated 3d plot of the distribution of electric field line
Scanning electron microscope (SEM) images of (a) cleaved Si3N4 <t>microcylinders</t> and (b) lift-off Si3N4 microcylinders. The measured dimensions of these cylinders are shown below each image. The trapped orientations of the microcylinders on an nSWAT device were determined for both (c) cleaved Si3N4 microcylinders and (d) lift-off Si3N4 microcylinders based on their optical images. On an nSWAT device17, a 1064-nm laser is coupled into the TM mode of a Si3N4 waveguide (250 nm high and 750 nm wide) before passing through a 50/50 splitter that creates counter-propagating waves to form a standing wave within a fluidic pool region. The antinodes of the standing wave form trap centers for an array of traps. The entire trap array may also be translocated via a microheater, which changes the phase of one of the counter propagating waves. Bright field microscopy image scale bars in the inserts of (c) and (d) are 1 μm in length.
Simulated 3d Plot Of The Distribution Of Electric Field Line, supplied by COMSOL Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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simulated 3d plot of the distribution of electric field line - by Bioz Stars, 2026-06
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Ansoft Corporation maxwell 3-d field simulation software
Scanning electron microscope (SEM) images of (a) cleaved Si3N4 <t>microcylinders</t> and (b) lift-off Si3N4 microcylinders. The measured dimensions of these cylinders are shown below each image. The trapped orientations of the microcylinders on an nSWAT device were determined for both (c) cleaved Si3N4 microcylinders and (d) lift-off Si3N4 microcylinders based on their optical images. On an nSWAT device17, a 1064-nm laser is coupled into the TM mode of a Si3N4 waveguide (250 nm high and 750 nm wide) before passing through a 50/50 splitter that creates counter-propagating waves to form a standing wave within a fluidic pool region. The antinodes of the standing wave form trap centers for an array of traps. The entire trap array may also be translocated via a microheater, which changes the phase of one of the counter propagating waves. Bright field microscopy image scale bars in the inserts of (c) and (d) are 1 μm in length.
Maxwell 3 D Field Simulation Software, supplied by Ansoft Corporation, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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COMSOL Inc 3d electric field simulation software
Scanning electron microscope (SEM) images of (a) cleaved Si3N4 <t>microcylinders</t> and (b) lift-off Si3N4 microcylinders. The measured dimensions of these cylinders are shown below each image. The trapped orientations of the microcylinders on an nSWAT device were determined for both (c) cleaved Si3N4 microcylinders and (d) lift-off Si3N4 microcylinders based on their optical images. On an nSWAT device17, a 1064-nm laser is coupled into the TM mode of a Si3N4 waveguide (250 nm high and 750 nm wide) before passing through a 50/50 splitter that creates counter-propagating waves to form a standing wave within a fluidic pool region. The antinodes of the standing wave form trap centers for an array of traps. The entire trap array may also be translocated via a microheater, which changes the phase of one of the counter propagating waves. Bright field microscopy image scale bars in the inserts of (c) and (d) are 1 μm in length.
3d Electric Field Simulation Software, supplied by COMSOL Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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COMSOL Inc 3-d magnetic field simulations
Scanning electron microscope (SEM) images of (a) cleaved Si3N4 <t>microcylinders</t> and (b) lift-off Si3N4 microcylinders. The measured dimensions of these cylinders are shown below each image. The trapped orientations of the microcylinders on an nSWAT device were determined for both (c) cleaved Si3N4 microcylinders and (d) lift-off Si3N4 microcylinders based on their optical images. On an nSWAT device17, a 1064-nm laser is coupled into the TM mode of a Si3N4 waveguide (250 nm high and 750 nm wide) before passing through a 50/50 splitter that creates counter-propagating waves to form a standing wave within a fluidic pool region. The antinodes of the standing wave form trap centers for an array of traps. The entire trap array may also be translocated via a microheater, which changes the phase of one of the counter propagating waves. Bright field microscopy image scale bars in the inserts of (c) and (d) are 1 μm in length.
3 D Magnetic Field Simulations, supplied by COMSOL Inc, used in various techniques. Bioz Stars score: 90/100, based on 1 PubMed citations. ZERO BIAS - scores, article reviews, protocol conditions and more
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Image Search Results


Illustration of the induction heated (IH)-VMD process. Bottom layer: temperature profile in the feed; Middle layer: composite membrane; Top: vacuum chamber. Right image: enlargement of the Fe-CNTs layer . Reproduced with permission from Elsevier, 2019.

Journal: Membranes

Article Title: Research Progress in Computational Fluid Dynamics Simulations of Membrane Distillation Processes: A Review

doi: 10.3390/membranes11070513

Figure Lengend Snippet: Illustration of the induction heated (IH)-VMD process. Bottom layer: temperature profile in the feed; Middle layer: composite membrane; Top: vacuum chamber. Right image: enlargement of the Fe-CNTs layer . Reproduced with permission from Elsevier, 2019.

Article Snippet: A 3D CFD model of the VMD process using COMSOL multi-physical field simulation software was established [ ], which could predict the permeate flux and surface temperature in the process.

Techniques: Membrane

Scanning electron microscope (SEM) images of (a) cleaved Si3N4 microcylinders and (b) lift-off Si3N4 microcylinders. The measured dimensions of these cylinders are shown below each image. The trapped orientations of the microcylinders on an nSWAT device were determined for both (c) cleaved Si3N4 microcylinders and (d) lift-off Si3N4 microcylinders based on their optical images. On an nSWAT device17, a 1064-nm laser is coupled into the TM mode of a Si3N4 waveguide (250 nm high and 750 nm wide) before passing through a 50/50 splitter that creates counter-propagating waves to form a standing wave within a fluidic pool region. The antinodes of the standing wave form trap centers for an array of traps. The entire trap array may also be translocated via a microheater, which changes the phase of one of the counter propagating waves. Bright field microscopy image scale bars in the inserts of (c) and (d) are 1 μm in length.

Journal: ACS applied materials & interfaces

Article Title: High Trap Stiffness Microcylinders for Nanophotonic Trapping

doi: 10.1021/acsami.9b10041

Figure Lengend Snippet: Scanning electron microscope (SEM) images of (a) cleaved Si3N4 microcylinders and (b) lift-off Si3N4 microcylinders. The measured dimensions of these cylinders are shown below each image. The trapped orientations of the microcylinders on an nSWAT device were determined for both (c) cleaved Si3N4 microcylinders and (d) lift-off Si3N4 microcylinders based on their optical images. On an nSWAT device17, a 1064-nm laser is coupled into the TM mode of a Si3N4 waveguide (250 nm high and 750 nm wide) before passing through a 50/50 splitter that creates counter-propagating waves to form a standing wave within a fluidic pool region. The antinodes of the standing wave form trap centers for an array of traps. The entire trap array may also be translocated via a microheater, which changes the phase of one of the counter propagating waves. Bright field microscopy image scale bars in the inserts of (c) and (d) are 1 μm in length.

Article Snippet: To quantitatively assess trap stiffness enhancement with the use of Si 3 N 4 microcylinders, we first performed 3D full-field electromagnetic simulations of the microcylinders using the COMSOL Multiphysics finite element method software.

Techniques: Microscopy

(a) Trap stiffness may be measured by the power spectrum of the trapped particle motion. The example shown here is a measurement from a cleaved microcylinder at ~6 mW of laser power at the trapping region (540 Hz camera sampling rate, ~5–10 seconds per trace). A fit to the power spectrum using a Lorentzian function yields a trap stiffness of 4.16 pN/(nm-W). (b) Trap stiffness may also be measured by the variance of the trapped particle motion. The same trace as shown in (a) was analyzed based on the variance of the particle motion and equipartition theory. This yielded a trap stiffness of 3.94 pN/(nm-W). (c) A comparison of the measured trap stiffness enhancement for the cleaved (N = 11) and lift-off (N = 6) microcylinders relative to the measured values for more conventional 380-nm polystyrene microspheres (N = 18). The viscous drag coefficient was measured to be 22.2 ± 4.0 × 10−6 pN-sec/nm for lift-off microcylinders, and 19.2 ± 1.9 × 10−6 pN-sec/nm for cleaved microcylinders. Error bars are standard deviations. Results from simulations are also shown for comparison with error bars obtained from a distribution of simulated microcylinders that match the size distribution of fabricated microcylinders.

Journal: ACS applied materials & interfaces

Article Title: High Trap Stiffness Microcylinders for Nanophotonic Trapping

doi: 10.1021/acsami.9b10041

Figure Lengend Snippet: (a) Trap stiffness may be measured by the power spectrum of the trapped particle motion. The example shown here is a measurement from a cleaved microcylinder at ~6 mW of laser power at the trapping region (540 Hz camera sampling rate, ~5–10 seconds per trace). A fit to the power spectrum using a Lorentzian function yields a trap stiffness of 4.16 pN/(nm-W). (b) Trap stiffness may also be measured by the variance of the trapped particle motion. The same trace as shown in (a) was analyzed based on the variance of the particle motion and equipartition theory. This yielded a trap stiffness of 3.94 pN/(nm-W). (c) A comparison of the measured trap stiffness enhancement for the cleaved (N = 11) and lift-off (N = 6) microcylinders relative to the measured values for more conventional 380-nm polystyrene microspheres (N = 18). The viscous drag coefficient was measured to be 22.2 ± 4.0 × 10−6 pN-sec/nm for lift-off microcylinders, and 19.2 ± 1.9 × 10−6 pN-sec/nm for cleaved microcylinders. Error bars are standard deviations. Results from simulations are also shown for comparison with error bars obtained from a distribution of simulated microcylinders that match the size distribution of fabricated microcylinders.

Article Snippet: To quantitatively assess trap stiffness enhancement with the use of Si 3 N 4 microcylinders, we first performed 3D full-field electromagnetic simulations of the microcylinders using the COMSOL Multiphysics finite element method software.

Techniques: Sampling, Comparison