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COMSOL Inc simulation schematic diagram
a <t>Schematic</t> illustration about se-HICFs as self-powered sensor based on the principles of electrostatic induction ( b ) The working principle of se-HICFs for noncontact sensing. c The potential distribution during the se-HICFs sensing moving object simulated by the <t>COMSOL</t> software based on finite-element <t>simulation.</t> d The V oc of se-HICFs with different diameters in sensing the test object. e The V oc of se-HICFs in different sensing distance with the test object. f The V oc of se-HICFs when sensing test objects with different sizes. g The V oc of se-HICFs when sensing the PET film with area of 5 ⨯ 5 cm 2 with frequency from 0.5 to 2.5 Hz. h The V oc of se-HICFs when sensing different test objects with various materials. i The V oc of se-HICFs in diameter of 50 μm and 200 μm when sensing a PET film within 60 days. (The se-HICFs length is 10 cm, the PET film is in size of 5 ⨯ 5 cm 2 , the loading distance is 8 cm and the reference distance is 1 cm). The error bar for each data point in ( d – i ) is standard deviation calculated based on 3 parallel measurements.
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a Schematic illustration about se-HICFs as self-powered sensor based on the principles of electrostatic induction ( b ) The working principle of se-HICFs for noncontact sensing. c The potential distribution during the se-HICFs sensing moving object simulated by the COMSOL software based on finite-element simulation. d The V oc of se-HICFs with different diameters in sensing the test object. e The V oc of se-HICFs in different sensing distance with the test object. f The V oc of se-HICFs when sensing test objects with different sizes. g The V oc of se-HICFs when sensing the PET film with area of 5 ⨯ 5 cm 2 with frequency from 0.5 to 2.5 Hz. h The V oc of se-HICFs when sensing different test objects with various materials. i The V oc of se-HICFs in diameter of 50 μm and 200 μm when sensing a PET film within 60 days. (The se-HICFs length is 10 cm, the PET film is in size of 5 ⨯ 5 cm 2 , the loading distance is 8 cm and the reference distance is 1 cm). The error bar for each data point in ( d – i ) is standard deviation calculated based on 3 parallel measurements.

Journal: Nature Communications

Article Title: Self-encapsulated ionic fibers based on stress-induced adaptive phase transition for non-contact depth-of-field camouflage sensing

doi: 10.1038/s41467-024-44848-5

Figure Lengend Snippet: a Schematic illustration about se-HICFs as self-powered sensor based on the principles of electrostatic induction ( b ) The working principle of se-HICFs for noncontact sensing. c The potential distribution during the se-HICFs sensing moving object simulated by the COMSOL software based on finite-element simulation. d The V oc of se-HICFs with different diameters in sensing the test object. e The V oc of se-HICFs in different sensing distance with the test object. f The V oc of se-HICFs when sensing test objects with different sizes. g The V oc of se-HICFs when sensing the PET film with area of 5 ⨯ 5 cm 2 with frequency from 0.5 to 2.5 Hz. h The V oc of se-HICFs when sensing different test objects with various materials. i The V oc of se-HICFs in diameter of 50 μm and 200 μm when sensing a PET film within 60 days. (The se-HICFs length is 10 cm, the PET film is in size of 5 ⨯ 5 cm 2 , the loading distance is 8 cm and the reference distance is 1 cm). The error bar for each data point in ( d – i ) is standard deviation calculated based on 3 parallel measurements.

Article Snippet: The corresponding COMSOL simulation schematic diagram further confirmed the above non-contacting sensing principle through the calculated potential distribution (Fig. ) .

Techniques: Software, Standard Deviation