2011
DOI: 10.1016/j.apsusc.2011.07.095
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Synthesis and characterization of Parylene C/nanosilica composite film

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Cited by 9 publications
(5 citation statements)
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“…This assumption is possible because of the nature of parylene-C, which is flexible as a thin film but not inherently stretchable due to its relatively low elastic strain limit (1.5%−2.8%). [36,37] The maximum length of the unfolded electrode per period is taken as the arc length of the sine wave in one period. The modeled strain is thus calculated as the percentage ratio between maximum deformation (electrode in the fully unfolded state) and original length (electrode in the relaxed folded state), as follows:…”
Section: Resultsmentioning
confidence: 99%
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“…This assumption is possible because of the nature of parylene-C, which is flexible as a thin film but not inherently stretchable due to its relatively low elastic strain limit (1.5%−2.8%). [36,37] The maximum length of the unfolded electrode per period is taken as the arc length of the sine wave in one period. The modeled strain is thus calculated as the percentage ratio between maximum deformation (electrode in the fully unfolded state) and original length (electrode in the relaxed folded state), as follows:…”
Section: Resultsmentioning
confidence: 99%
“…This assumption is possible because of the nature of parylene‐C, which is flexible as a thin film but not inherently stretchable due to its relatively low elastic strain limit (1.5%−2.8%). [ 36,37 ] The maximum length of the unfolded electrode per period is taken as the arc length of the sine wave in one period. The modeled strain is thus calculated as the percentage ratio between maximum deformation (electrode in the fully unfolded state) and original length (electrode in the relaxed folded state), as follows: strain%θ,h=LunfoldedLrelaxedLrelaxed·100=0λ1+()π·tanθ·cosπ·tanθh·x2dxλλ·100$$\begin{eqnarray} &&\hspace*{-6pt}{\mathrm{strain}}_{\%}\left(\theta ,h\right) = \frac{{L}_{\mathrm{unfolded}} - {L}_{\mathrm{relaxed}}}{{L}_{\mathrm{relaxed}}} \cdot 100\nonumber\\ &&\hspace*{6pt}=\, \frac{\int_{0}^{\lambda}\sqrt{1+\left(\pi \cdot \tan \theta \cdot \cos \left(\frac{\pi \cdot \tan \theta}{h}\cdot x\right)\right)^{2}}\textit{dx} - \lambda}{\lambda}\cdot 100 \end{eqnarray}$$ withλ0.33embadbreak=2htanθ$$\begin{equation}{\mathrm{with\ }}\lambda \ = \frac{{2h}}{{{\mathrm{tan}}\theta }}\end{equation}$$where λ is the wavelength of the sine wave and depends directly on h and θ .…”
Section: Resultsmentioning
confidence: 99%
“…Unless otherwise stated, all parylene in this paper are the parylene C. The raw materials or dimer of the parylene C were also purchased from SCS Company, USA. The detailed deposition process are reported earlier by our group [51]. The whole wafer was annealed in N2 atmosphere at 200°C for 36 hours.…”
Section: Introductionmentioning
confidence: 99%
“…Compared to pure parylene C and other pure materials such as SiO 2 , polyimide, polyethylene, alumina (Al 2 O 3 ), benzocyclobutenes (BCB) and SiO 2 /poly(methyl methacrylate) (PMMA), nanocomposite parylene C (NCPC) exhibits some interesting properties [3947]. As an example, parylene C/Silica nanocomposites show greatly improved mechanical properties and thermal stability in comparison to pure PPXC films [48]. In a recent study, these properties, and especially thermal and UV stability, were further improved by combining nanosilica/titania particles with parylene C [49].…”
Section: Introductionmentioning
confidence: 99%