2017
DOI: 10.1016/j.compscitech.2017.10.020
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Improving the interfacial strength of silicone resin composites by chemically grafting silica nanoparticles on carbon fiber

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Cited by 91 publications
(37 citation statements)
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“…Hence, modifying the CF surfaces to create good interfacial properties can be crucial for increasing the composite's overall performances [10,11]. Recently, many approaches have been proposed for modifying carbon fiber surfaces to promote the interface properties of composites, such as coating or sizing, high-energy radiation, oxidation, chemical modification, and so on [12][13][14][15][16][17][18][19][20][21]. Among these approaches, chemical modification is considered to be one of the most effective approaches due to its simplicity and controllability without high energy.…”
Section: Introductionmentioning
confidence: 99%
“…Hence, modifying the CF surfaces to create good interfacial properties can be crucial for increasing the composite's overall performances [10,11]. Recently, many approaches have been proposed for modifying carbon fiber surfaces to promote the interface properties of composites, such as coating or sizing, high-energy radiation, oxidation, chemical modification, and so on [12][13][14][15][16][17][18][19][20][21]. Among these approaches, chemical modification is considered to be one of the most effective approaches due to its simplicity and controllability without high energy.…”
Section: Introductionmentioning
confidence: 99%
“…In the spectrum of SN, the absorption peaks at 1084, 947 and 795 cm −1 represent Si −O −Si asymmetric stretching vibration, Si −OH stretching vibration and Si −O −Si symmetric vibrations [37] . After being grafted by APTES, the new peak at 1405 cm −1 is assigned to the −NH 2 functional group, and the peaks at 2981 and 2896 cm −1 can be attributed to C-H stretching vibration belonging to APTES [38] . For SN@APTES-PWA, the unique bands of PWA (as presented in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…Contact angles were measured using a DSA100 instrument (Krüss, Germany). The dispersive components, polar components and total surface energy can be calculated according to Eqns : γ=γnormald+γnormalp,γnormals=γnormalsnormald+γnormalsnormalp,γnormall=γnormallnormald+γnormallnormalp γnormall1+cosθ=2()γldγsd1/2+2()γlpγsp1/2 where γ l ( γ s ), γ l d ( γ s d ) and γ l p ( γ s p ) are surface tension, dispersive and polar components of the test liquid (sample), respectively. In the present study, the test liquids were deionized water ( γ d = 21.8 mN m −1 , γ = 72.8 mN m −1 ) and glycerol ( γ d = 34.0 mN m −1 , γ = 64.0 mN m −1 ).…”
Section: Methodsmentioning
confidence: 99%