完整後設資料紀錄
DC 欄位語言
dc.contributor.author黃子瑜en_US
dc.contributor.authorHuang, Tzu-Yuen_US
dc.contributor.author郭心怡en_US
dc.contributor.authorKuo, Hsin-Yien_US
dc.date.accessioned2015-11-26T00:57:13Z-
dc.date.available2015-11-26T00:57:13Z-
dc.date.issued2015en_US
dc.identifier.urihttp://140.113.39.130/cdrfb3/record/nctu/#GT070251228en_US
dc.identifier.urihttp://hdl.handle.net/11536/126999-
dc.description.abstract本研究探討具弱非完美交界面壓電壓磁纖維複合材料在平面應變與橫向電磁場下之等效材料性質與磁電耦合行為。弱非完美意旨在交界面上法線方向之廣義應力:應力、電位移、磁通量密度傳遞連續,廣義勢能:應變、電場、磁場傳遞不連續,而本研究假設此不連續變化值與所對應之法線方向廣義應力項呈一線性比例關係(Linear spring-type interface),並藉由複變函數與微觀力學模型Mori-Tanaka模式、Ad hoc approximation模式以及雙層法(Two-level recursive scheme)來計算上述等效材料性質。 研究成果顯示,上述方法所預測之等效材料性質在不同內含物體積比下,皆有良好的一致性,除了C11 、C12 與(C11-C12)/2 在Ad hoc approximation模式預測上,只在些微弱非完美時(Slightly weakened interfaces)才會接近正確值;而雙層法的成功應用,得到非完美交界面可用三相複合材料來模擬。受到弱非完美交界面影響,本研究得到最大磁電電壓係數 分別為0.0048V/cmOe (BTO/CFO,fi=0.147 )與0.0038V/cmOe (CFO/BTO,fi=0.91 ),此數值相較完美交界面最大值0.9194V/cmOe (BTO/CFO,fi=0.063 )與0.9827V/cmOe (CFO/BTO,fi=0.937 )分別下降190倍與260倍,遠不及實際元件應用範圍;此外,等效材料性質因交界面弱非完美影響,具有內含物尺寸效應(Size-dependent effect)。zh_TW
dc.description.abstractThis research studies the effective properties and magneto-electric (ME) coupling of piezoelectric-piezomagnetic fibrous composites with mechanically compliant and weakly electromagnetic conducting interface under generalized plane strain with transverse electromagnetic fields. In this case, we assume that the displacement and potential have a jump across the interface and proportional to the normal components of the stress, electric displacement and magnetic flux density. The closed-form formula of the effective properties is obtained by using the complex variable approach and adopting micromechanical models. The numerical results obtained from different methods are shown in agreement, while the result of ad hoc approximation of C11 、C12 and (C11-C12)/2 is only correct for the interface condition of slightly weakened. The results obtained from the Mori-Tanaka method and the two-level recursive scheme show that the imperfect effect is equivalent to a three-phase composite. Due to the interface imperfection, the maximum magnetoelectric voltage coefficients become 0.0048V/cmOe (BTO/CFO,fi=0.147) and 0.0038V/cmOe (CFO/BTO,fi=0.91), which decrease by 190 times and 260 times compared to the case of perfect interface. Finally, we also study the size-dependent effect numerically.en_US
dc.language.isozh_TWen_US
dc.subject壓電壓磁纖維複合材料zh_TW
dc.subject平面應變與橫向電磁場zh_TW
dc.subject弱非完美交界面zh_TW
dc.subject複變函數zh_TW
dc.subjectMori-Tanaka模式zh_TW
dc.subjectAd hoc approximation模式zh_TW
dc.subject等效材料性質zh_TW
dc.subject磁電耦和效應zh_TW
dc.subjectpiezoelectric-piezomagnetic fibrous compositesen_US
dc.subjectgeneralized plane strain with transverse electromagnetic fieldsen_US
dc.subjectlinear spring-type interfaceen_US
dc.subjectcomplex variable approachen_US
dc.subjectMori-Tanaka methoden_US
dc.subjectAd hoc approximation methoden_US
dc.subjecteffective propertiesen_US
dc.subjectmagneto-electric (ME) couplingen_US
dc.title具弱非完美交界面多鐵性纖維複合材料 : 廣義面內問題zh_TW
dc.titleMultiferroic fibrous composites with spring-type imperfect interface : Generalized plane problemen_US
dc.typeThesisen_US
dc.contributor.department土木工程系所zh_TW
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