{"currentpage":1,"firstResult":0,"maxresult":10,"pagecode":5,"pageindex":{"endPagecode":5,"startPagecode":1},"records":[{"abstractinfo":"Based on the developed multiple-scattering theory [C.-W. Nan and F. S. Jin, Phys. Rev. B 48, 8578 (1993)], an effective-medium theory (EMT) is proposed to treat coupled electromechanical behavior in composite media. The explicit relations for determining effective behavior of piezoelectric composites are derived. To illustrate the technique, numerical results of piezoelectric ceramic/epoxy composites for various particle shapes are presented over the whole range of concentrations. The EMT estimates are shown to be in good agreement with available experimental results. Porous piezoelectric ceramics are also discussed. The EMT predicts a similar critical behavior for heterogeneous piezoelectric materials to recent experiments.","authors":[],"categoryName":"|","doi":"","fpage":"1155","id":"e7f59558-e05d-411c-962c-b1cfd1cce558","issue":"2","journal":{"abbrevTitle":"JOAP","id":"7dcf8a89-0513-40ee-be2d-759941dcef7e","issnPpub":"0021-8979","publisherId":"JOAP","title":"Journal of Applied Physics"},"keywords":[{"id":"941e4dc1-7057-468d-89f9-6b7b1fc4028f","keyword":"electromechanical properties;ceramics","originalKeyword":"electromechanical properties;ceramics"}],"language":"en","publisherId":"0021-8979_1994_2_1","title":"EFFECTIVE-MEDIUM THEORY OF PIEZOELECTRIC COMPOSITES","volume":"76","year":"1994"},{"abstractinfo":"As an analytical method, the effective-field theory (EFT) is used to study the dynamical response of the kinetic Ising model in the presence of a sinusoidal oscillating field. The effective-field equations of motion of the average magnetization are given for the square lattice (Z = 4) and the simple cubic lattice (Z = 6), respectively. The dynamic order parameter, the hysteresis loop area and the dynamic correlation are calculated. In the field amplitude h(0)/ZJ-temperature T/ZJ plane, the phase boundary separating the dynamic ordered and the disordered phase has been drawn. and the dynamical tricritical point has been observed. We also make the compare results of EFT with that given by using the mean field theory (MFT). (C) 2008 Elsevier B.V. All rights reserved.","authors":[],"categoryName":"|","doi":"","fpage":"5922","id":"82f9da7d-2e3b-46a9-bd3c-e16e5624c09f","issue":"37","journal":{"abbrevTitle":"PLA","id":"7b364793-d718-49d5-9832-ec34f0748fdf","issnPpub":"0375-9601","publisherId":"PLA","title":"Physics Letters A"},"keywords":[{"id":"5f9d1c9d-bc50-43ac-be4c-79b7a3763016","keyword":"kinetic Ising model;effective-field theory;phase transition;nonequilibrium phase-transition;oscillating field;magnetization;reversal;tricritical point;hysteresis;dynamics;resonance;systems;films","originalKeyword":"kinetic Ising model;effective-field theory;phase transition;nonequilibrium phase-transition;oscillating field;magnetization;reversal;tricritical point;hysteresis;dynamics;resonance;systems;films"}],"language":"en","publisherId":"0375-9601_2008_37_1","title":"Effective-field theory on the kinetic Ising model","volume":"372","year":"2008"},{"abstractinfo":"We build the perturbation expansion method for nonlinear composite media and extend the EMA for nonlinear effective conductivity. Using the solutions of boundary-value problems of a cylindrical in- clusion, we derive formulae for nonlinear effective conductivity.","authors":[{"authorName":"Guoqing GU+","id":"0262882c-d105-4b00-86bb-d2182ea6cefd","originalAuthorName":"Guoqing GU+"},{"authorName":" International Centre for Materials Physics","id":"d1c90eac-4d59-48df-bb04-140b7734ea2d","originalAuthorName":" International Centre for Materials Physics"},{"authorName":" Academia Sinica","id":"df077214-76ce-4ca9-834a-73059f8a6930","originalAuthorName":" Academia Sinica"},{"authorName":" 110015","id":"2ad0f2db-1d0a-44da-9880-e641f30078ce","originalAuthorName":" 110015"},{"authorName":" Shenyang","id":"93f9983e-e1c3-4dad-8e61-dedda328d7f1","originalAuthorName":" Shenyang"},{"authorName":" ChinaGe CHEN","id":"a018187c-272a-4dd9-8d05-f17ae59b6f02","originalAuthorName":" ChinaGe CHEN"},{"authorName":" College of Systems Science and Systems Engineering","id":"aab1f34c-163e-48af-84e1-55ad3bd92c39","originalAuthorName":" College of Systems Science and Systems Engineering"},{"authorName":" Shanghai Institute of Mechanical Engineering","id":"6b09ec47-9453-46e2-9936-defe3524a777","originalAuthorName":" Shanghai Institute of Mechanical Engineering"},{"authorName":" 200093","id":"2495f98f-f214-4a43-ac08-68790df5c5e1","originalAuthorName":" 200093"},{"authorName":" ShanghaiK.W.Yu","id":"05b5ac2d-adc8-41cd-a925-9968f6405dab","originalAuthorName":" ShanghaiK.W.Yu"},{"authorName":" Department of Physics","id":"b0c74d37-4cfa-4686-ae88-ced77b0f13a9","originalAuthorName":" Department of Physics"},{"authorName":" Chin","id":"125698f5-cd7a-49c9-8842-eead7f884544","originalAuthorName":" Chin"}],"categoryName":"|","doi":"","fpage":"145","id":"363aaa08-b66e-4a54-8875-5e373d513c09","issue":"2","journal":{"abbrevTitle":"CLKXJSY","coverImgSrc":"journal/img/cover/JMST.jpg","id":"11","issnPpub":"1005-0302 ","publisherId":"CLKXJSY","title":"材料科学技术(英文)"},"keywords":[{"id":"9e8400b9-1ec7-4a43-9627-0747ad4b3e8f","keyword":"effective medium approximation","originalKeyword":"effective medium approximation"},{"id":"2c7ac8cf-9a5f-40e6-b026-f42be6bd1583","keyword":"null","originalKeyword":"null"}],"language":"en","publisherId":"1005-0302_1993_2_14","title":"Effective Medium Approximation for Nonlinear Composite Media","volume":"9","year":"1993"},{"abstractinfo":"In this paper, we establish an effective medium approximation (EMA) for effective conductivity of nonlinear composite media. As an example, we consider a two-dimensional composite medium with a cylindrical inclusion embedded in a homogeneous host, both the host and the inclusion having nonlinear current-voltage constitutive relations, and apply the perturbation expansion method to derive its analytic series solution. Using the nonlinear EMA we derive the formulae of the first-, the third- and the fifth-order effective conductivities, which are valid for nonlinear composite media with middle concentration of inclusion.","authors":[],"categoryName":"|","doi":"","fpage":"265","id":"cc510201-1868-4d94-8b5a-d0ae992fa48d","issue":"3","journal":{"abbrevTitle":"CITP","id":"45f28bf6-874e-4b98-936f-4562e2c56a77","issnPpub":"0253-6102","publisherId":"CITP","title":"Communications in Theoretical Physics"},"keywords":[{"id":"db729137-84f3-4f79-9c8c-79e447f66cf0","keyword":"field","originalKeyword":"field"}],"language":"en","publisherId":"0253-6102_1994_3_1","title":"PERTURBATION EXPANSION METHOD AND EFFECTIVE-MEDIUM APPROXIMATION FOR EFFECTIVE CONDUCTIVITY OF NONLINEAR COMPOSITE MEDIA","volume":"22","year":"1994"},{"abstractinfo":"As an analytical method, the effective-field theory (EFT) is used to study the dynamical response of the kinetic Ising model in the presence of a sinusoidal oscillating field. The effective-field equations of motion of the average magnetization are given for the honeycomb lattice (Z=3). The Liapunov exponent lambda is calculated for discussing the stability of the magnetization and it is used to determine the phase boundary. In the field amplitude h(0)/ZJ-temperature T/ZJ plane, the phase boundary separating the dynamic ordered and the disordered phase has been drawn. In contrast to previous analytical results that predicted a tricritical point separating a dynamic phase boundary line of continuous and discontinuous transitions, we find that the transition is always continuous. There is inconsistency between our results and previous analytical results, because they do not introduce sufficiently strong fluctuations.","authors":[],"categoryName":"|","doi":"","fpage":"927","id":"519a54c2-9a9b-4133-a548-c03ab44a38f8","issue":"5","journal":{"abbrevTitle":"CITP","id":"45f28bf6-874e-4b98-936f-4562e2c56a77","issnPpub":"0253-6102","publisherId":"CITP","title":"Communications in Theoretical Physics"},"keywords":[{"id":"77e2aa17-582d-422e-bd4a-9843b2313b92","keyword":"kinetic Ising model;effective-field theory;phase transition;nonequilibrium phase-transition;oscillating field;magnetization;reversal;tricritical point;hysteresis;dynamics;resonance;systems;films","originalKeyword":"kinetic Ising model;effective-field theory;phase transition;nonequilibrium phase-transition;oscillating field;magnetization;reversal;tricritical point;hysteresis;dynamics;resonance;systems;films"}],"language":"en","publisherId":"0253-6102_2009_5_1","title":"Effective-Field Theory for Kinetic Ising Model on Honeycomb Lattice","volume":"51","year":"2009"},{"abstractinfo":"利用有效媒质理论描述了金属薄膜形成过程中电导率变化规律,与实验测得的Al薄膜形成过程中电导率变化结果比较接近.分析和讨论了一些影响计算结果准确性的因素.","authors":[{"authorName":"曹晓晖","id":"8c891112-840a-47ff-8dd9-2b869af6d617","originalAuthorName":"曹晓晖"},{"authorName":"唐兆麟","id":"a31a5071-a5fc-4d08-b48b-e2b12c3c6128","originalAuthorName":"唐兆麟"},{"authorName":"黄荣芳","id":"faf6eed6-8158-4075-9f1c-f673c412d4b4","originalAuthorName":"黄荣芳"},{"authorName":"闻立时","id":"b2beb568-8c5d-44d4-b751-0d70bfe6c4b9","originalAuthorName":"闻立时"},{"authorName":"师昌绪","id":"b831cbb4-937e-444f-bef0-61c2095572c5","originalAuthorName":"师昌绪"}],"categoryName":"|","doi":"","fpage":"404","id":"f9470af3-0deb-46a7-8f8f-bbdc41bfc975","issue":"4","journal":{"abbrevTitle":"JSXB","coverImgSrc":"journal/img/cover/JSXB.jpg","id":"48","issnPpub":"0412-1961","publisherId":"JSXB","title":"金属学报"},"keywords":[{"id":"aa86ea06-8759-4de4-bd7c-42f87d69f03b","keyword":"薄膜","originalKeyword":"薄膜"},{"id":"569d7311-144d-4e60-a722-c4e416261758","keyword":" conductivity","originalKeyword":" conductivity"},{"id":"5ef3c883-dafb-4ab4-ae0a-97f80f85fb05","keyword":" effective medium theory","originalKeyword":" effective medium theory"}],"language":"zh","publisherId":"0412-1961_1996_4_2","title":"金属薄膜形成过程中电导特性变化的有效媒质理论","volume":"32","year":"1996"},{"abstractinfo":"A relation between multiple-scattering theory and micromechanical models of effective elastic material properties of heterogeneous materials has been established within a unified theoretical framework, and exemplified on three important approximations. the average t-matrix (or Mori-Tanaka), symmetric self-consistency (coherent potential), and asymmetric self-consistency approximations. (C) 1996 Elsevier Science Limited and Techna S.r.l.","authors":[],"categoryName":"|","doi":"","fpage":"457","id":"7796d111-fd55-48a3-9dba-1d8c4250e3d0","issue":"6","journal":{"abbrevTitle":"CI","id":"c9dac959-f5a2-456a-9890-ad059e192bf2","issnPpub":"0272-8842","publisherId":"CI","title":"Ceramics International"},"keywords":[{"id":"96611384-3a3a-4a2d-9726-4cf18b1ad3ff","keyword":"elastic properties;polycrystals;inclusions;matrix","originalKeyword":"elastic properties;polycrystals;inclusions;matrix"}],"language":"en","publisherId":"0272-8842_1996_6_1","title":"A relation between multiple-scattering theory and micromechanical models of effective thermoelastic properties","volume":"22","year":"1996"},{"abstractinfo":"As an analytical method, the effective-field theory (EFT) is used to study an Ising spin system in a transverse magnetic field under a time oscillating longitudinal field. The effective-field equations of motion of the average magnetization are given for the square lattice (Z = 4). In the longitudinal field amplitude h(0)/Z J-transverse field Gamma/ZJ plane, the phase boundary separating the dynamic ordered and the disordered phase also has been drawn, and there is no dynamical tricritical point on the dynamic phase transition boundary. The dependence of the critical temperature on the transverse field is calculated and phase diagrams are presented. We also make the compare results of EFT with that given by using the mean field theory (MFT). (C) 2010 Elsevier B.V. All rights reserved.","authors":[],"categoryName":"|","doi":"","fpage":"1885","id":"3719b91b-5102-4d3c-b1a0-19f63784019f","issue":"17-18","journal":{"abbrevTitle":"PLA","id":"7b364793-d718-49d5-9832-ec34f0748fdf","issnPpub":"0375-9601","publisherId":"PLA","title":"Physics Letters A"},"keywords":[{"id":"f4dbced9-39c0-49c9-945a-1ddabf0f637c","keyword":"Transverse Ising model;Effective-field theory;Dynamic phase transition;nonequilibrium phase-transition;magnetization reversal;honeycomb;lattice;tricritical point;arbitrary spin;crystal-field;thin-films;hysteresis;dynamics;diagrams","originalKeyword":"Transverse Ising model;Effective-field theory;Dynamic phase transition;nonequilibrium phase-transition;magnetization reversal;honeycomb;lattice;tricritical point;arbitrary spin;crystal-field;thin-films;hysteresis;dynamics;diagrams"}],"language":"en","publisherId":"0375-9601_2010_17-18_1","title":"Effective-field theory on the transverse Ising model under a time oscillating longitudinal field","volume":"374","year":"2010"},{"abstractinfo":"The effective-field theory (EFT) is used to study the dynamical response of the kinetic spin-1 Blume-Capel model in the presence of a sinusoidal oscillating magnetic field. The effective-field dynamic equations are given for the honeycomb lattice (Z = 3). The dynamic order parameter, the dynamic quadruple moment, the hysteresis loop area and the dynamic correlation are calculated. We have found that the behavior of the system strongly depends on the crystal interaction D. The dynamic phase boundaries separating the paramagnetic phase and the ferromagnetic phase are obtained. There is the region of the phase space where both a paramagnetic phase and a ferromagnetic phase coexist. The dynamic transition from one region to the other can be of first or second order depending on the frequency of the magnetic field. There is no dynamic tricritical point on the dynamic phase transition line. The results are also compared with those obtained from the mean-field theory (MET). (C) 2011 Elsevier B.V. All rights reserved.","authors":[],"categoryName":"|","doi":"","fpage":"29","id":"6f9c77f5-382b-4563-a68b-f0a837a0b90e","issue":"42737","journal":{"abbrevTitle":"PAMAIA","id":"fc88484d-3bd5-4752-a5d2-ae874bc56c0a","issnPpub":"0378-4371","publisherId":"PAMAIA","title":"Physica a-Statistical Mechanics and Its Applications"},"keywords":[{"id":"939223bd-8a9f-40fc-9db5-8c4c35da3f46","keyword":"Kinetic spin-1 Blume-Capel model;Effective-field theory;Dynamic phase;transition;single-ion-anisotropy;ising-model;phase-transition;magnetization;reversal;systems;hysteresis;ferromagnet;dynamics;point;films","originalKeyword":"Kinetic spin-1 Blume-Capel model;Effective-field theory;Dynamic phase;transition;single-ion-anisotropy;ising-model;phase-transition;magnetization;reversal;systems;hysteresis;ferromagnet;dynamics;point;films"}],"language":"en","publisherId":"0378-4371_2012_42737_1","title":"Effective-field theory on the kinetic spin-1 Blume-Capel model","volume":"391","year":"2012"},{"abstractinfo":"","authors":[{"authorName":"","id":"473aeb92-154e-44c2-8c04-6802171c6ea9","originalAuthorName":""}],"doi":"","fpage":"367","id":"3f5ec04d-713d-4a8a-a309-266f960d4bac","issue":"4","journal":{"abbrevTitle":"CLKXJSY","coverImgSrc":"journal/img/cover/JMST.jpg","id":"11","issnPpub":"1005-0302 ","publisherId":"CLKXJSY","title":"材料科学技术(英文)"},"keywords":[{"id":"f1fbb637-461b-4ddb-b76a-2e859488e326","keyword":"","originalKeyword":""}],"language":"zh","publisherId":"clkxjsxb-e200004003","title":"Effective-Medium Theory for Two-Phase Random Composites with an Interfacial Shell","volume":"16","year":"2000"}],"totalpage":189,"totalrecord":1884}