標(biāo)題: Titlebook: An Introduction to the Theory of Piezoelectricity; Jiashi Yang Textbook 2018Latest edition Springer Nature Switzerland AG 2018 Piezoelectr [打印本頁] 作者: 遠(yuǎn)見 時(shí)間: 2025-3-21 17:35
書目名稱An Introduction to the Theory of Piezoelectricity影響因子(影響力)
書目名稱An Introduction to the Theory of Piezoelectricity影響因子(影響力)學(xué)科排名
書目名稱An Introduction to the Theory of Piezoelectricity網(wǎng)絡(luò)公開度
書目名稱An Introduction to the Theory of Piezoelectricity網(wǎng)絡(luò)公開度學(xué)科排名
書目名稱An Introduction to the Theory of Piezoelectricity被引頻次
書目名稱An Introduction to the Theory of Piezoelectricity被引頻次學(xué)科排名
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書目名稱An Introduction to the Theory of Piezoelectricity讀者反饋
書目名稱An Introduction to the Theory of Piezoelectricity讀者反饋學(xué)科排名
作者: Morphine 時(shí)間: 2025-3-21 20:46 作者: 縫紉 時(shí)間: 2025-3-22 00:58
https://doi.org/10.1007/978-3-642-92992-2ation, the summation convention for repeated tensor indices, and the convention that a comma followed by an index denotes partial differentiation with respect to the coordinate associated with the index.作者: Vsd168 時(shí)間: 2025-3-22 08:28 作者: 收集 時(shí)間: 2025-3-22 08:52 作者: 歡騰 時(shí)間: 2025-3-22 14:52 作者: Medicaid 時(shí)間: 2025-3-22 17:32 作者: 象形文字 時(shí)間: 2025-3-23 00:13
https://doi.org/10.1007/978-3-642-92992-2d in the linear theory of piezoelectricity may skip this chapter and begin with Chap. ., Sect. .. This chapter uses the two-point Cartesian tensor notation, the summation convention for repeated tensor indices, and the convention that a comma followed by an index denotes partial differentiation with作者: 仔細(xì)檢查 時(shí)間: 2025-3-23 05:05 作者: adulterant 時(shí)間: 2025-3-23 07:21
https://doi.org/10.1007/978-3-322-98874-4ions of homogeneous differential equations and boundary conditions. Sections 4.2, 4.3, 4.4, 4.5, 4.6, 4.7, 4.8, 4.9, 4.10, 4.11, 4.12, and 4.13 are on antiplane problems of polarized ceramics for which the notation in Sect. 2.9 is followed.作者: 我邪惡 時(shí)間: 2025-3-23 12:06
https://doi.org/10.37307/b.978-3-503-21135-7 in-plane dimensions of the plates are infinite, what matters is the finite plate thickness. Sects. 5.2 and 5.7 are on antiplane problems of polarized ceramics for which the notation in Sect. 2.9 is followed. The solutions in Sects. 5.1, 5.2, 5.3, 5.4, 5.5, 5.6, and 5.7 are exact. Those in Sects. 5.作者: 才能 時(shí)間: 2025-3-23 16:46 作者: 原告 時(shí)間: 2025-3-23 18:35
Die friedliche Anwendung der AtomenergieChap. .. These include the effects of heat conduction; mechanical and electrical dissipations due to viscosity, dielectric loss and semiconduction; nonlocal and gradients effects; as well as electromagnetic effects.作者: 誘拐 時(shí)間: 2025-3-24 01:49
Die friedliche Anwendung der Atomenergiericity. In particular, Sect. 8.2 is an antiplane problem for which the notation of Section 2.9 is followed. Sections 8.4 and 8.5 employ approximate one-dimensional equations for thin rods. Sections 8.6 and 8.7 are on elastic rods and beams with piezoelectric elements in extension and bending, respec作者: flavonoids 時(shí)間: 2025-3-24 04:53 作者: Infirm 時(shí)間: 2025-3-24 07:09 作者: 杠桿支點(diǎn) 時(shí)間: 2025-3-24 11:06
Vibrations of Finite Bodies, in-plane dimensions of the plates are infinite, what matters is the finite plate thickness. Sects. 5.2 and 5.7 are on antiplane problems of polarized ceramics for which the notation in Sect. 2.9 is followed. The solutions in Sects. 5.1, 5.2, 5.3, 5.4, 5.5, 5.6, and 5.7 are exact. Those in Sects. 5.8, 5.9, and 5.10 are approximate.作者: Canvas 時(shí)間: 2025-3-24 18:52
Other Effects,Chap. .. These include the effects of heat conduction; mechanical and electrical dissipations due to viscosity, dielectric loss and semiconduction; nonlocal and gradients effects; as well as electromagnetic effects.作者: 憤怒歷史 時(shí)間: 2025-3-24 20:51
Piezoelectric Devices,ricity. In particular, Sect. 8.2 is an antiplane problem for which the notation of Section 2.9 is followed. Sections 8.4 and 8.5 employ approximate one-dimensional equations for thin rods. Sections 8.6 and 8.7 are on elastic rods and beams with piezoelectric elements in extension and bending, respectively.作者: Indolent 時(shí)間: 2025-3-25 03:08
https://doi.org/10.1007/978-3-642-92992-2In this chapter we specialize on the nonlinear equations in Chap. . for large deformations and strong fields to the case of infinitesimal deformations and weak fields, which results in the linear theory of piezoelectricity. A few theoretical aspects of the linear theory are also discussed.作者: COMMA 時(shí)間: 2025-3-25 03:42
Linear Theory of Piezoelectricity,In this chapter we specialize on the nonlinear equations in Chap. . for large deformations and strong fields to the case of infinitesimal deformations and weak fields, which results in the linear theory of piezoelectricity. A few theoretical aspects of the linear theory are also discussed.作者: 極微小 時(shí)間: 2025-3-25 10:37 作者: 冷淡周邊 時(shí)間: 2025-3-25 14:16
Springer Nature Switzerland AG 2018作者: Pedagogy 時(shí)間: 2025-3-25 18:16 作者: 修剪過的樹籬 時(shí)間: 2025-3-25 23:02
https://doi.org/10.1007/978-3-322-98874-4vices are discussed. The concept of electromechanical coupling factor is introduced. In Particular, Sects. 3.3, 3.4, 3.8, 3.9, 3.10, 3.11, 3.12, and 3.13 are on antiplane deformations of polarized ceramics [1].作者: 符合你規(guī)定 時(shí)間: 2025-3-26 02:22 作者: COMMA 時(shí)間: 2025-3-26 04:43
https://doi.org/10.37307/b.978-3-503-21135-7 in-plane dimensions of the plates are infinite, what matters is the finite plate thickness. Sects. 5.2 and 5.7 are on antiplane problems of polarized ceramics for which the notation in Sect. 2.9 is followed. The solutions in Sects. 5.1, 5.2, 5.3, 5.4, 5.5, 5.6, and 5.7 are exact. Those in Sects. 5.8, 5.9, and 5.10 are approximate.作者: 言外之意 時(shí)間: 2025-3-26 10:02
Die friedliche Anwendung der AtomenergieChap. .. These include the effects of heat conduction; mechanical and electrical dissipations due to viscosity, dielectric loss and semiconduction; nonlocal and gradients effects; as well as electromagnetic effects.作者: 樂器演奏者 時(shí)間: 2025-3-26 15:55 作者: insomnia 時(shí)間: 2025-3-26 20:04 作者: 搖曳的微光 時(shí)間: 2025-3-27 00:45
Studien Deutsch als Fremd- und Zweitspracheto biasing fields, characterization of nonlinear electroelastic materials by propagation of small-amplitude waves in electroelastic bodies under biasing fields, and electrostrictive ceramics which operate under a biasing electric field. This chapter presents the linear theory for small fields superp作者: BATE 時(shí)間: 2025-3-27 02:11 作者: harmony 時(shí)間: 2025-3-27 07:33 作者: Aggrandize 時(shí)間: 2025-3-27 10:37 作者: 熱烈的歡迎 時(shí)間: 2025-3-27 16:23 作者: Inveterate 時(shí)間: 2025-3-27 21:36 作者: 反感 時(shí)間: 2025-3-28 01:15 作者: 先行 時(shí)間: 2025-3-28 02:28
Other Effects,Chap. .. These include the effects of heat conduction; mechanical and electrical dissipations due to viscosity, dielectric loss and semiconduction; nonlocal and gradients effects; as well as electromagnetic effects.作者: CURB 時(shí)間: 2025-3-28 08:26
Piezoelectric Devices,ricity. In particular, Sect. 8.2 is an antiplane problem for which the notation of Section 2.9 is followed. Sections 8.4 and 8.5 employ approximate one-dimensional equations for thin rods. Sections 8.6 and 8.7 are on elastic rods and beams with piezoelectric elements in extension and bending, respec作者: 大洪水 時(shí)間: 2025-3-28 11:38
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