By Aurelio L. Araujo, Carlos A. Mota Soares
This paintings used to be compiled with improved and reviewed contributions from the seventh ECCOMAS Thematic convention on shrewdpermanent buildings and fabrics, that was once held from three to six June 2015 at Ponta Delgada, Azores, Portugal. The convention supplied a finished discussion board for discussing the present state-of-the-art within the box in addition to producing idea for destiny rules particularly on a multidisciplinary point.
The scope of the convention integrated subject matters on the topic of the next areas:
Fundamentals of clever fabrics and buildings; Modeling/formulation and characterization of clever actuators, sensors and shrewdpermanent fabric platforms; tendencies and advancements in assorted components equivalent to fabric technological know-how together with composite fabrics, clever hydrogels, interfacial phenomena, part limitations and boundary layers of part obstacles, keep an eye on, micro- and nano-systems, electronics, and so forth. to be thought of for clever platforms; Comparative overview of other clever actuators and sensors; research of structural ideas and designs by way of their adaptability to clever applied sciences; layout and improvement of shrewdpermanent buildings and structures; Biomimetic phenomena and their notion in engineering; Fabrication and trying out of clever buildings and structures; purposes of shrewdpermanent fabrics, buildings and similar know-how; shrewdpermanent robots; Morphing wings and shrewdpermanent aircrafts; man made muscle mass and biomedical functions; shrewdpermanent buildings in mechatronics; and effort harvesting.
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Additional resources for Smart Structures and Materials: Selected Papers from the 7th ECCOMAS Thematic Conference on Smart Structures and Materials
Curr Opin Solid State Mater Sci 1:698–705 4. Kuna M (2010) Fracture mechanics of piezoelectric materials—where are we right now? Eng Fract Mech 77(2):309–326 5. Schneider GA (2007) Inﬂuence of electric ﬁeld and mechanical stresses on the fracture of ferroelectrics. Annu Rev Mater Res 37:491–538 6. Huber Je, Fleck Na, Landis CM, McMeeking RM (1999) A constitutive model for ferroelectric polycrystals. J Mech Phys Solids 47(8):1663–1697 7. Furuta A, Uchino K (1993) Dynamic observation of crack propagation in piezoelectric multilayer actuators.
They can describe shape changes in both SMA phases (martensite or austenite) when subjected to monotonic as well as cyclic loading, including minor loop behaviour. The model is validated by stress-strain experiments and the results show outstanding correlation with experimental data. Since the model is A. Pai (✉) ⋅ I. Koke ⋅ A. de I. de A. de T. Niendorf ⋅ P. Krooss ⋅ M. de P. de M. L. A. 1007/978-3-319-44507-6_3 41 42 A. Pai et al. based on simple closed-form equations, it is extremely computational eﬃcient and can build the foundation for the development of real-time capable SMA models for control algorithms.
19). The calculation of the parabolic coeﬃcient q to represent grain sluggishness then proceeds with the quadratic formula in Eq. 20). k2∗ is subsequently 52 A. Pai et al. (a) (b) Fig. 6 Parameter update for unloading (a) and reloading (b) in austenite calculated with Eq. 21) to ensure a smooth transition between the parabola and the rest of the curve. 21) E3 − E2∗ ∙ ????∗1 : With all the other values, ????∗1 is then calculated with by solving for ????1 in Eq. 7) yielding Eq. 22) where ????2 , ????3 and ????q are calculated with Eqs.
Smart Structures and Materials: Selected Papers from the 7th ECCOMAS Thematic Conference on Smart Structures and Materials by Aurelio L. Araujo, Carlos A. Mota Soares