نتایج جستجو برای: classical lamination theory

تعداد نتایج: 927734  

The hydrogen abstraction reaction of OH radical with CH3CH2OCF2CHF2 (HFE-374pc2) is investigated theoretically by semi-classical transition state theory. The stationary points on the potential energy surface of the reaction are located by using KMLYP density functional method along with 6-311++G(d,p) basis set. Vibrational anharmonicity coefficients, ...

Journal: :physical chemistry research 2014
vahid saheb mohammad solimannejad

the hydrogen abstraction reaction by oh radical from ch2brch2br (r1) and ch₃chbr2 (r2) is investigated theoretically by semi-classical transition state theory. the stationary points for both reactions are located by using ωb97x-d and kmlyp density functional methods along with cc-pvtz basis. single-point energy calculations are performed at the qcisd(t) and ccsd(t) levels of theory with differe...

Journal: :International journal of innovative technology and exploring engineering 2022

Carbon Nanotubes reinforced composite materials are widely used in aerospace engineering due to high strength-to-weight ratios, which can be tailored per requirements. The behaviour of the structures depends on various factors like, Lamination scheme, Ply orientation and loading conditions. In present work, Static deflection stresses analysis a Nano Tube laminated hybrid plate extends First Ord...

Journal: :Journal of The Brazilian Society of Mechanical Sciences and Engineering 2021

Abstract In this work, the bending behavior of nanoplates subjected to both sinusoidal and uniform loads in hygrothermal environment is investigated. The present plate theory based on classical laminated thin with strain gradient effect take into account nonlocality nanostructures. equilibrium equations have been carried out by using principle virtual works a system partial differential sixth o...

Journal: :Composites Science and Technology 2022

The comprehensive design feasibility for woven composites has been established by identifying the missing component in tool these materials, so-called controllable parameters. These are parameters that involved, directly or indirectly, manufacturing of preforms, and they include tow densities, number size filaments a intra-tow fibre volume fractions. Controllable have related through simple pro...

2015
Anupama Sathyamurthy Dong-Min Yin Arnab Barik Chengyong Shen Jonathan C. Bean Dwight Figueiredo Jin-Xiong She Wen-Cheng Xiong

Cortical lamination is crucial for the assembly of cerebellar circuitry. In this process, granule neurons (GNs) migrate along Bergmann glia (BG), which are specialized astroglial cells, from the external granule layer to the internal granule layer. However, the molecular mechanisms underlying BG development are not well understood. Here, we show that GFAP::Cre;Erbb3 mice, which lack Erbb3 in bo...

2015
Anupama Sathyamurthy Dong-Min Yin Arnab Barik Chengyong Shen Jonathan C. Bean Dwight Figueiredo Jin-Xiong She Wen-Cheng Xiong

Cortical lamination is crucial for the assembly of cerebellar circuitry. In this process, granule neurons (GNs) migrate along Bergmann glia (BG), which are specialized astroglial cells, from the external granule layer to the internal granule layer. However, the molecular mechanisms underlying BG development are not well understood. Here, we show that GFAP::Cre;Erbb3 mice, which lack Erbb3 in bo...

2010

a) Energy-momentum Based on Noether’s theorem, construct the energy-momentum tensor for classical electromagnetism from the above Lagrangian. Note that the usual procedure does not result in a symmetric tensor. To remedy that, we can add to T μν a term of the form ∂λK λμν , where K is antisymmetric in its first two indices. Such an object is automatically divergenceless, so T̂ μν = T μν + ∂λK λμ...

2011
JOSEPH G. CONLON

where g : R × R × R → R is a C function. Once we specify a parameter path u(t), t ≥ t1, in the parameter space we can solve (1.1) uniquely for x(t), t ≥ t1, with the given initial condition x(t1) = x0. Alternatively if we specify a parameter path u(t), t ≤ t1, in the parameter space we can solve (1.1) uniquely for x(t), t ≤ t1, with the given terminal condition x(t1) = x0. Suppose now that for ...

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