spatial waves
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2020 ◽  
Vol 14 (6) ◽  
pp. 2070033
Author(s):  
Jun Yan Dai ◽  
Liu Xi Yang ◽  
Jun Chen Ke ◽  
Ming Zheng Chen ◽  
Wankai Tang ◽  
...  

Sensors ◽  
2020 ◽  
Vol 20 (11) ◽  
pp. 3058
Author(s):  
Javier Martinez-Roman ◽  
Ruben Puche-Panadero ◽  
Angel Sapena-Bano ◽  
Manuel Pineda-Sanchez ◽  
Juan Perez-Cruz ◽  
...  

Induction machines (IMs) are critical components of many industrial processes, what justifies the use of condition-based maintenance (CBM) systems for detecting their faults at an early stage, in order to avoid costly breakdowns of production lines. The development of CBM systems for IMs relies on the use of fast models that can accurately simulate the machine in faulty conditions. In particular, IM models must be able to reproduce the characteristic harmonics that the IM faults impress in the spatial waves of the air gap magneto-motive force (MMF), due to the complex interactions between spatial and time harmonics. A common type of fault is the eccentricity of the rotor core, which provokes an unbalanced magnetic pull, and can lead to destructive rotor-stator rub. Models developed using the finite element method (FEM) can achieve the required accuracy, but their high computational costs hinder their use in online CBM systems. Analytical models are much faster, but they need an inductance matrix that takes into account the asymmetries generated by the eccentricity fault. Building the inductance matrix for eccentric IMs using traditional techniques, such as the winding function approach (WFA), is a highly complex task, because these functions depend on the combined effect of the winding layout and of the air gap asymmetry. In this paper, a novel method for the fast and simple computation of the inductance matrix for eccentric IMs is presented, which decouples the influence of the air gap asymmetry and of the winding configuration using two independent tensors. It is based on the construction of a primitive inductance tensor, which formulates the eccentricity fault using single conductors as the simplest reference frame; and a winding tensor that converts it into the inductance matrix of a particular machine, taking into account the configuration of the windings. The proposed approach applies routine procedures from tensor algebra for performing such transformation in a simple way. It is theoretically explained and experimentally validated with a commercial induction motor with a mixed eccentricity fault.


2020 ◽  
Vol 14 (6) ◽  
pp. 1900133 ◽  
Author(s):  
Jun Yan Dai ◽  
Liu Xi Yang ◽  
Jun Chen Ke ◽  
Ming Zheng Chen ◽  
Wankai Tang ◽  
...  

2019 ◽  
pp. 1900478 ◽  
Author(s):  
Meng Wang ◽  
Hui Feng Ma ◽  
Liang Wei Wu ◽  
Shi Sun ◽  
Wen Xuan Tang ◽  
...  

2019 ◽  
Author(s):  
Mark Greenwood ◽  
Mirela Domijan ◽  
Peter D. Gould ◽  
Anthony J.W. Hall ◽  
James C.W. Locke

AbstractEvery plant cell has a genetic circuit, the circadian clock, that times key processes to the day-night cycle. These clocks are aligned to the day-night cycle by multiple environmental signals that vary across the plant. How does the plant integrate clock rhythms, both within and between organs, to ensure coordinated timing? To address this question, we examined the clock at the sub-tissue level across Arabidopsis thaliana seedlings under multiple environmental conditions and genetic backgrounds. Our results show that the clock runs at different speeds (periods) in each organ, which causes the clock to peak at different times across the plant in both constant environmental conditions and light-dark cycles. Closer examination reveals that spatial waves of clock gene expression propagate both within and between organs. Using a combination of modeling and experiment, we reveal that these spatial waves are the result of the period differences between organs and local coupling, rather than long distance signaling. With further experiments we show that the endogenous period differences, and thus the spatial waves, are caused by the organ specificity of inputs into the clock. We demonstrate this by modulating periods using light and metabolic signals, as well as with genetic perturbations. Our results reveal that plant clocks are set locally by organ specific inputs, but coordinated globally via spatial waves of clock gene expression.


2019 ◽  
Vol 36 (2) ◽  
pp. 293 ◽  
Author(s):  
Shahid Iqbal ◽  
Shuo Liu ◽  
Guo Dong Bai ◽  
Muhammad Furqan ◽  
Hamza Ahmad Madni ◽  
...  

eLife ◽  
2018 ◽  
Vol 7 ◽  
Author(s):  
Peter D Gould ◽  
Mirela Domijan ◽  
Mark Greenwood ◽  
Isao T Tokuda ◽  
Hannah Rees ◽  
...  

The Arabidopsis circadian clock orchestrates gene regulation across the day/night cycle. Although a multiple feedback loop circuit has been shown to generate the 24-hr rhythm, it remains unclear how robust the clock is in individual cells, or how clock timing is coordinated across the plant. Here we examine clock activity at the single cell level across Arabidopsis seedlings over several days under constant environmental conditions. Our data reveal robust single cell oscillations, albeit desynchronised. In particular, we observe two waves of clock activity; one going down, and one up the root. We also find evidence of cell-to-cell coupling of the clock, especially in the root tip. A simple model shows that cell-to-cell coupling and our measured period differences between cells can generate the observed waves. Our results reveal the spatial structure of the plant clock and suggest that unlike the centralised mammalian clock, the Arabidopsis clock has multiple coordination points.


2018 ◽  
Author(s):  
Peter D Gould ◽  
Mirela Domijan ◽  
Mark Greenwood ◽  
Isao T Tokuda ◽  
Hannah Rees ◽  
...  

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