rough boundaries
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2021 ◽  
Author(s):  
Jiri Vohanka ◽  
Ivan Ohlidal ◽  
Vilma Buršíková ◽  
Petr Klapetek ◽  
Nupinder Jeet Kaur

Author(s):  
Vladimir Khvesyuk ◽  
Aleksandr Barinov ◽  
B. Liu ◽  
W. Qiao

The paper discusses current problems related to the heat transfer in solid-state nanostructures: the influence of real rough boundaries on the effective thermal conductivity and contact thermal resistance


2021 ◽  
Vol 2057 (1) ◽  
pp. 012111
Author(s):  
A A Barinov ◽  
V I Khvesyuk

Abstract Because of the rapid development of semiconductor electronics and the tendency to size reduction of the elements of transistors, there is an urgent task of assessing the heat transfer regime, which determines the ability to maintain the required thermal regime. In this work, the heat transfer in micro- and nanostructures in silicon is considered, and a comprehensive analysis of factors determining the heat transfer regime is carried out. In particular, the effect of the interaction of phonons with the sample boundaries in the quasi-ballistic and ballistic heat transfer regimes, where these processes play a decisive role, is evaluated using statistical model of phonon scattering on rough boundaries of samples.


eLife ◽  
2021 ◽  
Vol 10 ◽  
Author(s):  
Medha Sharma ◽  
Tao Jiang ◽  
Zi Chen Jiang ◽  
Carlos E Moguel-Lehmer ◽  
Tony Harris

Structures and machines require smoothening of raw materials. Self-organized smoothening guides cell and tissue morphogenesis, and is relevant to advanced manufacturing. Across the syncytial Drosophila embryo surface, smooth interfaces form between expanding Arp2/3-based actin caps and surrounding actomyosin networks, demarcating the circumferences of nascent dome-like compartments used for pseudo-cleavage. We found that forming a smooth and circular boundary of the surrounding actomyosin domain requires Arp2/3 in vivo. To dissect the physical basis of this requirement, we reconstituted the interacting networks using node-based models. In simulations of actomyosin networks with local clearances in place of Arp2/3 domains, rough boundaries persisted when myosin contractility was low. With addition of expanding Arp2/3 network domains, myosin domain boundaries failed to smoothen, but accumulated myosin nodes and tension. After incorporating actomyosin mechanosensitivity, Arp2/3 network growth locally induced a surrounding contractile actomyosin ring that smoothened the interface between the cytoskeletal domains, an effect also evident in vivo. In this way, a smooth structure can emerge from the lateral interaction of irregular active materials.


2021 ◽  
Author(s):  
Medha Sharma ◽  
Tao Jiang ◽  
Zi Chen Jiang ◽  
Carlos E. Moguel-Lehmer ◽  
Tony J. C. Harris

AbstractStructures and machines require smoothening of raw materials. Self-organized smoothening guides cell and tissue morphogenesis, and is relevant to advanced manufacturing. Across the syncytial Drosophila embryo surface, smooth interfaces form between expanding Arp2/3-based actin caps and surrounding actomyosin networks, demarcating the circumferences of nascent dome-like compartments used for pseudo-cleavage. We found that smoothening of the actomyosin interfaces requires Arp2/3 in vivo. To dissect the physical basis of this requirement, we reconstituted the interacting networks using node-based models. When actomyosin networks were simulated with clearances instead of Arp2/3 networks, rough boundaries persisted with low levels of myosin contractility. With addition of expanding Arp2/3 networks, network-network interfaces failed to smoothen, but accumulated myosin nodes and tension. After incorporating actomyosin mechanosensitivity, Arp2/3 network growth induced local contractility and smoothening of the interfaces, effects also evident in vivo. In this way, a smooth structure can emerge from the lateral interaction of irregular starting materials.


Author(s):  
Florent Retailleau ◽  
Vadim Allheily ◽  
Lionel Merlat ◽  
Jean-François Henry ◽  
Jaona Harifidy Randrianalisoa

2020 ◽  
Vol 102 (14) ◽  
Author(s):  
N. A. Keepfer ◽  
G. W. Stagg ◽  
L. Galantucci ◽  
C. F. Barenghi ◽  
N. G. Parker

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