Thermal-Driven Dynamic Shape Change of Bimetallic Nanoparticles Extends Hot Electron Lifetime of Pt/MoS2 Catalysts

Author(s):  
Xiaoli Wang ◽  
Run Long
Author(s):  
Amit Maha ◽  
Su-Seng Pang

A thin composite curved beam under external loading is used to simulate different structures such as pressurized pipes, O-Rings etc. These products can undergo dynamic shape change and warping. A piezoelectric actuator is to be used to design for thin curved structures. Simple thin quarter circular beam geometry is analyzed with external loading at the free end. The orientation and placement of the piezoelectric material on a composite curved beam directly affects the deflection and stress applied to that beam. The optimal placement for an actuator for shape recovery was estimated.


2020 ◽  
Vol 7 (1) ◽  
pp. 1-2
Author(s):  
Maedeh Ganji ◽  
◽  
Jose Ruiz ◽  
Robert Percy ◽  
Emil Missov ◽  
...  

1989 ◽  
Vol 146 ◽  
Author(s):  
Peter J. Wright ◽  
Ahmad Kermani ◽  
Krishna C. Saraswat

ABSTRACTA new technique of post-oxidation annealing has been introduced to improve the properties and long term reliability of ultrathin (<100 Å) MOS gate dielectrics. In this technique, after oxidation, nitridation is done in NH3 followed by a light reoxidation in O2 and then an inert anneal in Ar or N2. Using this technique both optimum performance as well as reliability can be obtained without sacrificing either. NH3 anneal of SiO2 improved the hot electron immunity, but degraded the interface quality. Good properties could be obtained by a strong reoxidation of the nitrided films, however, at the expense of a substantial increase in the film thickness. Nitrogen and argon ambients were found to be equally effective at improving film properties. By annealing the film in an inert ambient following reoxidation of the nitroxide, fixed charge can be further decreased with little oxide grown, electron mobility in NMOS FETs increases further, and the hot electron lifetime is much longer than that of the starting oxide.


AIAA Journal ◽  
2018 ◽  
Vol 56 (9) ◽  
pp. 3745-3756
Author(s):  
Joseph P. Calogero ◽  
Mary I. Frecker ◽  
Zohaib Hasnain ◽  
James E. Hubbard

2015 ◽  
Vol 15 (14) ◽  
pp. 7819-7829 ◽  
Author(s):  
Y. Zhang ◽  
M. S. Sanchez ◽  
C. Douet ◽  
Y. Wang ◽  
A. P. Bateman ◽  
...  

Abstract. The change in shape of atmospherically relevant organic particles is used to estimate the viscosity of the particle material without the need for removal from aerosol suspension. The dynamic shape factors χ of particles produced by α-pinene ozonolysis in a flow tube reactor, under conditions of particle coagulation, were measured while altering the relative humidity (RH) downstream of the flow tube. As relative humidity was increased, the results showed that χ could change from 1.27 to 1.02, corresponding to a transition from aspherical to nearly spherical shapes. The shape change could occur at elevated RH because the organic material had decreased viscosity and was therefore able to flow to form spherical shapes, as favored by the minimization of surface area. Numerical modeling was used to estimate the particle viscosity associated with this flow. Based on particle diameter and RH exposure time, the viscosity dropped from 10(8.7±2.0) to 10(7.0±2.0) Pa s (two sigma) for an increase in RH from < 5 to 58 % at 293 K. These results imply that the equilibration of the chemical composition of the particle phase with the gas phase can shift from hours at mid-range RH to days at low RH.


2012 ◽  
Vol 196 (1) ◽  
pp. 103-114 ◽  
Author(s):  
Julia K. Gilden ◽  
Sebastian Peck ◽  
Yi-Chun M. Chen ◽  
Matthew F. Krummel

Increasing evidence supports a critical role for the septin cytoskeleton at the plasma membrane during physiological processes including motility, formation of dendritic spines or cilia, and phagocytosis. We sought to determine how septins regulate the plasma membrane, focusing on this cytoskeletal element’s role during effective amoeboid motility. Surprisingly, septins play a reactive rather than proactive role, as demonstrated during the response to increasing hydrostatic pressure and subsequent regulatory volume decrease. In these settings, septins were required for rapid cortical contraction, and SEPT6-GFP was recruited into filaments and circular patches during global cortical contraction and also specifically during actin filament depletion. Recruitment of septins was also evident during excessive blebbing initiated by blocking membrane trafficking with a dynamin inhibitor, providing further evidence that septins are recruited to facilitate retraction of membranes during dynamic shape change. This function of septins in assembling on an unstable cortex and retracting aberrantly protruding membranes explains the excessive blebbing and protrusion observed in septin-deficient T cells.


2018 ◽  
Vol 9 (1) ◽  
Author(s):  
Hyosun Lee ◽  
Juhyung Lim ◽  
Changhwan Lee ◽  
Seoin Back ◽  
Kwangjin An ◽  
...  

2014 ◽  
Vol 1843 (6) ◽  
pp. 1182-1187 ◽  
Author(s):  
Kimberley J. Lewis ◽  
Benjamin Masterman ◽  
Iraj Laffafian ◽  
Sharon Dewitt ◽  
Jennie S. Campbell ◽  
...  

2016 ◽  
Vol 810 ◽  
pp. 155-174 ◽  
Author(s):  
S. C. Steele ◽  
G. D. Weymouth ◽  
M. S. Triantafyllou

Dynamic shape change of the octopus mantle during fast jet escape manoeuvres results in added mass energy recovery to the energetic advantage of the octopus, giving escape thrust and speed additional to that due to jetting alone. We show through numerical simulations and experimental validation of overall wake behaviour, that the success of the energy recovery is highly dependent on shrinking speed and Reynolds number, with secondary dependence on shape considerations and shrinking amplitude. The added mass energy recovery ratio $\unicode[STIX]{x1D702}_{ma}$, which measures momentum recovery in relation to the maximum momentum recovery possible in an ideal flow, increases with increasing the non-dimensional shrinking parameter $\unicode[STIX]{x1D70E}^{\ast }={\dot{a}}_{max}/U\sqrt{\mathit{Re }_{0}}$, where ${\dot{a}}_{max}$ is the maximum shrinking speed, $U$ is the characteristic flow velocity and $\sqrt{\mathit{Re }_{0}}$ is the Reynolds number at the beginning of the shrinking motion. An estimated threshold $\unicode[STIX]{x1D70E}^{\ast }\approx 10$ determines whether or not enough energy is recovered to the body to produce net thrust. Since there is a region of high transition for $10<\unicode[STIX]{x1D70E}^{\ast }<30$ where the recovery performance varies widely and for $\unicode[STIX]{x1D70E}^{\ast }>100$ added mass energy is recovered at diminishing returns, we propose a design criterion for shrinking bodies to be in the range of $50<\unicode[STIX]{x1D70E}^{\ast }<100$, resulting in 61–82 % energy recovery.


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