scholarly journals Synthesis and electrochemical performance of aluminum antimonide alloy anode prepared by melt spinning

2014 ◽  
Author(s):  
Daniel Julian Kharistal
2011 ◽  
Vol 158 (12) ◽  
pp. A1404 ◽  
Author(s):  
Yanyi Wang ◽  
Peixin Zhang ◽  
Xiangzhong Ren ◽  
Guobin Yi

2017 ◽  
Vol 42 (16) ◽  
pp. 11654-11661 ◽  
Author(s):  
Ma Jingling ◽  
Ren Fengzhang ◽  
Wang Guangxin ◽  
Xiong Yi ◽  
Li Yaqiong ◽  
...  

RSC Advances ◽  
2021 ◽  
Vol 11 (43) ◽  
pp. 26586-26593
Author(s):  
Edna Mados ◽  
Nimrod Harpak ◽  
George Levi ◽  
Fernando Patolsky ◽  
Emanuel Peled ◽  
...  

Electroless coating of a silicon nanowires (SiNW) anode (a) followed by annealing, forms nickel silicide layer (b), which enables stable electrochemical behaviour of SiNi-alloy anode and higher capacity retention compared to the pristine SiNW anode (c).


2009 ◽  
Vol 484 (1-2) ◽  
pp. 864-869 ◽  
Author(s):  
Mengwei Wang ◽  
Hailei Zhao ◽  
Jianchao He ◽  
Ronglin Wang ◽  
Jingbo Chen ◽  
...  

Author(s):  
Raja K. Mishra

The discovery of a new class of permanent magnets based on Nd2Fe14B phase in the last decade has led to intense research and development efforts aimed at commercial exploitation of the new alloy. The material can be prepared either by rapid solidification or by powder metallurgy techniques and the resulting microstructures are very different. This paper details the microstructure of Nd-Fe-B magnets produced by melt-spinning.In melt spinning, quench rate can be varied easily by changing the rate of rotation of the quench wheel. There is an optimum quench rate when the material shows maximum magnetic hardening. For faster or slower quench rates, both coercivity and maximum energy product of the material fall off. These results can be directly related to the changes in the microstructure of the melt-spun ribbon as a function of quench rate. Figure 1 shows the microstructure of (a) an overquenched and (b) an optimally quenched ribbon. In Fig. 1(a), the material is nearly amorphous, with small nuclei of Nd2Fe14B grains visible and in Fig. 1(b) the microstructure consists of equiaxed Nd2Fe14B grains surrounded by a thin noncrystalline Nd-rich phase. Fig. 1(c) shows an annular dark field image of the intergranular phase. Nd enrichment in this phase is shown in the EDX spectra in Fig. 2.


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