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  • 2010-2014  (3)
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  • 2010-2014  (3)
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  • 1
    Online Resource
    Online Resource
    AICIT ; 2013
    In:  International Journal of Digital Content Technology and its Applications Vol. 7, No. 8 ( 2013-4-30), p. 598-606
    In: International Journal of Digital Content Technology and its Applications, AICIT, Vol. 7, No. 8 ( 2013-4-30), p. 598-606
    Type of Medium: Online Resource
    ISSN: 1975-9339 , 2233-9310
    URL: Issue
    Language: Unknown
    Publisher: AICIT
    Publication Date: 2013
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  • 2
    Online Resource
    Online Resource
    The Electrochemical Society ; 2014
    In:  ECS Meeting Abstracts Vol. MA2014-04, No. 2 ( 2014-06-10), p. 421-421
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2014-04, No. 2 ( 2014-06-10), p. 421-421
    Abstract: Introduction Lithium rich layered material has attracted much attention because of its high capacity, however, the low effciency in the 1st cycle and poor rate property is a big issue for its practical use. We adopted a (NH 4 ) 2 S 2 O 8 treatment on Li 1.2 Ni 0.16 Co 0.08 Mn 0.56 O 2 material, the prodcut showed a greatly increased 1 st cycle efficinecy of above 90% and a capacity as high as 200mAh. g -1 at 4C rate. Experiment Li 1.2 Ni 0.16 Co 0.08 Mn 0.56 O 2 was prepared by a rheological method. Stoichiometric amount of Li 2 CO 3 , Ni(CH 3 COO) 2 ·4H 2 O, Co(CH 3 COO) 2 ·4H 2 O, Mn(CH 3 COO) 2 ·4H 2 O and oxalic acid were mixed. And then a proper amount of water was added. After stirring the mixture at 80-90 ºC for 4 h, it was dried at 120 ºC for 10 h, followed by annealing at 850 ºC for 20 h. (NH 4 ) 2 S 2 O 8 solution with different concerntration was used to treat the above Li 1.2 Ni 0.16 Co 0.08 Mn 0.56 O 2 sample, the product was named as 20%-RL,30%-RL, 40%-RL, 50%-RL according the different concerntration of (NH 4 ) 2 S 2 O 8 solution. Cycling test was conducted to evaluate the cyclcing stability and rate property of the products. The samples were characterized in terms of XRD, SEM, XPS and Raman measurement. Result and discussion The 1 st charge/discharge curves are compared in Fig.1. The pristine Li 1.2 Ni 0.16 Co 0.08 Mn 0.56 O 2 shows an intial caapcity of 224.0 mAh g -1 but with a low efficiency of 79%. With the increasing of the (NH 4 ) 2 S 2 O 8 concerntration, the product shows an increased effciency and reachs 99% in the “40%-RL” sample. Additionally, the (NH 4 ) 2 S 2 O 8 treatment leads to an improvement in the cycling stability. In Fig.2, untreated Li 1.2 Ni 0.16 Co 0.08 Mn 0.56 O 2 maintains 88% capacity in the 100 th cycle, while the “40%-RL” sample shows capacity retention of 97% after 100 cyles. The (NH 4 ) 2 S 2 O 8 -treated samples also present greatly improved rate performance. In Fig.3, the increase of the current rate from 0.1C to 4C causes a capacity decrease from 255mAh.g -1 to 67mAh.g -1 for the pristine Li 1.2 Ni 0.16 Co 0.08 Mn 0.56 O 2 sample. For the (NH 4 ) 2 S 2 O 8 -treated samples, they all exhibit a much better rate property than the untreated phase. Especially for the “30%-RL” and “40%-RL” sample, they both present a capcity above 200mAh.g -1 at the 4C rate. XRD measurements prove that the (NH 4 ) 2 S 2 O 8 -treatment weakens the super lattice in the Lithium rich layered material. ICP and Raman analysis furtheres reveal that the Li content in Li 2 MnO 3 decreased after the (NH 4 ) 2 S 2 O 8 -treatment, which can be the main reason of the efficiency increase in the 1 st cycle.
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2014
    detail.hit.zdb_id: 2438749-6
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  • 3
    Online Resource
    Online Resource
    IOP Publishing ; 2011
    In:  Journal of Physics D: Applied Physics Vol. 44, No. 25 ( 2011-06-29), p. 255201-
    In: Journal of Physics D: Applied Physics, IOP Publishing, Vol. 44, No. 25 ( 2011-06-29), p. 255201-
    Abstract: Simulation methods employing continuity equations to describe particle transportation are used to examine the process of single discharge. However, it is difficult to simulate partial discharge (PD) behaviour accurately by these methods, because it will take too much computation time to simulate consecutive PD sequences. In this report, in order to save computation time, a simple three-dimensional network is used to simulate PD sequences in a small void under ac voltage. The model considers charge generation, charge transport and charge disappearance, and electrical field redistribution in three dimensions. The continuity equations for electrons, positive ions and negative ions, including the effects of ionization, attachment, recombination, electron diffusion and the transport of charge under electrical field are solved simultaneously with Poisson's equation. With this model, the phase-resolved PD pattern and the current forms of each PD are obtained. Moreover, considering the propagation process of each PD and its influence on surface charge distribution, the fall part of PD current form and the effect of previous discharge on the subsequent one are also studied.
    Type of Medium: Online Resource
    ISSN: 0022-3727 , 1361-6463
    Language: Unknown
    Publisher: IOP Publishing
    Publication Date: 2011
    detail.hit.zdb_id: 209221-9
    detail.hit.zdb_id: 1472948-9
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