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Fig. 11 a Galvanostatic charge and discharge curves and b variation in discharge capacity of
NaNi 0.5 Mn 0.5 O 2 in Na cells at 4.8 mA g -1
[ 21 ]
Fig. 12 a voltage profiles (first and fifth charge/discharge cycle; open circles and diamonds) for
Na/Na 0.85 Li 0.17 Ni 0.21 Mn 0.64 O 2 cell between 4.2 and 2.0 V. Additional discharge voltage profiles
for high-rate studies are also shown and labeled in the legend. The trickle charge data points have
been removed for clarity, and b capacity versus cycle number for Na/Na 0.85 Li 0.17 Ni 0.21 Mn 0.64 O 2
cell between 4.2 and 2.0 V [ 23 ]
Recently, Komaba et al. used Fe to substitute Ni in Na 0.67 Ni 0.5 Mn 0.5 O 2 to
obtain P2-Na 0.67 Fe 0.5 Mn 0.5 O 2 [ 24 ]. This material achieved a reversible capacity of
190 mAh g -1 with an average voltage of 2.75 V (Fig. 13 ). Hence, the energy
density was estimated to be 520 Wh kg -1 , which is comparable to that of LiFePO 4
(about 530 Wh kg -1 ) and slightly higher than that of LiMn 2 O 4 (about
450 Wh kg -1 )[ 24 ]. If assembled with hard carbon (250-300 mAh g -1 ) or alloy
Sn/Sb (300-500 mAh g -1 ) anode, the energy density of the system would be
hopefully close to that of LiFePO 4 /C battery, even higher than that of LiMn 2 O 4 /C
battery. Besides, this material has the advantage of elemental abundance.
3.2 Polyanion-Based Cathode Materials
Over the last decade, polyanion compounds have attracted much attention as the
cathode materials for Li-ion battery, due to their highly thermal and structural
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