V. Focused Fundamental Research - EERE - U.S. Department of ...
V. Focused Fundamental Research - EERE - U.S. Department of ...
V. Focused Fundamental Research - EERE - U.S. Department of ...
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Zhang, Liu – PNNL<br />
V.B.10 Development <strong>of</strong> High Energy Cathode (PNNL)<br />
LiMnPO 4 can be tuned simply by adjusting the Li content<br />
in the synthesis step, which provides important clues on<br />
the activation and stabilization <strong>of</strong> phosphate-based cathode<br />
materials.<br />
Figure V - 52: Rietveld refinement <strong>of</strong> XRD data <strong>of</strong> the LixMnPO4 series. Refinements for x = 0.8 and 1.1 compositions are done using two phases, LiMnPO4<br />
and Mn2P2O7. Mn2P2O7 peaks are marked with blue arrows. Green arrows indicate small impurity peaks <strong>of</strong> Li3PO4. Red arrows indicate unidentified impurities<br />
in Li0.5MnPO4.<br />
C/20 <br />
Figure V - 53: Cycling stability <strong>of</strong> LixMnPO4 (0.5≤ x ≤1.2) between 2.0 and<br />
4.5 V at C/20 rate. (1C=150 mA/g).<br />
Synthesis <strong>of</strong> High-Voltage Spinel LiNi 0.5 Mn 1.5 O 4 .<br />
We have developed a novel synthesis approach for<br />
preparing high-voltage spinel LiNi 0.5 Mn 1.5 O 4 and its Crsubstituted<br />
phase that involves only milling and heating.<br />
Both LiNi 0.5 Mn 1.5 O 4 and LiNi 0.45 Cr 0.05 Mn 1.5 O 4 have cubic<br />
structures that can be indexed into the Fd-3m space group.<br />
For the undoped spinel, a trace amount <strong>of</strong> Li x Ni 1-y O was<br />
identified. After 5% substitution <strong>of</strong> Ni by Cr in<br />
LiNi 0.5 Mn 1.5 O 4 , no Li x Ni 1-y O impurity was observed in the<br />
XRD pattern, which indicated a pure spinel phase.<br />
Rietveld refinements showed an increase <strong>of</strong> the lattice<br />
parameter from a = 8.17396(8) Å in LiNi 0.5 Mn 1.5 O 4 to<br />
8.1860(1) Å after Cr-doping, which suggests an increased<br />
amount <strong>of</strong> the disordered phase.<br />
Figure V - 54 compares the morphologies <strong>of</strong> the pure and<br />
Cr-substituted spinels. LiNi 0.5 Mn 1.5 O 4 exhibits a uniform<br />
particle size distribution as shown in Figure V - 54a. The<br />
octahedral particle diameters were around 2 μm and further<br />
aggregated into secondary particles. After Cr-doping, the<br />
morphology <strong>of</strong> the spinel did not change much. However,<br />
the octahedral shape <strong>of</strong> the spinel particles became more<br />
distinct as shown in Figure V - 54d. LiNi 0.5 Mn 1.5 O 4 consists<br />
<strong>of</strong> both ordered and disordered phases as revealed by Figure<br />
V - 54b and Figure V - 54c. The highlighted reflections are<br />
forbidden by the Fd-3m space group. The occurrence <strong>of</strong><br />
the super lattice pattern was caused by the ordering<br />
between Ni 2+ and Mn 4+ , which indicates the coexistence <strong>of</strong><br />
an ordered phase in the undoped spinel that cannot be<br />
directly observed from XRD pattern. However, after Crdoping,<br />
the extra diffraction spots were no longer<br />
observable in Figure V - 54e and Figure V - 54f, both <strong>of</strong> which<br />
showed typical spinel patterns. In other words, Cr-doping<br />
FY 2011 Annual Progress Report 515 Energy Storage R&D