Ponce Victor, Galvez-Aranda Diego E, Seminario Jorge M
Department of Chemical Engineering, Texas A&M University, College Station, TX 77843, USA.
Phys Chem Chem Phys. 2021 Jan 6;23(1):597-606. doi: 10.1039/d0cp02851g.
Present Li-ion battery (LIB) technology requires strong improvements in performance, energy capacity, charging-time, and cost to expand their application to e-mobility and grid storage. Li-metal is one of the most promising materials to replace commercial anodes such as graphite because of its 10 times higher specific capacity. However, Li-metal has high reactivity with commercial liquid electrolytes; thus, new solid materials are proposed to replace liquid electrolytes when Li-metal anodes are used. We present a theoretical analysis of the charging process in a full nanobattery, containing a LiCoO2 cathode, a Li7P2S8I solid-state electrolyte (SSE), a Li-metal anode as well as Al and Cu collectors for the cathode and anode, respectively. In addition, we added a Li3P/Li2S film as a solid electrolyte interphase (SEI) layer between the Li-anode and SSE. Thus, we focus this study on the SEI and SSE. We simulated the charging of the nanobattery with an external voltage by applying an electric field. We estimated temperature profiles within the nanobattery and analyzed Li-ion transport through the SSE and SEI. We observed a slight temperature rise at the SEI due to reactions forming PS3- and P2S74- fragments at the interfaces; however, this temperature profile changes due to the charging current under the presence of the external electric field ε = 0.75 V Å-1. Without the external field, the calculated open-circuit voltage (OCV) was 3.86 V for the battery, which is within the range of values of commercial cobalt-based LIBs. This voltage implies a spontaneous fall of available Li-ions from the anode to the cathode (during discharge). The charge of this nanobattery requires overcoming the OCV plus an additional voltage that determines the charging current. Thus, we applied an external potential able to neutralize the OCV, plus an additional 1.6 V to induce the transport of Li+ from the cathode up to the anode. Several interesting details about Li+ transport paths through the SSE and SEI are discussed.
目前的锂离子电池(LIB)技术需要在性能、能量容量、充电时间和成本方面有显著改进,以将其应用扩展到电动汽车和电网储能领域。锂金属因其比容量高10倍,是替代石墨等商用负极最有前景的材料之一。然而,锂金属与商用液体电解质的反应活性很高;因此,当使用锂金属负极时,人们提出了新的固体材料来替代液体电解质。我们对一个全纳米电池的充电过程进行了理论分析,该电池包含LiCoO₂ 正极、Li₇P₂S₈I 固态电解质(SSE)、锂金属负极以及分别用于正极和负极的铝和铜集流体。此外,我们在锂负极和SSE之间添加了一层Li₃P/Li₂S薄膜作为固体电解质界面(SEI)层。因此,我们将这项研究聚焦于SEI和SSE。我们通过施加电场,用外部电压模拟了纳米电池的充电过程。我们估计了纳米电池内部的温度分布,并分析了锂离子通过SSE和SEI的传输情况。我们观察到由于在界面处形成PS₃⁻和P₂S₇⁴⁻碎片的反应,SEI处有轻微的温度升高;然而,在外部电场ε = 0.75 V Å⁻¹存在的情况下,这种温度分布会因充电电流而改变。在没有外部电场的情况下,计算得出该电池的开路电压(OCV)为3.86 V,这在商用钴基LIBs的值范围内。这个电压意味着在放电过程中,可用锂离子从负极自发地流向正极。对这个纳米电池进行充电需要克服OCV加上一个决定充电电流的额外电压。因此,我们施加了一个能够抵消OCV的外部电势,再加上额外的1.6 V以诱导Li⁺从正极传输到负极。文中讨论了关于Li⁺通过SSE和SEI的传输路径的几个有趣细节。