Why my cells degrade with cycling?
As positive lithium ions move out of the cathode during a charge cycle, its crystal lattice usually expands because of repulsion between the negative oxygen ions. In some materials (such as NCM811), high-voltage cycling may also cause transformation to another crystal phase and in turn, abrupt lattice expansion. This can then cause particle cracking and, eventually, loss of capacity in the battery cell.
Likewise, when lithium ions enter the anode during charging, it also causes expansion of the lattice. In the case of graphite anodes, the lattice structure changes to LiC12 and then to LiC6. During discharge, it reverses back to graphite (C). After a few charge-discharge cycles, some lithium ions may be retained in the anode, causing a reduction in discharge capacity. In the case of alternative anode materials like silicon, which have a much larger initial capacity, the lattice expansion may be so large that particle cracking happens rapidly.
In operando XRD can investigate the crystalline structure of electrode materials at atomic scale, and how it changes as the cell is charged or discharged. For any new battery material development, in operando XRD therefore provides a straightforward way of determining the electrode materials’ stability with cycling.
Our Empyrean XRD platform enables battery manufacturers and developers to investigate coin, electrochemical, pouch, and prismatic cells with in situ charge-discharge cycling.
Example of in operando cycling of NCM333 and graphite anode cells. The green line in Fig. 1(a) shows the cell’s voltage variation, from 3.2 volts in its discharged state to 4.3 volts in its fully charged state. The peak around 6.8°2θ is 003 peak of the NCM cathode, and its changing position reflects changes in the C-parameter with cycling. The discontinuous peak around 9°2θ is from the graphite anode, which changes from graphite to LiC12 and then to LiC6 during the charge cycle, and then reverses back to LiC12 and then graphite during the discharge cycle. Fig. 1(b) shows the change in c-parameter during cycling – from 14.47 in a fully charged state to 14.14 in a discharged state.
Coin and electrochemical cells
All types of coin cells that have at least one side with an X-ray transparent window can be studied on the Empyrean XRD. We provide a specialized coin cell holder, which can be used for charge-discharge cycling.
The Empyrean XRD can also support electrochemical cells with an X-ray transparent window, like beryllium or glassy carbon. We can supply these electrochemical cells – with the option of heating and cooling – that can then be mounted on the Empyrean XRD.
Fig. 2(a) An electrochemical cell supported on the Empyrean XRD platform. The cell can also be heated or cooled to investigate cycling durability at non-ambient temperatures. Fig. 2(b) shows a coin cell holder with electrical connections, for mounting coin cells that have at least one face with an X-ray transparent window.
Pouch and prismatic cells
The Empyrean supports 60 kV excitation, enabling the high-intensity 22.16 keV Ag radiation required for pouch cell research. Indeed, multilayer pouch cells up to 5 mm thick can be analyzed on the Empyrean XRD platform, which is equipped with Ag radiation and a GaliPIX3D Detector. What’s more, special multilayer focusing mirrors deliver high resolution and a high-brilliance X-ray beam, further shortening measurement times.
Fig. 3(a) shows pouch or prismatic cell mounting on the Empyrean XRD. A mechanism to apply pressure on pouch cells is also supported. Fig. 3(b) shows the high-performance GaliPIX3D detector with CdTe sensor, making in operando XRD on thick pouch cells possible.