Semco university – All about the Lithium-Ion Batteries

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Volume expansion in shelving stage – Semco University

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Introduction

Lithium-ion batteries are accompanied by volume expansion, including structural expansion and gas production expansion, during the process of formation, cycling, storage, and overcharging. The charge-discharge rate determines the rate of the lithium-deintercalation reaction of the battery cell, and it is also accompanied by different degrees of heat generation or lithium evolution. When researchers study the electrical properties of the battery cell, they usually add a certain amount of time at the end of charging or discharging. The shelving stabilizes the cell state and eliminates thermal effects or polarization. How does the volume of the cell change during the shelving stage? In this paper, the in-situ monitoring of the volume expansion of the pouch cells of the LCO/Graphite system after different magnifications was carried out to explore the effect of magnification on the expansion.

Figure 1. Various factors that affect the fast charging of lithium-ion batteries

Experimental Test Information

Test equipment: Gas production volume monitor, model GVM2200 can adjust the temperature from 20°C to 80°C, as shown in Figure 2.

Figure 2. Gas Production Volume Monitor

Test parameters: cell information is shown in Table 1.

Cell information
SystemLco/graphite
Capacity2000mah
Voltage2.8-4.35v
ModelSoft case – 345877
Table 1. Cell Information
Experimental Parameters:

Set up four experimental groups according to the parameters in Table 2 below. After each charge and discharge, leave the battery for 1hour, then place the battery in the in-situ gas production volume monitor, and adjust the oil bath temperature to 25℃. And real-time monitoring of cell volume changes.

 1st cycle2nd cycle3rd cycle4th cycle
CC1.0-4.35V
CVNone0.1C0.05C0.025C
Rest60 min
DC1.0C1.0C0.5C0.25C
Rest60 min
Table 2. Charge and discharge parameters

Analysis of Experimental Results

In-situ monitoring of the cell volume expansion curve in the whole process the charge-discharge curves and volume change curves of the four cycles are shown in Fig. 3. Constant current charging stage: As the SOC continues to increase, the volume continues to expand, which is mainly related to the structural expansion caused by the continuous insertion of lithium ions into the graphite. After entering the constant voltage and shelving stage, the volume of the cell begins to shrink and gradually stabilizes. In the constant current discharge stage: as the DOD gradually increases, the volume of the cell shrinks continuously. When the discharge rate gradually becomes smaller, the abnormal volume expansion of the cell at the initial stage of discharge also gradually decreases. In the shelving stage after discharge, the volume of the cell continues to decrease and tends to be stable over time. Next, we perform a detailed analysis of the shelving phases A and B after charging and discharging.

Figure 3. Different charging and discharging current and volume change curves of cells.

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Volume Expansion Analysis During Charging and Resting

Select the resting part A after charging for each circle in Figure 3 for analysis, as shown in Figure 4. Since the cut-off current of each cycle of charging gradually decreases, from the volume curve of shelving, when there is no CV in the first cycle, the cut-off current of charging is 1C, and the volume at this time gradually decreases with the shelving time, and after about 1500 s constant. The constant voltage stage is added in the last three laps. When the charge cut-off current is less than 0.1C, the volume shrinkage appears at the position where the constant voltage starts. When the battery is put on hold after charging, the volume basically does not change. This shows that the volume shrinkage is related to the current reduction. When there is a constant voltage, the current reduction will be accompanied by the volume shrinkage. This is probably because the internal polarization of the battery decreases during the constant voltage stage, and the difference in lithium concentration in the electrode thickness direction decreases. The reduction of stress and strain caused by concentration difference If there is no constant voltage stage, at the end of charging, the internal polarization of the battery is very large, and the difference in lithium concentration is also very large.

Figure 4

Effect of Charge Cut-off Current on Shelving Volume

In order to further explain the lithium-ion transport process and the evolution process of the state of charge in the battery during the constant current-constant voltage charging process, the mechanical – electrochemical model was used to study the lithium concentration, stress and strain distribution during the charging process.

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Constant Current Charging Stage

During the constant current charging stage, lithium ions are continuously interrelated between the graphite layers, resulting in structural expansion. As the SOC continues to increase, the volume continues to expand.

When the constant current charging is completed, the lithium-ion concentration in the electrolyte, the lithium concentration in the negative electrode particles, the strain and the stress are shown in Figure 5. It can be seen from Fig.5(a) that the closer to the cathode current collector, the higher the lithium-ion concentration in the electrolyte. This is because the cathode/anode particles near the separator are preferentially de-lithiated/lithiated. At the end of constant current charging, the degree of de-lithiation/lithiation of the particles near the separator is greater than that of the particles near the current collector. From Figure5(b), it can be seen that the lithium concentration in the anode particles close to the separator is higher. This is because the lithium diffusion distance of the electrolyte in the anode region far from the separator is longer than that of the anode particles close to the separator, so that the lithium ions reaching the anode are preferentially inserted into the particles close to the separator. In the anode particles near the separator, the solid-phase lithium concentration is higher, so their strain is higher, as shown in Fig. 5(c). At the same time, the strain is larger at the free surface of the particles, but smaller at the contact surfaces between particles and between particles and boundaries. This is because the intercalation of lithium ions causes the volume expansion of the particles. The free surface of the particle expands outward, resulting in greater deformation. But under the constraints of adjacent particles and boundaries, the deformation on the contact surface is small. Figure 5(d) shows that the stress distribution is opposite to the strain distribution. This is because the free surfaces of the particles are not constrained and therefore less stressed. But the contact surface is strongly constrained, so the stress is higher. The greatest stress is in the particles close to the diaphragm. The average strain (meaning the average value of the whole particle in the electrode) and the average stress of the negative electrode particles during constant current charging are shown in FIG. 6. Both of them gradually increased with time, and their changing trends were basically consistent with the relationship shown in Figure 3. After the CC charging is completed, the mean strain and mean stress reach their maximum values, respectively.

Figure 5. Lithium-ion concentration in electrolyte (a), graphite particle solid phase lithium concentration (b), graphite particle strain (c), graphite particle stress (d) distribution at the end of 1C CC charging
Figure 6. Average strain and average stress of anode particles during 1C CC charging

Volume Expansion Analysis in Discharge and Shelving Stages

The resting part B after the discharge of each circle in Fig.3 is selected for analysis, as shown in Fig.9. From the volume curve of shelving, as the discharge rate decreases, the amount of volume change during shelving also decreases gradually, and the time for volume stabilization is gradually shortened. The phenomenon of volume shrinkage in the shelving phase after discharge is similar to that in the shelving phase after charging, both of which are related to the polarization inside the cell and the uneven distribution of lithium concentration. The volume change curves corresponding to different discharge rates are analysed. As shown in Figure 10, in the early stage of discharge, the volume of the cells all show abnormal expansion, and as the discharge rate decreases, the expansion also gradually decreases, which is likely to be related to the internal thermal effect of the cell caused by the large magnification is also related.

Figure 7. Effect of Discharge Current on Shelf Volume
Figure 8. Effect of Discharge Current on Total Volume and Bounce Volume

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According to the simulation results of the constant current and constant voltage charging process, during the constant current discharge process, as the discharge process continues, lithium is deintercalated from the negative electrode particles, but intercalated into the positive electrode particles. At the same time, the electrochemical potential drives the movement of lithium in the electrolyte from the negative electrode to the positive electrode. The lithium concentration in the negative electrode particles decreased, but the lithium concentration in the positive electrode particles increased. In the direction of electrode thickness, there is also the problem of uneven distribution of lithium concentration, and this difference in lithium concentration is related to the thickness and magnification of the electrode. As shown in FIG. 11, at the end of the discharge, the electrode thickness is relatively small or the magnification is relatively small, and the lithium concentration distribution is relatively uniform. However, when the electrode thickness or the magnification increases, there is a clear concentration difference. For the positive electrode, the particulate lithium concentration near the separator is high, and the particulate lithium concentration near the current collector is low. Therefore, as the discharge rate decreases, the difference in lithium concentration inside the battery becomes smaller, and the stress and strain caused by the difference in concentration become smaller. The amount of volume change at the time of shelving is also gradually reduced, and the time for volume stabilization is gradually shortened.

Figure 9. Concentration distribution of particulate solid phase lithium at the end of discharge
Conclusion

In this Article, an in-situ gas production volume monitor (GVM2200) was used to monitor the volume expansion behavior of LCO/Graphite system cells at different rates. It is related to the uneven distribution of the lithium concentration in the discharge polarization, and it may also be related to the thermal effect of the cell caused by the current. Therefore, setting an appropriate charge cut-off current can effectively eliminate the influence of uneven distribution of lithium concentration inside the cell on volume expansion. However, since the current during the discharge process is generally large, it is necessary to increase the shelving time after the discharge to stabilize the cell state.

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