Study on Interfacial Stability and Electrochemical Performance of LFP/Graphite Battery Regulated by Mechanical Pressure

Table of Contents

Composite image showing the Nano Materials Science journal article header titled "Pressurized vs. unpressurized LiFePO4 batteries" by Wang, Yan et al., the acknowledgments section thanking IEST Instrument (Initial Energy Science & Technology Co., Ltd) for support, a schematic diagram of the powder resistivity and compaction density measurement setup, and a product photo of the IEST PRCD3100 system

Abstract

A recent study published in Nano Materials Science by researchers at Beijing Institute of Technology systematically investigates how mechanical pressure regulates interfacial stability and failure mechanisms in LFP/graphite battery. Comparing cells cycled at 0 MPa (unpressurized) and 0.1 MPa (pressurized), the study found that moderate pressure reduces capacity fade from 24.31% to just 5.14%. Multi-scale characterization — including in-situ XRD, XPS, TOF-SIMS, and AFM — reveals that 0.1 MPa promotes the formation of a LiF-rich, mechanically robust SEI layer on the graphite anode, suppresses Al current collector corrosion at the cathode, and enhances LiFePO₄/FePO₄ phase transition reversibility. The IEST PRCD3100 powder resistivity and compaction density system was used to characterize electrode powder properties, and IEST Instrument is acknowledged in the study.

📄 Source Paper

Wang Y., Yan K., Dong J., Tang R., Guan Y., Zhao G., Lu Y., Hao J., Li B., Mo S., He X., Li N., Chen L., Wu F., Su Y.


Pressurized vs. unpressurized LiFePO₄ batteries: A comparative study on interfacial stability and electrochemical performance.
Nano Materials Science, 2025.

DOI: 10.1016/j.nanoms.2025.11.020
|  Journal: Nano Materials Science (ScienceDirect / Elsevier)
|  Institutions: Beijing Institute of Technology; BIT Chongqing Innovation Center; State Grid Electric Power Research Institute

✓ IEST Instrument acknowledged — PRCD powder resistivity and compaction density measurement system used in this research

1. Background: Why Mechanical Pressure Matters for LFP/Graphite Battery Cycle Life

LFP/graphite batteries — cells using LiFePO₄ (lithium iron phosphate) cathodes and graphite anodes — dominate commercial electric vehicle and grid energy storage deployments due to their high safety, long cycle life, and cost competitiveness. During real-world operation, these batteries are subject to continuous mechanical pressure arising from three sources: module assembly preloading, housing constraint, and the repeated volumetric expansion and contraction of electrodes during cycling.

Mechanical pressure in battery systems is defined as the compressive stress applied to a cell stack, typically expressed in MPa, that affects electrode particle contact geometry, electrode–electrolyte interfacial stability, lithium-ion transport behavior, and electrode structural evolution over cycling. Prior research has established that moderate external pressure improves electrode contact, reduces interfacial impedance, and stabilizes SEI film formation — but the coupled mechanisms by which pressure simultaneously regulates graphite anode SEI composition, cathode interfacial stability, aluminum current collector corrosion, and LiFePO₄/FePO₄ phase transformation reversibility in a full LFP/graphite cell had not been systematically characterized.

The SEI layer (solid electrolyte interphase) is defined as the passivation film that forms on the graphite anode surface during the first charge cycle from electrolyte reductive decomposition. Its composition — particularly the ratio of inorganic components (LiF, Li₂CO₃) to organic components (ROCO₂Li, ROLi) — determines ionic conductivity, mechanical stability, and the rate of ongoing electrolyte consumption during cycling. A LiF-rich SEI layer is mechanically harder and more ionically selective, providing superior long-term protection compared to organic-dominated SEI layers that are prone to cracking during volume change cycles.

2. Key Findings: Moderate Pressure Slashes Capacity Fade From 24.31% to 5.14%

The research team compared the electrochemical performance of LFP/graphite pouch cells under two conditions: no applied pressure (0 MPa) and moderate applied mechanical pressure (0.1 MPa). After cycling, the cells were analyzed using a comprehensive suite of characterization techniques — in-situ XRD, SEM, AFM, HRTEM, XPS, FTIR, TOF-SIMS, and DCIR measurement — to correlate electrochemical performance with structural and chemical evolution at both electrodes.

Table 1. Performance comparison — pressurized (0.1 MPa) vs. unpressurized (0 MPa) LFP/graphite battery (Wang et al., Nano Materials Science, 2025)
Performance Metric 0 MPa (No Pressure) 0.1 MPa (Moderate Pressure) Improvement
Capacity decay rate 24.31% 5.14% ~5× reduction in capacity fade
DCIR growth rate Faster growth Slower growth Reduced impedance rise = better interfacial stability
Irreversible FePO₄ phase (post-cycling) 34.1% 18.8% 45% reduction in irreversible cathode phase loss
Temperature rise during cycling Higher Lower Reduced Joule heating from lower internal resistance
Graphite anode SEI composition Organic-dominated; non-uniform LiF-rich; uniform; mechanically stable Better SEI quality → suppressed continuous electrolyte decomposition
Al current collector corrosion More severe Reduced Cathode current collector integrity preserved

3. Mechanism 1 — Improved Electrochemical Performance and LFP Phase Transformation Uniformity

Electrochemical characterization confirms that 0.1 MPa mechanical pressure produces a measurable and significant improvement in LFP/graphite battery cycle stability. DCIR (direct current internal resistance) growth is substantially slower under pressure, indicating that interfacial stability is maintained more effectively throughout cycling. Reduced polarization in charge/discharge curves and more sharply defined features in dQ/dV analysis confirm that the electrochemical reaction kinetics are better preserved under pressure.

dQ/dV analysis (differential capacity analysis) — in which the derivative of capacity with respect to voltage is plotted against voltage to reveal phase transformation peaks — shows that the characteristic LiFePO₄ ↔ FePO₄ two-phase transition peaks remain more distinct and better-resolved under 0.1 MPa compared to the unpressurized condition, where peak broadening and shifting indicate progressive kinetic deterioration and reduced phase transformation reversibility.

In-situ XRD measurements during cycling reveal that 0.1 MPa pressure promotes more spatially uniform LiFePO₄/FePO₄ phase transformation — meaning lithium extraction and insertion occur more homogeneously across the cathode electrode rather than concentrating in localized regions. This uniformity directly reduces mechanical stress gradients within the cathode electrode and diminishes the driving force for crack formation and particle fracture. Concurrently, temperature measurements confirm lower thermal accumulation under pressure, consistent with reduced internal resistance and Joule heating.

Electrochemical performance comparison of LFP/graphite battery at O MPa vs 0.1 MPa mechanical pressure: capacityretention curves showing 24.31% decay at o MPa versus 5.14% decay at 0.1 MPa, DCIR evolution, and d0/dV differential capacity analysis for the second cycle

Figure 1. Electrochemical performance of LFP/graphite batteries under 0 MPa and 0.1 MPa mechanical pressure: (a) capacity retention; (b) DCIR evolution; (c–d) charge/discharge curves and dQ/dV analysis. Capacity decay: 0 MPa → 24.31%; 0.1 MPa → 5.14%.

4. Mechanism 2 — Cathode Structural Integrity and Reduced Interfacial Side Reactions

Post-cycling characterization of the LFP cathode reveals that mechanical pressure substantially preserves cathode structural integrity and reduces parasitic interfacial reactions on the cathode side. SEM imaging shows that LFP cathode particles maintain more complete morphology after cycling under 0.1 MPa pressure compared to the 0 MPa condition, where greater particle fracture and surface roughening are evident.

Quantitative phase analysis using XRD shows that the irreversible FePO₄ phase content — residual non-lithiated cathode material that cannot be re-lithiated, representing permanently lost capacity — is reduced from 34.1% to 18.8% under 0.1 MPa pressure. This 45% reduction in irreversible phase content confirms that mechanical pressure promotes more complete and reversible LiFePO₄/FePO₄ two-phase cycling, directly explaining the improved capacity retention.

XPS (X-ray photoelectron spectroscopy) surface analysis indicates that pressure reduces the accumulation of electrolyte decomposition products on the cathode surface — including phosphate and fluoride species from PF₆⁻ anion decomposition — consistent with the lower interfacial side reaction rate enabled by more stable electrode–electrolyte contact under pressure. Reduced aluminum current collector corrosion under pressure also contributes to maintained cathode current collection efficiency throughout cycling.

In-situ XRD and temperature analysis of LFP cathode under O MPa and 0.1 MPa mechanical pressure during charging:showing more uniform LiFePO4/FePO4 two- phase transformation under O.1 MPa and lower temperature rise confirming reduced Joule heating

Figure 2. In-situ XRD and temperature evolution of LFP cathode under 0 MPa and 0.1 MPa mechanical pressure: (a–b) lattice parameter evolution during LiFePO₄/FePO₄ two-phase transformation showing improved uniformity at 0.1 MPa; (c) temperature profiles confirming reduced thermal accumulation under pressure.

Post-cycling characterization of LFP cathode: SEM morphology comparison showing better particle integrity at 0.1MPa vs o MPa, XPS surface chemistry showing reduced electrolyte decomposition products, and XRD phase analysisshowing irreversible FePO4 content reduced from 34.1% to 18.8% under pressure

Figure 3. Post-cycling LFP cathode characterization: (a) SEM morphology; (b) XRD phase analysis — irreversible FePO₄: 34.1% (0 MPa) → 18.8% (0.1 MPa); (c) XPS surface chemistry showing reduced electrolyte decomposition product accumulation under pressure.

5. Mechanism 3 — LiF-Rich SEI Formation and Graphite Anode Protection

The most mechanistically significant finding of this study is that 0.1 MPa mechanical pressure fundamentally alters the composition and morphology of the SEI layer that forms on the graphite anode surface during cycling.

Under 0 MPa conditions, the graphite anode SEI layer is dominated by organic components — lithium alkyl carbonates (ROCO₂Li, ROLi) and lithium carbonate (Li₂CO₃) — which are mechanically soft and prone to cracking during the 10–15% volume expansion and contraction of graphite during lithiation/de-lithiation cycles. Cracks in the organic SEI expose fresh graphite surface, triggering further electrolyte decomposition and SEI regrowth in an ongoing capacity-consuming cycle that progressively thickens the SEI and increases interfacial impedance.

Under 0.1 MPa mechanical pressure, XPS, FTIR, HRTEM, and TOF-SIMS characterization consistently show that the graphite anode SEI layer becomes:

  • LiF-rich: inorganic LiF content in the SEI is substantially higher under pressure. LiF has high mechanical strength (Young’s modulus ~65 GPa), high ionic conductivity for Li⁺ transport, and chemical stability against further reduction — making it an ideal SEI component for long-term cycling stability.
  • More uniform: the LiF-rich SEI distributes more homogeneously across the graphite particle surface, eliminating the composition gradients and localized weak spots that initiate cracking under mechanical stress during cycling.
  • More mechanically stable: the harder, denser LiF-rich SEI layer maintains integrity during graphite volume expansion/contraction cycles, suppressing ongoing electrolyte decomposition and graphite structural damage.

TOF-SIMS depth profiling confirms the compositional differences between pressurized and unpressurized SEI layers at nanometer resolution, showing that LiF species are enriched throughout the SEI thickness (not merely at the surface) under 0.1 MPa pressure. HRTEM imaging shows that the pressurized graphite anode retains a more ordered crystal structure with fewer structural defects after cycling — consistent with the protective effect of a mechanically stable SEI that prevents solvent co-intercalation and graphite exfoliation.

Post-cycling graphite anode characterization under O MPa and 0.1 MPa mechanical pressure:XPS showing LiF-rich SEIcomposition at O.1 MPa, AFM surface morphology showing more uniform SEl layer, HRTEM showing preserved graphitecrystal structure, and TOF-SIMS depth profiling confirming LiF enrichment throughout SEl thickness

Figure 4. Post-cycling graphite anode characterization: (a) XPS C 1s and F 1s spectra showing LiF-rich SEI composition under 0.1 MPa; (b) AFM surface morphology — more uniform SEI under pressure; (c) HRTEM showing preserved graphite crystal lattice; (d) TOF-SIMS depth profiles confirming LiF enrichment throughout SEI at 0.1 MPa.

6. The Role of IEST PRCD3100 in This Research

🔬 IEST Instrument Contribution to This Research

The Beijing Institute of Technology research team utilized IEST Instrument’s PRCD series Powder Resistivity and Compaction Density Measurement System in the electrode material characterization workflow for this study. The PRCD system provides simultaneous measurement of powder electronic resistivity and compaction density under controlled pressure (up to 350 MPa) — directly supporting the electrode material characterization that underpins the pressure-dependent interfacial behavior studied in this paper. Electrode powder resistivity under controlled compression is a key parameter for understanding how mechanical pressure modifies electrode particle contact resistance and electronic transport — variables central to the interfacial stability analysis reported here.

Acknowledgement: “The authors also thank for the support from Initial Energy Science & Technology Co., Ltd (IEST).” — Wang et al., Nano Materials Science, 2025.

Acknowledgement The authors also thank for the support from Initial Energy Science & Technology Co., Ltd (IEST). — Wang et al., Nano Materials Science, 2025.Figure 5. IEST Instrument is acknowledged in the paper’s Acknowledgments section.

7. Conclusions and Implications for LFP Battery Module Design

This study provides the most comprehensive multi-scale characterization of mechanical pressure effects on LFP/graphite battery interfacial stability published to date, combining electrochemical testing (DCIR, dQ/dV), in-situ structural analysis (XRD), and surface/interface characterization (SEM, AFM, HRTEM, XPS, FTIR, TOF-SIMS) to establish a mechanistic framework linking applied pressure to battery performance.

The central conclusion is that moderate mechanical pressure (0.1 MPa) is not merely an external packaging constraint but an active regulator of LFP/graphite battery chemistry and degradation pathways:

  • On the graphite anode: pressure promotes LiF-rich, uniform, mechanically stable SEI formation → suppresses electrolyte decomposition, graphite structural damage, and capacity-consuming SEI regrowth.
  • On the LFP cathode: pressure promotes uniform LiFePO₄/FePO₄ two-phase transformation → reduces irreversible FePO₄ phase accumulation (34.1% → 18.8%), reduces Joule heating, and decreases aluminum current collector corrosion.
  • At the system level: these combined effects reduce capacity decay from 24.31% to 5.14% — a nearly 5× improvement in cycling stability — with lower DCIR growth, reduced polarization, and lower temperature rise throughout cycling.

Key quantitative findings: 0.1 MPa mechanical pressure applied to LFP/graphite batteries reduces capacity decay from 24.31% to 5.14%; reduces irreversible FePO₄ phase from 34.1% to 18.8%; promotes LiF-rich, uniform SEI layer formation on graphite anodes; and suppresses aluminum current collector corrosion. These findings establish that stack pressure in battery modules is a primary design variable for interfacial stability and long-term LFP/graphite battery performance — not merely a mechanical packaging consideration — and provide quantitative targets (approximately 0.1 MPa) for optimizing module assembly preload to maximize cycle life in EV and energy storage applications.

8. Original Paper

Wang Y., Yan K., Dong J., Tang R., Guan Y., Zhao G., Lu Y., Hao J., Li B., Mo S., He X., Li N., Chen L., Wu F., Su Y. Pressurized vs. unpressurized LiFePO₄ batteries: A comparative study on interfacial stability and electrochemical performance. Nano Materials Science, 2025. DOI: 10.1016/j.nanoms.2025.11.020

9. Related IEST Testing Solutions for LFP Battery Research

IEST Instrument provides a comprehensive portfolio of testing systems directly applicable to the research methodologies used in this study:

10. FAQ: Mechanical Pressure Effects on LFP/Graphite Battery SEI and Interfacial Stability

10.1 How does mechanical pressure improve LFP/graphite battery performance?

Mechanical pressure (0.1 MPa) improves LFP/graphite battery performance through four coupled mechanisms: (1) it promotes the formation of a LiF-rich, uniform, mechanically stable SEI layer on the graphite anode — suppressing ongoing electrolyte decomposition and capacity-consuming SEI regrowth; (2) it enables more uniform LiFePO₄/FePO₄ two-phase transformation across the cathode electrode, reducing irreversible phase loss (34.1% → 18.8% irreversible FePO₄); (3) it reduces aluminum current collector corrosion and harmful by-product deposition on the cathode side; and (4) it lowers DCIR growth rate and Joule heating throughout cycling. Together these mechanisms reduce capacity decay from 24.31% (0 MPa) to 5.14% (0.1 MPa) — a nearly 5× improvement.

10.2 What is a LiF-rich SEI layer and why is it better for battery cycling stability?

A LiF-rich SEI layer is a solid electrolyte interphase film on the graphite anode surface in which inorganic lithium fluoride (LiF) is the dominant component, compared to the organic carbonates (ROCO₂Li, Li₂CO₃) that dominate SEI in unpressurized conditions. LiF-rich SEI layers are superior for cycling stability for three reasons: (1) LiF has high mechanical hardness (Young’s modulus ~65 GPa), allowing the SEI to accommodate repeated graphite volume expansion (10–15%) without cracking; (2) LiF is chemically stable against further reductive decomposition, suppressing ongoing electrolyte consumption at the anode interface; (3) LiF provides sufficient Li⁺ ionic conductivity for lithiation while blocking electron transport and solvent co-intercalation. The result is a protective SEI that maintains its passivating function throughout thousands of cycles rather than continuously growing and consuming electrolyte.

10.3 What is the optimal mechanical pressure for LiFePO4 battery modules?

This study demonstrates that 0.1 MPa mechanical pressure is highly effective for LFP/graphite batteries, reducing capacity decay from 24.31% to 5.14% compared to unpressurized cycling. The 0.1 MPa value is consistent with the typical assembly preload range used in commercial EV battery modules (0.05–0.5 MPa depending on cell format). The study provides quantitative evidence that this pressure range is sufficient to activate the beneficial interfacial chemistry effects (LiF-rich SEI, uniform phase transformation) while remaining below the threshold that would cause excessive compressive stress on electrode particles. Importantly, pressure uniformity across the cell face is as important as magnitude — non-uniform pressure creates localized stress concentrations that can accelerate rather than suppress degradation.

10.4 How does mechanical pressure affect LiFePO4/FePO4 phase transformation?

Mechanical pressure improves LiFePO₄/FePO₄ two-phase transformation in two ways, as shown by in-situ XRD and dQ/dV analysis. First, it promotes more spatially uniform phase transformation across the cathode electrode — preventing lithium extraction/insertion from concentrating in localized regions that experience more rapid structural degradation. Second, it improves phase transformation reversibility: the irreversible FePO₄ content (residual non-lithiated phase that cannot be re-lithiated) is reduced from 34.1% to 18.8% under 0.1 MPa pressure. This 45% reduction in irreversible phase directly translates to recovered capacity retention. The improved phase transformation uniformity also produces sharper, better-defined peaks in dQ/dV analysis — indicating preserved electrochemical reaction kinetics throughout cycling under pressure.

10.5 What characterization techniques are used to study pressure effects on battery interfaces?

This study employed a comprehensive multi-scale characterization approach: electrochemical characterization (DCIR measurement, charge/discharge curves, dQ/dV differential capacity analysis) for performance tracking; in-situ XRD during cycling for real-time cathode phase transformation monitoring; post-cycling SEM and AFM for electrode morphology and SEI surface uniformity; HRTEM for graphite crystal structure and SEI layer imaging at atomic resolution; XPS for surface chemical composition analysis of cathode and anode interfaces; FTIR for molecular-level identification of SEI organic components; and TOF-SIMS for nanometer-resolution SEI depth composition profiling. Together these techniques provide the complete picture from macroscopic electrochemical response through atomic-scale interface chemistry needed to establish mechanistic understanding of pressure effects on LFP/graphite battery interfacial stability.

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