heterogeneities in individual particles detected by synchrotron X-ray provide deep insights on the possible degradation mechanisms, the evolutions of the heterogeneities among hundreds of particles sitting in realistic surroundings are critical for the understanding of the true local electrochemical kinetics that dictate the real-time performance. Recent breakthroughs in a few synchrotron facilities have enabled in situ imaging of large number of particles in realistic battery electrodes. [18,19,24-27] However, achieving very high spatial and temporal resolutions at the same time is still very challenging. Yet more accessible testing platforms that can enable the economical and systematic verifications of new mathematical models to achieve the comprehensive understanding of dynamic heterogeneities in relevant electrochemical systems are critically needed. The immediate consequence of the spatiotemporal heterogeneities is that the actual reacting interfacial area at any instant, i.e., area of the operando (local and working) electrochemical interface, is only a small portion of the total available interfacial area usually obtained from the Brunauer-Emmett-Teller (BET) method. Given that existing electroanalytical techniques [28,29] rely on the square-law scaling D Li ∼ [I(t)/S] 2 to extract the diffusion coefficient D Li from the total current I(t) and the assumed constant total interfacial area S, the electrochemical kinetics in systems with strong heterogeneities may have been misinterpreted due to the smaller operando interfacial area. As one of the most widely used electrodes for both the nonaqueous [15,30] and aqueous [31] batteries, graphite electrodes are known to have strong reaction heterogeneities [13,15] reflected by its particle-by-particle reaction mechanism, [15,22] during the phase transformation between ordered stages [32] upon ion intercalation. Depending on the choices of electrode area, e.g., BET or geometric, the lithium-ion diffusion coefficient in graphite (D Li) extracted by the classic electroanalytical methods varies by about 8 orders of magnitude in the literature. [33-41] Still, D Li obtained for SOC ranges with phase transformation were always about 2 orders of magnitude lower than the average. [34,40] The discrepancy has long been doubted as the inaccuracy of the interfacial area, [42] but conclusive evidence is still missing. Similar orders-of-magnitude discrepancies also exist in other porous electrodes composed of phase-transforming [29] or solidsolution particles, [43-45] missing satisfactory explanations. The Electrochemical energy systems rely on particulate porous electrodes to store or convert energies. While the three-dimensional (3D) porous structures are introduced to maximize the interfacial area for better overall performance of the system, spatiotemporal heterogeneities arising from materials thermodynamics are localizing the charge transfer processes onto a limited portion of the available interfaces. Here, a simple but precise method is demonstrated to directly track an...