621 Angewandte Physik
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Understanding how electrolyte composition influences the structural factors governing charge storage in Prussian Blue analogues (PBAs) requires clarifying the coupled effects of ion desolvation, structural disorder, and transport pathway connectivity. Here, we demonstrate that electrolyte identity induces structural disorder, which correlates with transport dispersion measured under identical electrochemical conditions.
To establish this relationship, Fe-, Co-, and Ni-based hexacyanoferrate thin films were electrodeposited from chloride electrolytes (KCl, NaCl, NH4Cl, and LiCl), enabling a comparative investigation of structure–transport correlations across multiple length scales.
Although all systems crystallize in the cubic PBA structure, pronounced electrolyte-dependent variations in lattice parameters, defect concentration, and local coordination environments are observed. Na+ induces lattice expansion but simultaneously promotes vacancy formation, microstrain, and structural heterogeneity, whereas K+ and NH+4 produce more structurally coherent frameworks with reduced disorder. Raman spectroscopy reveals that increasing structural disorder broadens the distribution of local coordination environments, which
is accompanied by increasingly dispersed electrochemical behavior.
Electrochemical impedance spectroscopy reveals that charge storage is governed by coupled ion–electron transport processes, with the impedance increasing by more than one order of magnitude from FeHCF to NiHCF. Importantly, the constant phase element (CPE) exponent decreases systematically with increasing Raman band broadening, revealing a strong correlation between structural disorder and transport dispersion.
These results demonstrate that electrolyte identity controls not only lattice dimensions but, more importantly, the organization and connectivity of defect networks. Consequently, optimal electrochemical performance arises from a balance between structural coherence and accessible transport pathways rather than from lattice expansion alone.
This article presents analytical approaches for determining the stress state in hypotrochoidal profiles (H-profiles) under torsional, bending, and shear loading. The focus lies on shear loading. Using conformal mapping, a formulation of elasticity theory is first adapted to H-profile cross-sections. Closed-form solutions for the respective stress components are then derived by solving a reformulated surface integral. Suitable conformal mappings for hypotrochoidal contours are obtained through a successive method applied to their parametric description. These mappings are essential for the elasticity-theoretical formulation used to determine the stress state in the profile bar. Building on this, the transverse shear stresses for H-profile cross-sections are determined for the first time. The influence of shear stresses on the overall stress state is discussed in detail. These stresses generally act in a rotational manner and superimpose on the torsional stresses. This effect proves more pronounced here than in circular cross-sections. Accompanying finite element analyses (FEA), carried out for several examples, showed very good agreement with the analytical solutions. From the resulting maximum stress values and stress gradients, form and notch factors are calculated. The proposed procedure also applies to combined loading cases. It is intended for use in the new standard covering hypotrochoidal profile contours.
燃料电池汽车氢气泄漏扩散分区域数值研究
(2026)
Conventional industrial‐scale production of metal powders generally occurs in large plants, where each batch sizes several hundred kilograms of powder. However, these production methods are economically impractical for manufacturers with lower demands, such as those involved in prototyping and developing new alloys for additive manufacturing. This study investigates wire arc atomizing as a viable alternative for producing metal powders that are specifically tailored to precise requirements and manufactured in a batch size of one. The wire melting process is controlled by modulating the electrical current, using pulsed and unpulsed DC. Arc power varies across a wide range to assess its impact on particle size distribution. Furthermore, the produced metal powders undergo comprehensive characterization and evaluation to determine their suitability for additive manufacturing, ensuring they meet specific application requirements.
Accurate monitoring of the hydrogen concentration is critical for optimizing fuel cell performance, minimizing purge losses, and reducing long-term degradation. Conventional hydrogen sensors often rely on catalytic materials and face limitations such as the need of oxygen purging when operated in fuel cell environments. Here, we report the discovery of a novel hydrogen-sensing mechanism based on organic molecules, without the use of catalytic metals. The sensor is based on a typical vertical stack geometry, containing Alq3 as active organic material. Upon exposure to hydrogen, the device shows an increase in resistivity, yielding a reliable sensor signal that varies linearly with hydrogen concentration, temperature, and humidity, and exhibits a relative response of up to 3.5 % at 100 %vol hydrogen. By exposing the sensor to an external magnetic field, the rise and fall times of the sensor response were found to be tunable. This novel organic sensor demonstrates sensitivity across a wide range of hydrogen concentrations under fuel cell-relevant conditions and beyond. This new class of hydrogen sensors with high miniaturization potential and cost efficiency paves the way for real-time hydrogen monitoring and advanced control strategies in fuel cells, the chemical industry, or energy storage applications.
More than half a century of intense research in modern control theory has not stopped practitioners from continuing to use PID controllers for most real-world control problems. While not a mathematical one, this might be the most convincing proof of their robustness: if necessary, they can be implemented with minimal control engineering experience. Often, controllers are designed by individuals who are experts in their specific domain but are not dedicated control theory specialists. To address the needs of these engineers, this article wants to put an approach known as Active Disturbance Rejection Control (ADRC) in the spotlight—a method that has gradually evolved into an industry-ready alternative to PID control. Reflecting on two decades of improvements, this article portrays ADRC as a solution for everyday control problems that can be both easier to use and richer in out-of-the-box features.
This work investigates the optical stability of formamidinium–cesium lead halide perovskite thin films deposited on fluorine-doped tin oxide substrates and aged under ambient conditions for 21 days. The optical response was analyzed through specular and diffuse transmittance and reflectance measurements, collected with light incident from both sides of the heterostructure. Specular transmittance exhibits nonmonotonic variations with an initial increase followed by a gradual decrease over time, while diffuse transmittance increases systematically across the full spectral range, indicating the progressive formation of scattering centers. Total reflectance decreases monotonically with aging, revealing that degradation is primarily governed by absorption-related optical losses. Despite these changes, the absorption edge remains stable, and the optical bandgap and Urbach tail show no significant variation. Direction-dependent measurements demonstrate that the fluorine-doped tin oxide substrate is the dominant source of initial scattering whereas the perovskite layer initially reduces optical contrast and later introduces disorder as degradation progresses. Haze values remain nearly constant over time, indicating that changes in scattering efficiency are moderate compared to absorption losses. These results demonstrate that integrating sphere-based optical spectroscopy provides a nondestructive and effective framework for monitoring early stage degradation in perovskite thin films.