Pub Date : 2026-10-08Epub Date: 2026-09-26DOI: 10.1021/acs.jpcb.6c04328
Eric P. Jacobo, Michael J. Martinez, Barbara Barile, Alessia Memeo, Grazia Paola Nicchia, James A. Brozik
Aquaporin-4 (AQP4)is an integral membrane protein channel specificfor water molecules. It is highly polarized in the endfeet of astrocytesin the central nervous system where it allows water–ion homeostasis.AQP4 has two N-terminal isoforms: M1 (long) and M23 (short). Bothisoforms retain their function but differ in their N-terminal lengths,which regulate AQP4 aggregation size. There are also long and shortisoforms at the C-terminus. The long form has a 29-amino-acid extension(AQP4ex) that interacts with α-syntrophin, a component of thedystrophin-associated protein complex (DAPC). This interaction anchorsAQP4 to the perivascularastrocyte endfeet through the DAPC, therebymaintaining its polarized localization at the blood–brain barrier.This study uses peptides with the sequence of the extended regionto demonstrate a strong interaction with α-syntrophin, boundto a glass surface via maleimide-PEG silane chemistry. It was observedthat substituting alanine for threonine, four amino acids from theC-terminus, eliminates binding, and an alanine scan shows that thelast six amino acids at the C-terminus also play a crucial role. Kineticstudies using time-lapse single-molecule fluorescence imaging wereused to determine the Gibbs free energy of activation for both forwardand reverse rates (ΔG‡) usingan Eyring analysis. Equilibrium constants (Keq) were measured between 15 and 37 °C, and standard-statethermodynamic free energies (ΔG°), enthalpies(ΔH°), and entropies (ΔS°) were determined using a van’t Hoff analysis. It wasfound that forward rates ranged from 4.5 × 104 to1.0 × 105 M–1 s–1 depending on peptide length, with ΔG‡forward = 45–46 kJ mol–1. Reverse rates ranged from 11.6 to 21.1 s–1 dependingon peptide length, with ΔG‡reverse = 65.2–67.0 kJ mol–1.Using a vant’ Hoff analysis, the overall standard-state freeenergies were between −19 and −22 kJ mol–1. The work also describes how dynamic single-molecule imaging canbe used to determine kinetic and thermodynamic properties.
{"title":"AQP4 Extended Region Binds to α-Syntrophin with a Novel Binding Motif","authors":"Eric P. Jacobo, Michael J. Martinez, Barbara Barile, Alessia Memeo, Grazia Paola Nicchia, James A. Brozik","doi":"10.1021/acs.jpcb.6c04328","DOIUrl":"https://doi.org/10.1021/acs.jpcb.6c04328","url":null,"abstract":"<p>Aquaporin-4 (AQP4)is an integral membrane protein channel specificfor water molecules. It is highly polarized in the endfeet of astrocytesin the central nervous system where it allows water–ion homeostasis.AQP4 has two N-terminal isoforms: M1 (long) and M23 (short). Bothisoforms retain their function but differ in their N-terminal lengths,which regulate AQP4 aggregation size. There are also long and shortisoforms at the C-terminus. The long form has a 29-amino-acid extension(AQP4ex) that interacts with α-syntrophin, a component of thedystrophin-associated protein complex (DAPC). This interaction anchorsAQP4 to the perivascularastrocyte endfeet through the DAPC, therebymaintaining its polarized localization at the blood–brain barrier.This study uses peptides with the sequence of the extended regionto demonstrate a strong interaction with α-syntrophin, boundto a glass surface via maleimide-PEG silane chemistry. It was observedthat substituting alanine for threonine, four amino acids from theC-terminus, eliminates binding, and an alanine scan shows that thelast six amino acids at the C-terminus also play a crucial role. Kineticstudies using time-lapse single-molecule fluorescence imaging wereused to determine the Gibbs free energy of activation for both forwardand reverse rates (Δ<em>G</em><sup>‡</sup>) usingan Eyring analysis. Equilibrium constants (<em>K</em><sub>eq</sub>) were measured between 15 and 37 °C, and standard-statethermodynamic free energies (Δ<em>G</em>°), enthalpies(Δ<em>H</em>°), and entropies (Δ<em>S</em>°) were determined using a van’t Hoff analysis. It wasfound that forward rates ranged from 4.5 × 10<sup>4</sup> to1.0 × 10<sup>5</sup> M<sup>–1</sup> s<sup>–1</sup> depending on peptide length, with Δ<em>G</em><sup>‡</sup><sub>forward</sub> = 45–46 kJ mol<sup>–1</sup>. Reverse rates ranged from 11.6 to 21.1 s<sup>–1</sup> dependingon peptide length, with Δ<em>G</em><sup>‡</sup><sub>reverse</sub> = 65.2–67.0 kJ mol<sup>–1</sup>.Using a vant’ Hoff analysis, the overall standard-state freeenergies were between −19 and −22 kJ mol<sup>–1</sup>. The work also describes how dynamic single-molecule imaging canbe used to determine kinetic and thermodynamic properties.</p>","PeriodicalId":60,"journal":{"name":"The Journal of Physical Chemistry B","volume":"130 40","pages":"10427–10437"},"PeriodicalIF":3.2,"publicationDate":"2026-10-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149124898","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
In this study, molecular dynamics simulations combinedwith Ramanspectroscopic characterization were employed to investigate the localcoordination environments, oxygen coordination states, polyhedralconnectivity, and network polymerization characteristics in binaryAl2O3–Y2O3 glasseswithin the composition range of 60–75 mol % Al2O3. Comprehensive analysis of the radial distribution function,coordination number distribution, and angular distribution functionhas been used to characterize the short-range ordered structures ofAl–O and Y–O and to elucidate the distribution characteristicsof aluminum–oxygen structure units such as [AlO4], [AlO5], and [AlO6]. Furthermore, the evolutionof corner-sharing and edge-sharing behaviors, revealed by bond-anglevariations, has been identified. Distributions of oxygen species and Qi species further revealed the evolution ofglass network connectivity with composition variation. Deconvolutionof Raman spectra in the high-wavenumber region enabled the quantitativeanalysis of microstructure species. This study provided a comprehensiveunderstanding of the structure evolution in Al-rich binary Al2O3–Y2O3 glasses, establishinga theoretical foundation for the rational network design.
{"title":"Microstructure of Binary Al2O3–Y2O3 Glasses Investigated by Molecular Dynamics Simulation and Raman Spectroscopy","authors":"Xiang Xia, Jinglin You, Yufan Zhao, Jiansheng Geng, Longxing Zhang, Wenna Ren, Jian Song, Guopeng Liu, Qingli Zhang, Songming Wan","doi":"10.1021/acs.jpcb.6c02956","DOIUrl":"https://doi.org/10.1021/acs.jpcb.6c02956","url":null,"abstract":"<p>In this study, molecular dynamics simulations combinedwith Ramanspectroscopic characterization were employed to investigate the localcoordination environments, oxygen coordination states, polyhedralconnectivity, and network polymerization characteristics in binaryAl<sub>2</sub>O<sub>3</sub>–Y<sub>2</sub>O<sub>3</sub> glasseswithin the composition range of 60–75 mol % Al<sub>2</sub>O<sub>3</sub>. Comprehensive analysis of the radial distribution function,coordination number distribution, and angular distribution functionhas been used to characterize the short-range ordered structures ofAl–O and Y–O and to elucidate the distribution characteristicsof aluminum–oxygen structure units such as [AlO<sub>4</sub>], [AlO<sub>5</sub>], and [AlO<sub>6</sub>]. Furthermore, the evolutionof corner-sharing and edge-sharing behaviors, revealed by bond-anglevariations, has been identified. Distributions of oxygen species and <em>Q</em><sub>i</sub> species further revealed the evolution ofglass network connectivity with composition variation. Deconvolutionof Raman spectra in the high-wavenumber region enabled the quantitativeanalysis of microstructure species. This study provided a comprehensiveunderstanding of the structure evolution in Al-rich binary Al<sub>2</sub>O<sub>3</sub>–Y<sub>2</sub>O<sub>3</sub> glasses, establishinga theoretical foundation for the rational network design.</p>","PeriodicalId":60,"journal":{"name":"The Journal of Physical Chemistry B","volume":"130 40","pages":"10704–10718"},"PeriodicalIF":3.2,"publicationDate":"2026-10-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149124883","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-10-08Epub Date: 2026-09-24DOI: 10.1021/acs.jpcb.6c02313
Thomas D. Killeen, Michael R. Stoneman, Ionel Popa, Qiuyan Chen, Valerică Raicu
Investigations ofG protein-coupled receptors (GPCRs)interactionswith nonvisual arrestins in living cells are essential to understandingthe complex molecular mechanisms of GPCR-based signaling. Quantitativeanalysis of these interactions remains challenging in live cells,particularly when attempting to repeatedly image distinct cellularregions with high precision. Here, we describe the implementationof an optical imaging stabilization approach that integrates the recentlydeveloped Focal Readjustment for Enhanced Vertical Resolution (FREVR)technology into a multiphoton microscope, enabling high-precisionalternation between image-forming sample planes with <20 nanometerrepeatability and stability over time. Using this setup, we monitoredthe dynamic recruitment of arrestin-2 (Arr2) to the plasma membraneof HEK-293 cells expressing muscarinic acetylcholine M2 receptors (M2R) by alternately imaging distinct planesof interest, the basolateral membrane and a membrane cross-section.Following stimulation of M2R by agonist ligand, we observeda pronounced redistribution of cytoplasmic Arr2 toward the plasmamembrane in both cellular cross sections and at the basolateral membrane.This method enables direct comparison of receptor and arrestin dynamicsacross regions of individual cells with very high precision, eliminatingthe need for averaging over numerous cells in order to denoise biologicallyrelevant signals, and thereby capturing physiological cell-to-cellvariability with accuracy.
{"title":"Precise Alternation between Image-Forming Sample Planes Enables Quantitative Monitoring of Receptor-Arrestin Interaction Dynamics at the Plasma Membrane of Live Cells","authors":"Thomas D. Killeen, Michael R. Stoneman, Ionel Popa, Qiuyan Chen, Valerică Raicu","doi":"10.1021/acs.jpcb.6c02313","DOIUrl":"https://doi.org/10.1021/acs.jpcb.6c02313","url":null,"abstract":"<p>Investigations ofG protein-coupled receptors (GPCRs)interactionswith nonvisual arrestins in living cells are essential to understandingthe complex molecular mechanisms of GPCR-based signaling. Quantitativeanalysis of these interactions remains challenging in live cells,particularly when attempting to repeatedly image distinct cellularregions with high precision. Here, we describe the implementationof an optical imaging stabilization approach that integrates the recentlydeveloped Focal Readjustment for Enhanced Vertical Resolution (FREVR)technology into a multiphoton microscope, enabling high-precisionalternation between image-forming sample planes with <20 nanometerrepeatability and stability over time. Using this setup, we monitoredthe dynamic recruitment of arrestin-2 (Arr2) to the plasma membraneof HEK-293 cells expressing muscarinic acetylcholine M<sub>2</sub> receptors (M<sub>2</sub>R) by alternately imaging distinct planesof interest, the basolateral membrane and a membrane cross-section.Following stimulation of M<sub>2</sub>R by agonist ligand, we observeda pronounced redistribution of cytoplasmic Arr2 toward the plasmamembrane in both cellular cross sections and at the basolateral membrane.This method enables direct comparison of receptor and arrestin dynamicsacross regions of individual cells with very high precision, eliminatingthe need for averaging over numerous cells in order to denoise biologicallyrelevant signals, and thereby capturing physiological cell-to-cellvariability with accuracy.</p>","PeriodicalId":60,"journal":{"name":"The Journal of Physical Chemistry B","volume":"130 40","pages":"10371–10382"},"PeriodicalIF":3.2,"publicationDate":"2026-10-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149124918","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-10-08Epub Date: 2026-09-24DOI: 10.1021/acs.jpcb.6c02604
Marius Fiedler, Thomas Waluga, Irina Smirnova, Sven Jakobtorweihen
Protein adsorption at solid–liquid interfacesplays a crucialrole in many biological and technological processes, including thedesign of biomaterials, biosensor performance, and biocatalysis. Understandinghow proteins interact with surfaces is essential for controlling biofouling,optimizing medical implants, and engineering functional interfaces.Despite its significance, predicting adsorption behavior from molecular-levelinteractions remains challenging. In this work, we performed moleculardynamics simulations using umbrella sampling to sample the two-dimensionalfree-energy surface of bovine serum albumin adsorption on the anionicadsorbent Q Sepharose FF. By combining molecular dynamics simulationswith enhanced free energy sampling techniques, we systematically exploredthe orientations and positions of the protein near the surface. Noconformational changes were observed within the examined time scales.We obtained a comprehensive free-energy map that captures the adsorptionbehavior across the entire protein surface. This approach providesaccess to the adsorption free energy while accounting for contributionsfrom all possible adsorption sites and orientations. The resultinglandscape offers a detailed molecular-level understanding of how proteinsinteract with surfaces.
{"title":"Mapping the Free Energy Landscape of Protein Adsorption at Solid-Liquid Interfaces","authors":"Marius Fiedler, Thomas Waluga, Irina Smirnova, Sven Jakobtorweihen","doi":"10.1021/acs.jpcb.6c02604","DOIUrl":"https://doi.org/10.1021/acs.jpcb.6c02604","url":null,"abstract":"<p>Protein adsorption at solid–liquid interfacesplays a crucialrole in many biological and technological processes, including thedesign of biomaterials, biosensor performance, and biocatalysis. Understandinghow proteins interact with surfaces is essential for controlling biofouling,optimizing medical implants, and engineering functional interfaces.Despite its significance, predicting adsorption behavior from molecular-levelinteractions remains challenging. In this work, we performed moleculardynamics simulations using umbrella sampling to sample the two-dimensionalfree-energy surface of bovine serum albumin adsorption on the anionicadsorbent Q Sepharose FF. By combining molecular dynamics simulationswith enhanced free energy sampling techniques, we systematically exploredthe orientations and positions of the protein near the surface. Noconformational changes were observed within the examined time scales.We obtained a comprehensive free-energy map that captures the adsorptionbehavior across the entire protein surface. This approach providesaccess to the adsorption free energy while accounting for contributionsfrom all possible adsorption sites and orientations. The resultinglandscape offers a detailed molecular-level understanding of how proteinsinteract with surfaces.</p>","PeriodicalId":60,"journal":{"name":"The Journal of Physical Chemistry B","volume":"130 40","pages":"10690–10703"},"PeriodicalIF":3.2,"publicationDate":"2026-10-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149124850","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Althoughphotodynamic therapy (PDT) has emerged as apromisingtreatment for unresectable cholangiocarcinoma, the hypoxic tumor microenvironmentseverely limits oxygen-dependent Type II photochemical processes,resulting in insufficient reactive oxygen species (ROS) generationand compromised therapeutic outcomes. Therefore, developing Type Iphotosensitizers (PSs) with optimized excited-state dynamics and efficienthypoxia-tolerant ROS generation is critical for improving PDT efficacyunder hypoxic conditions. Herein, we developed three hemicyanine-basedType I PSs (HCy1–3) and systematically investigatedthe relationship between molecular structure, TICT-mediated excited-staterelaxation, and ROS generation behavior. By modulating the electron-donatingcapability of donor moieties, the TICT characteristics of the hemicyaninescaffold were precisely tuned, thereby regulating the competitionbetween nonradiative decay and ROS-generating pathways. Among them, HCy3 exhibited enhanced excited-state utilization and thehighest Type I ROS generation efficiency under both normoxic and hypoxicconditions. Furthermore, HCy3 efficiently accumulatedin mitochondria and induced mitochondrial dysfunction, leading tosuperior photodynamic cytotoxicity against cholangiocarcinoma cellsunder hypoxia compared with the clinically used PS HiPorfin. The therapeuticpotential of HCy3 was further validated in cholangiocarcinomaorganoids. This study establishes a structure–photophysics-photochemistrycorrelation between TICT regulation and Type I ROS generation, providinga mechanistic strategy for designing high-performance hypoxia-tolerantPSs for PDT.
{"title":"Tuning Excited-State TICT Dynamics in Hemicyanine Type I Photosensitizers for Hypoxia-Tolerant Photodynamic Therapy of Cholangiocarcinoma","authors":"Yiyan Ruan, Qinglong Qiao, Wenchao Jiang, Xiang Wang, Guixin Zhang, Zhaochao Xu","doi":"10.1021/acs.jpcb.6c05556","DOIUrl":"https://doi.org/10.1021/acs.jpcb.6c05556","url":null,"abstract":"<p>Althoughphotodynamic therapy (PDT) has emerged as apromisingtreatment for unresectable cholangiocarcinoma, the hypoxic tumor microenvironmentseverely limits oxygen-dependent Type II photochemical processes,resulting in insufficient reactive oxygen species (ROS) generationand compromised therapeutic outcomes. Therefore, developing Type Iphotosensitizers (PSs) with optimized excited-state dynamics and efficienthypoxia-tolerant ROS generation is critical for improving PDT efficacyunder hypoxic conditions. Herein, we developed three hemicyanine-basedType I PSs (<strong>HCy1–3</strong>) and systematically investigatedthe relationship between molecular structure, TICT-mediated excited-staterelaxation, and ROS generation behavior. By modulating the electron-donatingcapability of donor moieties, the TICT characteristics of the hemicyaninescaffold were precisely tuned, thereby regulating the competitionbetween nonradiative decay and ROS-generating pathways. Among them, <strong>HCy3</strong> exhibited enhanced excited-state utilization and thehighest Type I ROS generation efficiency under both normoxic and hypoxicconditions. Furthermore, <strong>HCy3</strong> efficiently accumulatedin mitochondria and induced mitochondrial dysfunction, leading tosuperior photodynamic cytotoxicity against cholangiocarcinoma cellsunder hypoxia compared with the clinically used PS HiPorfin. The therapeuticpotential of <strong>HCy3</strong> was further validated in cholangiocarcinomaorganoids. This study establishes a structure–photophysics-photochemistrycorrelation between TICT regulation and Type I ROS generation, providinga mechanistic strategy for designing high-performance hypoxia-tolerantPSs for PDT.</p>","PeriodicalId":60,"journal":{"name":"The Journal of Physical Chemistry B","volume":"130 40","pages":"10488–10496"},"PeriodicalIF":3.2,"publicationDate":"2026-10-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149124941","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-10-08Epub Date: 2026-08-28DOI: 10.1021/acs.jpcb.6c03131
Kailee Buttice, Shubhojit Banerjee, Thiago J. Pinheiro dos Santos, Ellie Kim, Qiufeng Yang, Alejandro Ramos-Ballesteros, Sheng Dai, Ruchi Gakhar, Santanu Roy, Vyacheslav S. Bryantsev, Adrien Couet
Optical basicity measurements provide a basis for determiningtherelative chlorobasicity of a given molten salt composition. This studyuses Bi3+ as a spectroscopic probe to investigate opticalbasicity across three binary molten chloride systems (LiCl-KCl, MgCl2–KCl, and ZnCl2–KCl) through in situUV–vis spectroscopy measurements of the 1S0→3P1 transition. LiCl-KCl systems exhibitthe highest optical basicity with minimal compositional dependence,while both divalent systems show stronger, yet nonlinear, dependencethat is reminiscent of acid–base titration curves. The influenceof cation electronegativity and polarizing power (Li+ <Mg2+ < Zn2+) directly reflects the basicitycurves, with ZnCl2–KCl displaying the steepest gradientsand lowest basicity values. Nonlinear dependencies in divalent systemsindicate formation of chloride-bridged network structures with coordinationstates dictated by the amount of KCl in a salt composition, whichwas further investigated and validated by molecular dynamics simulationsof polymeric structures formed in ZnCl2 and MgCl2-based salts using machine learning force fields. The temperaturedependence of chlorobasicity in terms of optical basicity was investigated,and a loose, positive correlation between the two was revealed. Thesefindings establish Bi3+ as a sensitive probe for understandingelectronic environments in molten chloride systems and provide insightsfor predicting the chemical behavior of molten salts for use in high-temperatureenvironments.
{"title":"In Situ UV–vis Quantification of Chlorobasicity in Binary Molten Chlorides","authors":"Kailee Buttice, Shubhojit Banerjee, Thiago J. Pinheiro dos Santos, Ellie Kim, Qiufeng Yang, Alejandro Ramos-Ballesteros, Sheng Dai, Ruchi Gakhar, Santanu Roy, Vyacheslav S. Bryantsev, Adrien Couet","doi":"10.1021/acs.jpcb.6c03131","DOIUrl":"10.1021/acs.jpcb.6c03131","url":null,"abstract":"<p>Optical basicity measurements provide a basis for determiningtherelative chlorobasicity of a given molten salt composition. This studyuses Bi<sup>3+</sup> as a spectroscopic probe to investigate opticalbasicity across three binary molten chloride systems (LiCl-KCl, MgCl<sub>2</sub>–KCl, and ZnCl<sub>2</sub>–KCl) through in situUV–vis spectroscopy measurements of the <sup>1</sup>S<sub>0</sub>→<sup>3</sup>P<sub>1</sub> transition. LiCl-KCl systems exhibitthe highest optical basicity with minimal compositional dependence,while both divalent systems show stronger, yet nonlinear, dependencethat is reminiscent of acid–base titration curves. The influenceof cation electronegativity and polarizing power (Li<sup>+</sup> <Mg<sup>2+</sup> < Zn<sup>2+</sup>) directly reflects the basicitycurves, with ZnCl<sub>2</sub>–KCl displaying the steepest gradientsand lowest basicity values. Nonlinear dependencies in divalent systemsindicate formation of chloride-bridged network structures with coordinationstates dictated by the amount of KCl in a salt composition, whichwas further investigated and validated by molecular dynamics simulationsof polymeric structures formed in ZnCl<sub>2</sub> and MgCl<sub>2</sub>-based salts using machine learning force fields. The temperaturedependence of chlorobasicity in terms of optical basicity was investigated,and a loose, positive correlation between the two was revealed. Thesefindings establish Bi<sup>3+</sup> as a sensitive probe for understandingelectronic environments in molten chloride systems and provide insightsfor predicting the chemical behavior of molten salts for use in high-temperatureenvironments.</p>","PeriodicalId":60,"journal":{"name":"The Journal of Physical Chemistry B","volume":"130 40","pages":"10719–10734"},"PeriodicalIF":3.2,"publicationDate":"2026-10-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"148872241","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-10-08Epub Date: 2026-09-25DOI: 10.1021/acs.jpcb.6c03657
Masoom Shaban, Adri C. T. van Duin, Diana van Duin, Margaret Kowalik, Mohammad E. Izadi, Alfred P. Weber, Nina Merkert
Reactive nitrogenspecies (RNSs) are key contributors to plasma-liquidprocesses and play a critical role in the chemistry of plasma-activatedwater (PAW). Despite their importance, their molecular-level behaviorin aqueous environments is still not well understood, largely dueto the absence of reliable reactive force fields. In this study, anew ReaxFF parameter set, ReaxFFCHONx-2026, is developedand systematically assessed for modeling nitrogen- and oxygen-containingreactive species under both gas-phase and aqueous conditions relevantto plasma systems. The parameter set is optimized using density functionaltheory (DFT) reference data for representative NOx reaction pathways and integrated with an existing aqueous/biomolecularReaxFF framework to enable reactive molecular dynamics simulationsin water. Its performance is validated through a range of structural,thermodynamic, and dynamic properties including radial distributionfunctions, potential energy profiles, and diffusion coefficients.The results demonstrate strong agreement with DFT calculations andpreviously reported data, particularly in describing N–O bondbreaking and solvation behavior. As a case study, the interactionof peroxynitrite (ONOO–) with water is investigatedusing reactive molecular dynamics, where atomic charges are dynamicallydetermined via the ReaxFF charge equilibration method. The simulationsshow protonation leading to ONOOH formation, pronounced site-specificsolvation around oxygen atoms, and preferential cleavage of the peroxideO–O bond. Analysis of diffusion further indicates that thepredicted transport properties of RNS are consistent with the availabledata, supporting the reliability of the developed force field. Overall,ReaxFFCHONx-2026 offers a robust framework for large-scaleatomistic simulations of PAW and reactive nitrogen chemistry.
{"title":"A New Reactive Force Field for NOx-Water Interactions: Development, Evaluation, and Molecular Dynamics Simulation of Peroxynitrite","authors":"Masoom Shaban, Adri C. T. van Duin, Diana van Duin, Margaret Kowalik, Mohammad E. Izadi, Alfred P. Weber, Nina Merkert","doi":"10.1021/acs.jpcb.6c03657","DOIUrl":"https://doi.org/10.1021/acs.jpcb.6c03657","url":null,"abstract":"<p>Reactive nitrogenspecies (RNSs) are key contributors to plasma-liquidprocesses and play a critical role in the chemistry of plasma-activatedwater (PAW). Despite their importance, their molecular-level behaviorin aqueous environments is still not well understood, largely dueto the absence of reliable reactive force fields. In this study, anew ReaxFF parameter set, ReaxFF<sub>CHONx</sub>-2026, is developedand systematically assessed for modeling nitrogen- and oxygen-containingreactive species under both gas-phase and aqueous conditions relevantto plasma systems. The parameter set is optimized using density functionaltheory (DFT) reference data for representative NO<sub><em>x</em></sub> reaction pathways and integrated with an existing aqueous/biomolecularReaxFF framework to enable reactive molecular dynamics simulationsin water. Its performance is validated through a range of structural,thermodynamic, and dynamic properties including radial distributionfunctions, potential energy profiles, and diffusion coefficients.The results demonstrate strong agreement with DFT calculations andpreviously reported data, particularly in describing N–O bondbreaking and solvation behavior. As a case study, the interactionof peroxynitrite (ONOO<sup>–</sup>) with water is investigatedusing reactive molecular dynamics, where atomic charges are dynamicallydetermined via the ReaxFF charge equilibration method. The simulationsshow protonation leading to ONOOH formation, pronounced site-specificsolvation around oxygen atoms, and preferential cleavage of the peroxideO–O bond. Analysis of diffusion further indicates that thepredicted transport properties of RNS are consistent with the availabledata, supporting the reliability of the developed force field. Overall,ReaxFF<sub>CHONx</sub>-2026 offers a robust framework for large-scaleatomistic simulations of PAW and reactive nitrogen chemistry.</p>","PeriodicalId":60,"journal":{"name":"The Journal of Physical Chemistry B","volume":"130 40","pages":"10540–10550"},"PeriodicalIF":3.2,"publicationDate":"2026-10-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149124672","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-10-08Epub Date: 2026-09-26DOI: 10.1021/acs.jpcb.6c03572
Ryosuke Kita, Kazuya Kobayashi, Sumihiko Murata
The understanding of mutual solubilitiesin H2-containingsystems is the foundation for improving H2-related processes.This study demonstrates that Gibbs ensemble Monte Carlo simulationssuccessfully predict the mutual solubility of hydrogen-alkane systemsover a wide range of conditions (323.2–462.5 K, 1.7–20.3MPa) with the optimal corrections to the combination rules. We foundthat the solubility of decane and hexadecane in H2 increasesby 2–3.3 times with an increasing number of methyl groups inthe alkane (branching). Notably, a decrease in the solubility parameterand an increase in alkane–H2 interactions are thekey mechanisms responsible for the enhanced solubility in H2. This study enables the prediction of mutual solubility for a varietyof hydrogen–alkane systems and reveals that introducing methylgroups is an effective strategy for enhancing the solubility of compoundsin H2 (termed H2-philicity).
{"title":"Enhancement of the Solubility of Alkanes in Hydrogen by Structural Branching","authors":"Ryosuke Kita, Kazuya Kobayashi, Sumihiko Murata","doi":"10.1021/acs.jpcb.6c03572","DOIUrl":"https://doi.org/10.1021/acs.jpcb.6c03572","url":null,"abstract":"<p>The understanding of mutual solubilitiesin H<sub>2</sub>-containingsystems is the foundation for improving H<sub>2</sub>-related processes.This study demonstrates that Gibbs ensemble Monte Carlo simulationssuccessfully predict the mutual solubility of hydrogen-alkane systemsover a wide range of conditions (323.2–462.5 K, 1.7–20.3MPa) with the optimal corrections to the combination rules. We foundthat the solubility of decane and hexadecane in H<sub>2</sub> increasesby 2–3.3 times with an increasing number of methyl groups inthe alkane (branching). Notably, a decrease in the solubility parameterand an increase in alkane–H<sub>2</sub> interactions are thekey mechanisms responsible for the enhanced solubility in H<sub>2</sub>. This study enables the prediction of mutual solubility for a varietyof hydrogen–alkane systems and reveals that introducing methylgroups is an effective strategy for enhancing the solubility of compoundsin H<sub>2</sub> (termed H<sub>2</sub>-philicity).</p>","PeriodicalId":60,"journal":{"name":"The Journal of Physical Chemistry B","volume":"130 40","pages":"10519–10529"},"PeriodicalIF":3.2,"publicationDate":"2026-10-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149124905","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-10-08Epub Date: 2026-09-29DOI: 10.1021/acs.jpcb.6c02416
Michael K. Gilson, Joe Cruz, Kunhuan Liu, Samrat Lohar, Helmut Carter, Daniel R. Roe, Tom Kurtzman
Systems in which the free energydensity is nonuniformin spaceare familiar; the surface tension of a water droplet and the surfaceenergy of a solid are good examples. Some such cases can be treatedwith prior theory, notably inhomogeneous solvation theory (IST), butIST is applicable only to liquids. Despite this limitation, IST hasproven useful as a guide to the design of ligands to bind a targetedprotein, based on the idea that ligands that displace high free energywater will tend to bind more tightly, other things being equal. Here,we present Generalized Thermodynamic Mapping (GTM) theory, a moregeneral theory that is applicable to the entirety of a biomolecularor other chemical system, and which thus may provide additional guidancefor molecular design. For example, it might highlight parts of a ligandwhose local free energy rises on binding, thus suggesting where modificationscould improve affinity. Starting from classical statistical thermodynamics,we derive structural decompositions that assign energy and entropyto individual atoms or to larger chemical components, such as aminoacid residues, and spatial decompositions that define continuouslyvarying thermodynamic densities throughout the system. The potentialenergy is decomposed via the multibody expansion, and the entropyvia the mutual information expansion. The resulting thermodynamicdensities satisfy key desiderata: their spatial integrals yield thecorrect total thermodynamic quantities, the densities vanish wherethe atomic number density is zero, and all entropy terms above firstorder go to zero in the absence of correlation. The entropy decompositionin GTM theory is closely related to that of IST, but it is simpler,largely because it expresses the entropy in terms of normalized probabilitydensity functions instead of nonnormalized correlation functions.We show that GTM theory is formally exact for any number of particles, N, whereas IST is not. The unified framework presented hereenables thermodynamic mapping of solute and solvent alike and is expectedto support a range of applications, including in structure-based drugdesign, protein design, the analysis of allostery, and materials science.The use of GTM theory to gain insight into protein-ligand bindingis illustrated here with an initial case study.
{"title":"A Generalized Theory for the Structural and Spatial Mapping of Energy, Entropy, and Free Energy","authors":"Michael K. Gilson, Joe Cruz, Kunhuan Liu, Samrat Lohar, Helmut Carter, Daniel R. Roe, Tom Kurtzman","doi":"10.1021/acs.jpcb.6c02416","DOIUrl":"https://doi.org/10.1021/acs.jpcb.6c02416","url":null,"abstract":"<p>Systems in which the free energydensity is nonuniformin spaceare familiar; the surface tension of a water droplet and the surfaceenergy of a solid are good examples. Some such cases can be treatedwith prior theory, notably inhomogeneous solvation theory (IST), butIST is applicable only to liquids. Despite this limitation, IST hasproven useful as a guide to the design of ligands to bind a targetedprotein, based on the idea that ligands that displace high free energywater will tend to bind more tightly, other things being equal. Here,we present Generalized Thermodynamic Mapping (GTM) theory, a moregeneral theory that is applicable to the entirety of a biomolecularor other chemical system, and which thus may provide additional guidancefor molecular design. For example, it might highlight parts of a ligandwhose local free energy rises on binding, thus suggesting where modificationscould improve affinity. Starting from classical statistical thermodynamics,we derive structural decompositions that assign energy and entropyto individual atoms or to larger chemical components, such as aminoacid residues, and spatial decompositions that define continuouslyvarying thermodynamic densities throughout the system. The potentialenergy is decomposed via the multibody expansion, and the entropyvia the mutual information expansion. The resulting thermodynamicdensities satisfy key desiderata: their spatial integrals yield thecorrect total thermodynamic quantities, the densities vanish wherethe atomic number density is zero, and all entropy terms above firstorder go to zero in the absence of correlation. The entropy decompositionin GTM theory is closely related to that of IST, but it is simpler,largely because it expresses the entropy in terms of normalized probabilitydensity functions instead of nonnormalized correlation functions.We show that GTM theory is formally exact for any number of particles, <em>N</em>, whereas IST is not. The unified framework presented hereenables thermodynamic mapping of solute and solvent alike and is expectedto support a range of applications, including in structure-based drugdesign, protein design, the analysis of allostery, and materials science.The use of GTM theory to gain insight into protein-ligand bindingis illustrated here with an initial case study.</p>","PeriodicalId":60,"journal":{"name":"The Journal of Physical Chemistry B","volume":"130 40","pages":"10383–10402"},"PeriodicalIF":3.2,"publicationDate":"2026-10-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149124999","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-10-08Epub Date: 2026-09-26DOI: 10.1021/acs.jpcb.6c04316
Eudes Fileti, Davi Fileti, André P. L. de Carvalho, Débora Ariana C. da Silva, Shern Ren Tee, Dinis O. Abranches, João A. P. Coutinho
The Zn2+ coordination shell in ZnCl2-basedbattery electrolytes is far more dynamic than its time-averaged structuresuggests. Using a machine-learning force field (MACE) fine-tuned withdensity functional theory data, we simulate nanosecond-scale moleculardynamics of a ZnCl2:urea:H2O deep eutectic electrolyteacross 300–400 K, a time regime inaccessible to ab initio methods and poorly captured by classical force fields.The Zn2+ first coordination shell is tetrahedral and compositionallymixed with chloride ions, urea, and water contributing comparableshares. This overall occupancy remains essentially constant with temperature,masking markedly asymmetric underlying kinetics. Residence-time analysisreveals that chloride is essentially nonexchanging on the nanosecondtime scale, while water and urea exchange continuously, with residencetimes an order of magnitude shorter and activation energies of 12.5and 16.2 kJ/mol, respectively. Potential of mean force and speciationanalyses identify ZnCl2 as the dominant solute speciesand show that ligand substitution proceeds predominantly through anassociative pathway. Self-diffusion coefficients and activation energiesfor all four constituent species further establish a mobility hierarchyconsistent with this coordination picture. Together, these resultsprovide a molecular-level rationale for the transport behavior ofZnCl2-based electrolytes and a general framework for understandingion speciation and lability in coordinating eutectic battery electrolytes.
{"title":"Zn2+ Coordination and Ligand-Exchange Dynamics in a ZnCl2-Based Deep Eutectic Electrolyte from Machine-Learning Molecular Dynamics","authors":"Eudes Fileti, Davi Fileti, André P. L. de Carvalho, Débora Ariana C. da Silva, Shern Ren Tee, Dinis O. Abranches, João A. P. Coutinho","doi":"10.1021/acs.jpcb.6c04316","DOIUrl":"https://doi.org/10.1021/acs.jpcb.6c04316","url":null,"abstract":"<p>The Zn<sup>2+</sup> coordination shell in ZnCl<sub>2</sub>-basedbattery electrolytes is far more dynamic than its time-averaged structuresuggests. Using a machine-learning force field (MACE) fine-tuned withdensity functional theory data, we simulate nanosecond-scale moleculardynamics of a ZnCl<sub>2</sub>:urea:H<sub>2</sub>O deep eutectic electrolyteacross 300–400 K, a time regime inaccessible to <em>ab initio</em> methods and poorly captured by classical force fields.The Zn<sup>2+</sup> first coordination shell is tetrahedral and compositionallymixed with chloride ions, urea, and water contributing comparableshares. This overall occupancy remains essentially constant with temperature,masking markedly asymmetric underlying kinetics. Residence-time analysisreveals that chloride is essentially nonexchanging on the nanosecondtime scale, while water and urea exchange continuously, with residencetimes an order of magnitude shorter and activation energies of 12.5and 16.2 kJ/mol, respectively. Potential of mean force and speciationanalyses identify ZnCl<sub>2</sub> as the dominant solute speciesand show that ligand substitution proceeds predominantly through anassociative pathway. Self-diffusion coefficients and activation energiesfor all four constituent species further establish a mobility hierarchyconsistent with this coordination picture. Together, these resultsprovide a molecular-level rationale for the transport behavior ofZnCl<sub>2</sub>-based electrolytes and a general framework for understandingion speciation and lability in coordinating eutectic battery electrolytes.</p>","PeriodicalId":60,"journal":{"name":"The Journal of Physical Chemistry B","volume":"130 40","pages":"10582–10590"},"PeriodicalIF":3.2,"publicationDate":"2026-10-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149130631","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}