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Polystyrene Chain Geometry Probed by Ion Mobility Mass Spectrometry and Molecular Dynamics Simulations
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    Polystyrene Chain Geometry Probed by Ion Mobility Mass Spectrometry and Molecular Dynamics Simulations
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    • Sarajit Naskar
      Sarajit Naskar
      Organic Synthesis and Mass Spectrometry Laboratory, Center of Innovation and Research in Materials and Polymers (CIRMAP), University of Mons - UMONS, 23 Place du Parc, B-7000 Mons, Belgium
      Center for Materials Science, School of Chemistry and Physics, Queensland University of Technology (QUT), 2 George Street, Brisbane, Queensland 4000, Australia
      Laboratory for Chemistry of Novel Materials, Center of Innovation and Research in Materials and Polymers (CIRMAP), University of Mons - UMONS, 23 Place du Parc, B-7000 Mons, Belgium
    • Andrea Minoia
      Andrea Minoia
      Laboratory for Chemistry of Novel Materials, Center of Innovation and Research in Materials and Polymers (CIRMAP), University of Mons - UMONS, 23 Place du Parc, B-7000 Mons, Belgium
    • Quentin Duez
      Quentin Duez
      Organic Synthesis and Mass Spectrometry Laboratory, Center of Innovation and Research in Materials and Polymers (CIRMAP), University of Mons - UMONS, 23 Place du Parc, B-7000 Mons, Belgium
      More by Quentin Duez
    • Aidan Izuagbe
      Aidan Izuagbe
      Center for Materials Science, School of Chemistry and Physics, Queensland University of Technology (QUT), 2 George Street, Brisbane, Queensland 4000, Australia
    • Julien De Winter
      Julien De Winter
      Organic Synthesis and Mass Spectrometry Laboratory, Center of Innovation and Research in Materials and Polymers (CIRMAP), University of Mons - UMONS, 23 Place du Parc, B-7000 Mons, Belgium
    • Stephen J. Blanksby
      Stephen J. Blanksby
      Center for Materials Science, School of Chemistry and Physics, Queensland University of Technology (QUT), 2 George Street, Brisbane, Queensland 4000, Australia
    • Christopher Barner-Kowollik
      Christopher Barner-Kowollik
      Center for Materials Science, School of Chemistry and Physics, Queensland University of Technology (QUT), 2 George Street, Brisbane, Queensland 4000, Australia
    • Jérôme Cornil
      Jérôme Cornil
      Laboratory for Chemistry of Novel Materials, Center of Innovation and Research in Materials and Polymers (CIRMAP), University of Mons - UMONS, 23 Place du Parc, B-7000 Mons, Belgium
    • Pascal Gerbaux*
      Pascal Gerbaux
      Organic Synthesis and Mass Spectrometry Laboratory, Center of Innovation and Research in Materials and Polymers (CIRMAP), University of Mons - UMONS, 23 Place du Parc, B-7000 Mons, Belgium
      *Email: [email protected]
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    Journal of the American Society for Mass Spectrometry

    Cite this: J. Am. Soc. Mass Spectrom. 2024, 35, 10, 2408–2419
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    https://doi.org/10.1021/jasms.4c00231
    Published September 15, 2024
    Copyright © 2024 American Society for Mass Spectrometry. Published by American Chemical Society. All rights reserved.

    Abstract

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    Polystyrene (PS) is a thermoplastic polymer commonly used in various applications due to its bulk properties. Designing functional polystyrenes with well-defined structures for targeted applications is of significant interest due to the rigid and apolar nature of the polymer chain. Progress is hindered to date by the limitations of current analytical methods in defining the atomistic-level folding of the polymer chain. The integration of ion mobility spectrometry and molecular dynamics simulations is beneficial in addressing these challenges. However, data on gas-phase polystyrene ions are rarely reported in the literature. We herein investigate the gas phase structure of polystyrene ions with different end groups to establish how the nature and the rigidity of the monomer unit affect the charge stabilization. We find that, in contrast to polar polymers in which the charges are located deep in the ionic globules, the charges in the PS ions are rather located at the periphery of the polymer backbone, leading to singly and doubly charged PS ions adopting dense elliptic-shaped structures. Molecular dynamics (MD) simulations indicate that the folding of the PS rigid chain is controlled by phenyl ring interactions with the charge ultimately remaining excluded from the core of the globular ions, whereas the folding of polyether ions is initiated by the folding of the flexible polyether chain around the sodium ion that remains deeply enclosed in the core of the ions.

    Copyright © 2024 American Society for Mass Spectrometry. Published by American Chemical Society. All rights reserved.

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    Supporting Information

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    The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/jasms.4c00231.

    • Preparation and characterization (including size exclusion chromatography, nuclear magnetic resonance, MALDI-Tof analysis) of the TEMPO-PS sample; MALDI-ToF analysis of the BU-PSLM/HM samples; electrospray mass spectra of TEMPO-PS and BU-PS; complete set of ion mobility and molecular dynamics data on TEMPO-PS and BU-PS ions; DFT calculations to establish the protonation center on TEMPO-PS and to establish the cation-π interactions between 3 benzene rings and a silver ion; and selected MD snapshots of PEG ions, BU-PS ions, and TEMPO-PS ions (PDF)

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    Journal of the American Society for Mass Spectrometry

    Cite this: J. Am. Soc. Mass Spectrom. 2024, 35, 10, 2408–2419
    Click to copy citationCitation copied!
    https://doi.org/10.1021/jasms.4c00231
    Published September 15, 2024
    Copyright © 2024 American Society for Mass Spectrometry. Published by American Chemical Society. All rights reserved.

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