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Projectile Impact Shock-Induced Deformation of One-Component Polymer Nanocomposite Thin Films.
Hyon, Jinho; Gonzales, Manny; Streit, Jason K; Fried, Omri; Lawal, Olawale; Jiao, Yang; Drummy, Lawrence F; Thomas, Edwin L; Vaia, Richard A.
Affiliation
  • Hyon J; Department of Materials Science & NanoEngineering, Rice University, Houston, Texas 77005, United States.
  • Gonzales M; Department of Materials Science and Engineering, Texas A&M University, College Station, Texas 77840, United States.
  • Streit JK; Materials and Manufacturing Directorate, Air Force Research Laboratory, Wright Patterson Air Force Base, Dayton, Ohio 45433-7750, United States.
  • Fried O; Materials and Manufacturing Directorate, Air Force Research Laboratory, Wright Patterson Air Force Base, Dayton, Ohio 45433-7750, United States.
  • Lawal O; Department of Materials Science & NanoEngineering, Rice University, Houston, Texas 77005, United States.
  • Jiao Y; Department of Materials Science & NanoEngineering, Rice University, Houston, Texas 77005, United States.
  • Drummy LF; United States Air Force Academy, Colorado Springs, Colorado 80840, United States.
  • Thomas EL; Materials and Manufacturing Directorate, Air Force Research Laboratory, Wright Patterson Air Force Base, Dayton, Ohio 45433-7750, United States.
  • Vaia RA; Materials and Manufacturing Directorate, Air Force Research Laboratory, Wright Patterson Air Force Base, Dayton, Ohio 45433-7750, United States.
ACS Nano ; 15(2): 2439-2446, 2021 Feb 23.
Article in En | MEDLINE | ID: mdl-33503365
ABSTRACT
Matrix-free assemblies of polymer-grafted nanoparticles (PGNs) enable mechanically robust materials for a variety of structural, electronic, and optical applications. Recent quasi-static mechanical studies have identified the key parameters that enhance canopy entanglement and promote plasticity of the PGNs below Tg. Here we experimentally explore the high-strain-rate shock impact behavior of polystyrene grafted NPs and compare their energy absorption capabilities to that of homopolystyrene for film thicknesses ranging from 75 to 550 nm and for impact velocities from 350 to 800 m/s. Modeling reveals that the initial shock compression results in a rapid temperature increase at the impact site. The uniformity of this heating is consistent with observations of greater kinetic energy absorption per mass (Ep*) of thinner films due to extensive visco-plastic deformation of molten film around the penetration site. Adiabatic heating is insufficient to raise the temperature at the exit surface of the thickest films resulting in increased strain localization at the impact periphery with less melt elongation. The extent and distribution of entanglements also influence Ep*. Structurally, each NP acts as a giant cross-link node, coupling surrounding nodes via the number of canopy chains per NP and the nature and number of entanglements between canopies anchored to different NPs. Load sharing via this dual network, along with geometrical factors such as film thickness, lead to extreme Ep* arising from the sequence of instantaneous adiabatic shock heating followed by visco-plastic drawing of the film by the projectile. These observations elucidate the critical factors necessary to create robust polymer-nanocomposite multifunctional films.
Key words

Full text: 1 Collection: 01-internacional Database: MEDLINE Type of study: Prognostic_studies Language: En Journal: ACS Nano Year: 2021 Document type: Article Affiliation country: Estados Unidos

Full text: 1 Collection: 01-internacional Database: MEDLINE Type of study: Prognostic_studies Language: En Journal: ACS Nano Year: 2021 Document type: Article Affiliation country: Estados Unidos