Thermal and Rheological Analysis of Polystyrene-Grafted Silica Nanocomposites
Two matrix-free polystyrene-grafted silica nanocomposite samples with graft chain lengths of 35 and 112 kg/mol are characterized by calorimetry and rheometry, and results are compared to neat polystyrenes of comparable molecular weights. The glass transition temperature T g of the nanocomposites is...
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Veröffentlicht in: | Macromolecules 2020-03, Vol.53 (6), p.2123-2135 |
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description | Two matrix-free polystyrene-grafted silica nanocomposite samples with graft chain lengths of 35 and 112 kg/mol are characterized by calorimetry and rheometry, and results are compared to neat polystyrenes of comparable molecular weights. The glass transition temperature T g of the nanocomposites is found to be approximately 1 to 2 K higher than that of the neat materials, whereas the absolute heat capacity is approximately 4–7% lower in the glassy and liquid states. The step change in heat capacity ΔC p at T g is 15% lower for the nanocomposites, consistent with an immobilized glassy layer of approximately 2 nm. The linear viscoelastic behavior of the nanocomposite samples differs significantly compared to their neat analogs in several ways: first, the G′ versus ω curves shift toward lower frequencies by approximately one decade due to the increase in the glass transition temperature; second, terminal flow behavior is absent; third, the rubbery plateau moduli (G N°) decreases by 7% for the 35 kg/mol grafted particles and increases by approximately two and a half-fold for the 112 kg/mol grafted particles; and fourth, the glassy modulus increases approximately 4% consistent with hydrodynamic reinforcement. On the other hand, the magnitude of the rubbery modulus is attributed to two effects, hydrodynamic reinforcement and a change in the effective entanglement density, which is governed by corona interpenetration coupled with the silica particles acting as physical entanglement points. |
doi_str_mv | 10.1021/acs.macromol.9b02127 |
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The glass transition temperature T g of the nanocomposites is found to be approximately 1 to 2 K higher than that of the neat materials, whereas the absolute heat capacity is approximately 4–7% lower in the glassy and liquid states. The step change in heat capacity ΔC p at T g is 15% lower for the nanocomposites, consistent with an immobilized glassy layer of approximately 2 nm. The linear viscoelastic behavior of the nanocomposite samples differs significantly compared to their neat analogs in several ways: first, the G′ versus ω curves shift toward lower frequencies by approximately one decade due to the increase in the glass transition temperature; second, terminal flow behavior is absent; third, the rubbery plateau moduli (G N°) decreases by 7% for the 35 kg/mol grafted particles and increases by approximately two and a half-fold for the 112 kg/mol grafted particles; and fourth, the glassy modulus increases approximately 4% consistent with hydrodynamic reinforcement. On the other hand, the magnitude of the rubbery modulus is attributed to two effects, hydrodynamic reinforcement and a change in the effective entanglement density, which is governed by corona interpenetration coupled with the silica particles acting as physical entanglement points.</description><identifier>ISSN: 0024-9297</identifier><identifier>EISSN: 1520-5835</identifier><identifier>DOI: 10.1021/acs.macromol.9b02127</identifier><language>eng</language><publisher>American Chemical Society</publisher><ispartof>Macromolecules, 2020-03, Vol.53 (6), p.2123-2135</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a399t-edceecf27f4fdc4fb27b631a87f771aeef9a64f3360b1b5556bbd612a3e71f553</citedby><cites>FETCH-LOGICAL-a399t-edceecf27f4fdc4fb27b631a87f771aeef9a64f3360b1b5556bbd612a3e71f553</cites><orcidid>0000-0003-4130-1232 ; 0000-0001-7498-2826 ; 0000-0002-2367-6199 ; 0000-0001-5831-502X ; 0000-0002-3991-6513</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://pubs.acs.org/doi/pdf/10.1021/acs.macromol.9b02127$$EPDF$$P50$$Gacs$$H</linktopdf><linktohtml>$$Uhttps://pubs.acs.org/doi/10.1021/acs.macromol.9b02127$$EHTML$$P50$$Gacs$$H</linktohtml><link.rule.ids>314,780,784,2765,27076,27924,27925,56738,56788</link.rule.ids></links><search><creatorcontrib>Sakib, Nazam</creatorcontrib><creatorcontrib>Koh, Yung P</creatorcontrib><creatorcontrib>Huang, Yucheng</creatorcontrib><creatorcontrib>Mongcopa, Katrina Irene S</creatorcontrib><creatorcontrib>Le, Amy N</creatorcontrib><creatorcontrib>Benicewicz, Brian C</creatorcontrib><creatorcontrib>Krishnamoorti, Ramanan</creatorcontrib><creatorcontrib>Simon, Sindee L</creatorcontrib><title>Thermal and Rheological Analysis of Polystyrene-Grafted Silica Nanocomposites</title><title>Macromolecules</title><addtitle>Macromolecules</addtitle><description>Two matrix-free polystyrene-grafted silica nanocomposite samples with graft chain lengths of 35 and 112 kg/mol are characterized by calorimetry and rheometry, and results are compared to neat polystyrenes of comparable molecular weights. The glass transition temperature T g of the nanocomposites is found to be approximately 1 to 2 K higher than that of the neat materials, whereas the absolute heat capacity is approximately 4–7% lower in the glassy and liquid states. The step change in heat capacity ΔC p at T g is 15% lower for the nanocomposites, consistent with an immobilized glassy layer of approximately 2 nm. The linear viscoelastic behavior of the nanocomposite samples differs significantly compared to their neat analogs in several ways: first, the G′ versus ω curves shift toward lower frequencies by approximately one decade due to the increase in the glass transition temperature; second, terminal flow behavior is absent; third, the rubbery plateau moduli (G N°) decreases by 7% for the 35 kg/mol grafted particles and increases by approximately two and a half-fold for the 112 kg/mol grafted particles; and fourth, the glassy modulus increases approximately 4% consistent with hydrodynamic reinforcement. 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The glass transition temperature T g of the nanocomposites is found to be approximately 1 to 2 K higher than that of the neat materials, whereas the absolute heat capacity is approximately 4–7% lower in the glassy and liquid states. The step change in heat capacity ΔC p at T g is 15% lower for the nanocomposites, consistent with an immobilized glassy layer of approximately 2 nm. The linear viscoelastic behavior of the nanocomposite samples differs significantly compared to their neat analogs in several ways: first, the G′ versus ω curves shift toward lower frequencies by approximately one decade due to the increase in the glass transition temperature; second, terminal flow behavior is absent; third, the rubbery plateau moduli (G N°) decreases by 7% for the 35 kg/mol grafted particles and increases by approximately two and a half-fold for the 112 kg/mol grafted particles; and fourth, the glassy modulus increases approximately 4% consistent with hydrodynamic reinforcement. On the other hand, the magnitude of the rubbery modulus is attributed to two effects, hydrodynamic reinforcement and a change in the effective entanglement density, which is governed by corona interpenetration coupled with the silica particles acting as physical entanglement points.</abstract><pub>American Chemical Society</pub><doi>10.1021/acs.macromol.9b02127</doi><tpages>13</tpages><orcidid>https://orcid.org/0000-0003-4130-1232</orcidid><orcidid>https://orcid.org/0000-0001-7498-2826</orcidid><orcidid>https://orcid.org/0000-0002-2367-6199</orcidid><orcidid>https://orcid.org/0000-0001-5831-502X</orcidid><orcidid>https://orcid.org/0000-0002-3991-6513</orcidid></addata></record> |
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title | Thermal and Rheological Analysis of Polystyrene-Grafted Silica Nanocomposites |
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