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2023
DOI: 10.1039/d3sm00044c
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Relatively homogeneous network structures of temperature-responsive gels synthesized via atom transfer radical polymerization

Abstract: The network structures of poly(N-isopropylacrylamide) (PNIPAAm) gels prepared by atom transfer radical polymerization (ATRP) were compared with those prepared by free radical polymerization (FRP), as a conventional radical polymerization. Temperature-responsive...

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Cited by 4 publications
(4 citation statements)
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“…Typically, the complex network topology results in a static < I > s and fluctuating < I > f components of the scattered electric field of nonergodic network. Using nonergodic analysis and the partial heterodyne method, [ 2,81–90 ] the apparent diffusion coefficient, D A , is determined from the exponential decay of the time‐averaged intensity correlation, which is written as Equation g2(τ)badbreak≡〈〉Ifalse(tfalse)Ifalse(t+τfalse)T〈〉Ifalse(tfalse)T2goodbreak=1goodbreak+Xg1false(τfalse)2goodbreak+2X(1X)g1(τ)$$\begin{equation}{g}_2(\tau ) \equiv \frac{{{{\left\langle {I(t)I(t + \tau )} \right\rangle }}_T}}{{{{\left\langle {I(t)} \right\rangle }}_T^2}} = 1 + {\left[ {X{g}_1(\tau )} \right]}^2 + 2X(1 - X){g}_1(\tau )\end{equation}$$where X is the ratio < I > f /(< I > f + < I > s ) and g 1 (τ) is the fluctuating component of the field correlation function. This ratio, X , can be determined from the initial amplitude of the time–intensity correlation function, σ 2 ≡ g 2 (0) − 1 = X (2 − X ).…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Typically, the complex network topology results in a static < I > s and fluctuating < I > f components of the scattered electric field of nonergodic network. Using nonergodic analysis and the partial heterodyne method, [ 2,81–90 ] the apparent diffusion coefficient, D A , is determined from the exponential decay of the time‐averaged intensity correlation, which is written as Equation g2(τ)badbreak≡〈〉Ifalse(tfalse)Ifalse(t+τfalse)T〈〉Ifalse(tfalse)T2goodbreak=1goodbreak+Xg1false(τfalse)2goodbreak+2X(1X)g1(τ)$$\begin{equation}{g}_2(\tau ) \equiv \frac{{{{\left\langle {I(t)I(t + \tau )} \right\rangle }}_T}}{{{{\left\langle {I(t)} \right\rangle }}_T^2}} = 1 + {\left[ {X{g}_1(\tau )} \right]}^2 + 2X(1 - X){g}_1(\tau )\end{equation}$$where X is the ratio < I > f /(< I > f + < I > s ) and g 1 (τ) is the fluctuating component of the field correlation function. This ratio, X , can be determined from the initial amplitude of the time–intensity correlation function, σ 2 ≡ g 2 (0) − 1 = X (2 − X ).…”
Section: Resultsmentioning
confidence: 99%
“…Typically, the complex network topology results in a static <I> s and fluctuating <I> f components of the scattered electric field of nonergodic network. Using nonergodic analysis and the partial heterodyne method, [2,[81][82][83][84][85][86][87][88][89][90] the apparent diffusion coefficient, D A , is determined from the exponential decay of the time-averaged intensity correlation, which is written as Equation 12g 2 (𝜏) ≡ ⟨I(t)I(t…”
Section: Resultsmentioning
confidence: 99%
“…Additionally, this may have an impact on the polymer's resistance, toughness, elasticity, viscosity, solubility, glass transition temperature (T g ), and melting point [56]. Because links prevent rotational movement between polymer chains, cross-linked polymers have a greater T g , and the molecular mobility nature is often assessed using the T g [46,[56][57][58]. Moreover, cross-linking makes the polymer chains heavier molecularly and less mobile, reducing the polymer's solubility.…”
Section: Hydrogel Preparationmentioning
confidence: 99%
“…Nevertheless, Sakai and other research groups ,, have conducted numerous studies to synthesize ordered cross-linked networks using precisely synthesized star-shaped polymers of uniform molecular weight as building blocks. They have achieved relatively highly ordered network structures.…”
Section: Introductionmentioning
confidence: 99%