YuTian Zhu

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Name: 朱雨田; YuTian Zhu
Organization: Changchun Institute of Applied Chemistry, Chinese Academy of Sciences , China
Department: State Key Laboratory of Polymer Physics and Chemistry
Title: Associate Researcher/Professor(PhD)

TOPICS

Co-reporter:Jiangping Xu, Yutian Zhu, Jintao Zhu and Wei Jiang  
Nanoscale 2013 vol. 5(Issue 14) pp:6344-6349
Publication Date(Web):21 May 2013
DOI:10.1039/C3NR01296D
Ultralong cylindrical micelles impregnated with gold nanoparticles were fabricated via the convergence of a surface-templated self-assembly method and the fragmentation of gold nanowires driven by Rayleigh instability. This approach could be proposed as an unconventional method for the fabrication of hybrid nanomaterials.
Co-reporter:Yuping Sheng, Xiaoping Yang, Nan Yan and Yutian Zhu  
Soft Matter 2013 vol. 9(Issue 27) pp:6254-6262
Publication Date(Web):04 Jun 2013
DOI:10.1039/C3SM00029J
Janus particles with two different compartments have enormous potential as building blocks of hierarchically multifunctional nanomaterials. One of the most versatile and powerful methods to fabricate Janus micelles is through the solution-state self-assembly of block copolymers. In this study, we applied the Monte Carlo simulation to study the self-assembly of a AB/BC diblock copolymer mixture in A- and C-selective solvents. Our simulations predicted a variety of novel Janus micelles, which include Janus-like cylinders, lamellas, vesicles, and rings, all of which were self-assembled from amphiphilic A4B6/B6C4 copolymers. The effects of control parameters, which include the solvent quality for solvophobic B blocks (εBS) and the incompatibility between the solvophilic A and C blocks (εAC), on the formation of Janus micelles were examined, and a generic phase diagram in εBS × εAC was constructed. The phase diagram demonstrates that the micellar shape mainly depends on εBS, whereas the formation of the Janus architecture is controlled by εAC. Moreover, the formation pathways of the Janus lamella, vesicle, and ring were investigated and their formation mechanisms were investigated.
Co-reporter:Xiaoping Yang, Yutian Zhu, Yongmei Wang
Polymer 2013 Volume 54(Issue 14) pp:3730-3736
Publication Date(Web):21 June 2013
DOI:10.1016/j.polymer.2013.05.018
Liquid chromatography at the critical condition (LCCC) method has been proposed as an attractive method to characterize individual blocks in block copolymers because it can make one block chromatographically “invisible” at the critical condition of its corresponding homopolymer. However, observable dependence of retention time on the “invisible” block length was reported in LCCC experimental studies of diblock copolymer [Macromolecules 2001;34:2353–2358; Anal Chem 2001;73:3884–3889.]. In this study, we re-examined the validity of the LCCC method for AB, BAB and ABA block copolymers by the lattice Monte Carlo simulation method with using random walk (RW) and self-avoiding walk chain (SAW) models. In the current study, the A block is set in the size exclusion mode and is chromatographically “visible”. The interaction between the B type monomer and the column surface are varied to identify the critical condition of B block in the block copolymer. Our simulation results establish that individual block, i.e. B block in the current work, from the block copolymer has its own critical condition for the first time. However, it was also found that the critical condition of B block might be different from the critical condition of B homopolymer. The critical condition of B block in the AB diblock is exactly equal to the critical condition of B homopolymer only when the chain is modeled by RW model. However, deviations of the critical condition of B block away from that of the B homopolymer are observed for AB copolymer using SAW model, and also for BAB and ABA copolymers whether the chain is modeled by RW or SAW models. Moreover, under the critical condition of B homopolymer, no dependence of the partition coefficient on the “invisible” B block length was observed for the AB and BAB copolymers when the copolymer chains were modeled by RW model. Distinct dependence of the partition coefficient of these two types' copolymers on the B block length was found when the chain was modeled by SAW model. For the ABA triblock copolymer, slight dependence of the partition coefficient on B block length was observed even for the RW model while this dependence became much stronger when the chain was modeled by SAW model. Moreover, it was also found that the partition coefficient of ABA copolymer is much smaller than those of AB and BAB copolymers under the critical condition of B homopolymer because of the chain architecture effect. The current study confirms that the block in the block copolymer is hard to be made completely chromatographically “invisible” because the intrinsic nature of the excluded volume interaction existed in real polymer system.
Co-reporter:Cui Mao, Jinrui Huang, Yutian Zhu, Wei Jiang, Qingxin Tang, and Xiaojing Ma
The Journal of Physical Chemistry Letters 2013 Volume 4(Issue 1) pp:43-47
Publication Date(Web):December 11, 2012
DOI:10.1021/jz301811b
We present a simple but efficient route to prepare a highly anisotropic conductive plastic thin film from the polypropylene/(styrene-ethylene/butadiene-styrene) triblock copolymer/graphene blend via shear-induced self-assembly. Under the shear-flow induction, GE nanosheets dispersed in the polymer matrix can spontaneously assemble into ordered parallel stripes, which endow the materials significantly conductive anisotropy. The electrical resistivity in the direction parallel to the graphene stripes is almost four orders of magnitude lower than that which is perpendicular to the stripes. This study provides a new method for the precise control of the organization of functional nano-objects in polymer matrix, which can be widely extended to the fabrication of other multifunctional anisotropic materials of interest in various fields.Keywords: conductive anisotropy; graphene; self-assembly; shear flow; thin films;
Co-reporter:Cui Mao, Yutian Zhu, and Wei Jiang
ACS Applied Materials & Interfaces 2012 Volume 4(Issue 10) pp:5281
Publication Date(Web):September 5, 2012
DOI:10.1021/am301230q
Polystyrene (PS) and poly(methyl methacrylate) (PMMA) blends filled with octadecylamine-functionalized graphene (GE-ODA) have been fabricated to obtain conductive composites with a lower electrical percolation threshold according to the concept of double percolation. The dependence of the electrical properties of the composites on the morphology is examined by changing the proportion of PS and PMMA. Our results reveal that the electrical conductivity of the composites can be optimal when PS and PMMA phases form a cocontinuous structure and GE-ODA nanosheets are selectively located and percolated in the PS phase. For the PS/PMMA blend (50w/50w), the composites exhibit an extremely low electrical percolation threshold (0.5 wt %) because of the formation of a perfect double percolated structure. Moreover, the rheological properties of the composites are also measured to gain a fundamental understanding of the relationship between microstructure and electrical properties.Keywords: double percolation; electrical properties; functionalized graphene; immiscible polymer blends; rheological properties;
Co-reporter:Yutian Zhu, Haizhou Yu, Yongmei Wang, Jie Cui, Weixin Kong and Wei Jiang  
Soft Matter 2012 vol. 8(Issue 17) pp:4695-4707
Publication Date(Web):09 Mar 2012
DOI:10.1039/C2SM07324B
In the current study, we applied the Monte Carlo method to study the self-assembly of linear ABC amphiphiles composed of two solvophobic A and B blocks and a solvophilic C block. A great number of multicompartment micelles are discovered from the simulations and the detailed phase diagrams for the ABC amphiphiles with different block lengths are obtained. The simulation results reveal that the micellar structure is largely controlled by block length, solvent quality, and incompatibility between the different block types. When the B block is longer than or as same as the terminal A block, a rich variety of micellar structures can be formed from ABC amphiphiles. By adjusting the solvent quality or incompatibility between the different block types, multiple morphological transitions are observed. These morphological sequences are well explained and consistent with all the previous experimental and theoretical studies. Despite the complexity of the micellar structures and morphological transitions observed for the self-assembly of ABC amphiphiles, two important common features of the phase behavior are obtained. In general, the micellar structures obtained in the current study can be divided into zero-dimensional (sphere-like structures, including bumpy-surfaced spheres and sphere-on-sphere structures), one-dimensional (cylinder-like structures, including rod and ring structures), two-dimensional (layer-like structures, including disk, lamella and worm-like and hamburger structures) and three-dimensional (vesicle) structures. It is found that the micellar structures transform from low- to high- dimensional structures when the solvent quality for the solvophobic blocks is decreased. In contrast, the micellar structures transform from high- to low-dimensional structures as the incompatibility between different block types increases. Furthermore, several novel micellar structures, such as the CBABC five-layer vesicle, hamburger, CBA three-layer ring, wormlike shape with bumps on the sides, and disk shape with bumps on the edge, are predicted in this study. The formation pathways of ring, hamburger, and worm-like micelles are also examined and their formation mechanisms are well elucidated.
Co-reporter:Nan Yan;Xiaoping Yang;Jiangping Xu;Yuping Sheng
Macromolecular Chemistry and Physics 2012 Volume 213( Issue 21) pp:2261-2266
Publication Date(Web):
DOI:10.1002/macp.201200354

Abstract

In this study, we developed a novel blending strategy, namely, the gradual blending method, to tune the micellar structure. Different from the most commonly used premixing blending method, which different block copolymers are premixed in a common solvent before their individual self-assembly, the gradual blending method involves gradually adding one type of block copolymer into the pre-generated micellar solution formed from another type of block copolymer. Moreover, we obtained a novel mesh-like vesicle from the self-assembly of the mixtures of P4VP43-b-PS260-b-P4VP43 and P4VP43-b-PS366-b-P4VP43 in 1,4-dioxane/water solution using the gradual blending method.

Co-reporter:Weixin Kong, Wei Jiang, Yutian Zhu, and Baohui Li
Langmuir 2012 Volume 28(Issue 32) pp:11714-11724
Publication Date(Web):July 17, 2012
DOI:10.1021/la3014943
Multicompartment micelles, especially those with highly symmetric surfaces such as patchy-like, patchy, and Janus micelles, have tremendous potential as building blocks of hierarchical multifunctional nanomaterials. One of the most versatile and powerful methods to obtain patchy multicompartment micelles is by the solution-state self-assembly of linear triblock copolymers. In this article, we applied the simulated annealing method to study the self-assembly of ABC linear terpolymers in C-selective solvents. Simulations predict a variety of patchy and patchy-like multicompartment micelles with high symmetry and also yield a detailed phase diagram to reveal how to control the patchy multicompartment micelle morphologies precisely. The phase diagram demonstrates that the internal segregated micellar structure depends on the ratio between the volume fractions of the two solvophobic blocks and their incompatibility, whereas the overall micellar shape depends on the copolymer concentration. The relationship between the interfacial energy, stretching energy of chains and the micellar morphology, micellar morphological transition are elucidated by computing the average contact number among the species, the mean square end-to-end distances of the whole terpolymers, the AB blocks in the terpolymers, the AB diblock copolymers, and angle distribution of terpolymers. The anchoring effect of the solvophilic C block on micellar structures is also examined by comparing the morphologies formed from ABC terpolymers and AB diblock copolymers.
5H-Benzo[a]phenoxazin-5-one,9-(diethylamino)-
Poly(l-lactide)
Poly[oxy[(1S)-1-methyl-2-oxo-1,2-ethanediyl]]
Poly[oxy(1-oxo-1,6-hexanediyl)]