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碳纳米材料是指分散相尺度至少有一维小于100 nm的碳材料,包括碳纳米管(CNT)、石墨烯、富勒烯等。近年来,碳纳米材料在氟橡胶(FKM)中的应用日益广泛。综述了FKM/石墨烯、FKM/CNT、FKM/碳纳米带等纳米复合材料的结构和性能,并对FKM/碳纳米复合材料的发展进行了展望。 相似文献
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一维纳米材料具有优良的尺寸效应,一维贵金属材料表现出不同于相应块体材料的特殊物理化学性能。本文以一维贵金属纳米结构的合成方法和机理为探讨重点,总结了近年来国内外用于控制合成一维贵金属纳米材料的主要方法,包括模板法、多元醇还原法、化学电沉积法以及金属催化还原法。着重以金属银、钯为例,介绍了其形状可控的一维纳米结构的生长机理,并以金、银等一维纳米材料为例介绍了其一维纳米结构在功能材料以及生物医学等领域的应用前景。指出建立一维金属纳米结构制备科学的新理论、新方法及其成核生长动力学模型是进一步研究的方向。 相似文献
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钛酸钡是新发现的场发射材料.为了开发适用于曲面显示和折叠屏显示器件的新型柔性场发射材料,建立钛酸钡一维纳米材料基本研究体系,通过调节水热法的工艺参数制备了一维钛酸钡纳米材料,进一步采用溶胶-凝胶和水热两步法制备了以柔性碳布为衬底的一维钛酸钡纳米材料,研究纳米棒的生长演化规律,筛选工艺指标,以期达到优化场发射性能的目的. 相似文献
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一维纳米材料是指仅长度为宏观尺度,其他方向为纳米尺度的新型材料,在光电子、生物医用、纳米传感、纳米储能等诸多领域具有潜在的应用前景,已成为21世纪化学、物理学、材料学及生命科学等科技领域的研究热点。本文介绍了一维纳米材料的制备方法,阐述了一维纳米材料各种生长机理,总结了一维纳米材料的表征方法,及在物理、化学、机械、材料等领域的应用。 相似文献
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Xiaolian Qiang Ramzi Chakroun Nicole Janoszka Andr H. Grschel 《Israel journal of chemistry》2019,59(10):945-958
Block copolymers (BCPs) are a subclass of soft matter extensively used in materials science and nanomedicine. They consist of two or more incompatible segments and are prone to self‐assemble into nanostructures with a characteristic size of 10–100 nm. BCPs thus naturally address the structural dimension between molecular and colloidal scales. This review gives a brief overview of recent developments in BCP self‐assembly under various conditions. Special emphasis is put on linear BCPs with three or more sequentially linked blocks, i. e. ABC triblock terpolymers, ABAC tetrablock terpolymers, and so on. We discuss their microphase separation in bulk, in the confinement of nanoemulsion droplets, and their hierarchical self‐assembly to multicompartment nanostructures in selective solvents. Regarding applications, block copolymers are widely used in templating and drug delivery, but their inherent asymmetry is also particularly useful for the synthesis of Janus nanoparticles. 相似文献
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Yi-Fang Huang Yan-Wei Chian Jrjeng Ruan Shi Jin Kwang-Un Jeong Horng-Yi Tang An-Chung Su 《Polymer》2011,52(18):4114-4122
For a designed LC homopolymer, bearing a polyimide backbone mesogen and two terminally-connected cyanobiphenyl mesogens via aliphatic spacers in a repeat unit, the formation of layer-type supramolecular nanostructures, and involved organization route within sheared film have been studied in this research. The anisotropic layer scheme induced within sheared film identified the feasible phase separation between distinct mesogens under the restriction of connection spacers. Further considering the periodic correlation of 2.3 nm preferably along the stacking direction, alternate stacks of mesogen bilayers were accounted for the growth of nanostructures. The shear-aligned assembly of layer-type nanostructures led to the presence of orientational order along the film x- and z-axes, and thus the formation of biaxial supramolecular nematic phase. The further annealing process at 160 °C initiated the development of orthorhombic lattice packing, which is conceivably via parallel sliding motion of nanostructures. This growth mechanism explains the existence of large range of bond orientation order, but less extensive positional order. For this orthorhombic lattice, the preferred azimuthal orientation and unusually high aspect ratio between transverse lattice dimensions approved the development of lattice packing from prior stacking of layer-type nanostructures. Upon annealing at 240 °C, the continue ordering process favored closer interaction between neighboring backbone mesogens along the b-axis, which nevertheless expanded the a-axis dimension and caused the packing of cyanobiphenyl mesogens much less oriented. These evolved structural features were attributed to the presence of a regular buckled pattern of cyanobiphenyl bilayers within lattices, as a result of mechanical deformation while being unable to linearly extend within insufficient lattice dimension. These structural analyses helps to describe multiple-step organization of layer-type nanostructures toward lattice packing, which is not likely referred to the packing behavior of individual repeat units. 相似文献
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对PET厂液相热媒系统作了讨论。针对一个热媒站供2套PET装置的情况进行重点分析,提出2套PET装置相互影响下调整液相热媒系统以稳定生产的注意要点及调整方向。 相似文献
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Crystalline Gaq3 1-D nanostructures and nanospheres could be fabricated by thermal evaporation under cold trap. The influences of the key
process parameters on formation of the nanostructures were also investigated. It has been demonstrated that the morphology
and dimension of the nanostructures were mainly controlled by working temperature and working pressure. One-dimensional nanostructures
were fabricated at a lower working temperature, whereas nanospheres were formed at a higher working temperature. Larger nanospheres
could be obtained when a higher working pressure was applied. The XRD, FTIR, and NMR analyses evidenced that the nanostructures
mainly consisted of δ-phase Gaq3. Their DSC trace revealed two small exothermic peaks in addition to the melting endotherm. The one in lower temperature region
was ascribed to a transition from δ to β phase, while another in higher temperature region could be identified as a transition
from β to δ phase. All the crystalline nanostructures show similar PL spectra due to absence of quantum confinement effect.
They also exhibited a spectral blue shift because of a looser interligand spacing and reduced orbital overlap in their δ-phase
molecular structures. 相似文献
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Surface energies of nanostructures are of considerable interest, and thermodynamic methods have provided valuable insight into the physics and chemistry of these systems. Although the effect of surface energy on melting behaviors of nanostructures has been widely investigated in theoretical calculations and simulations, from the thermodynamics at the nanometer scale point of view, the comprehensive understanding of the fundamental physical and chemical issues involved in nanostructures' melting is still lacking. For instance, nanostructures with negative curvature, such as nanotubes, show different melting behaviors compared with the nanostructures with positive curvature such as nanowires, and both nanotubes and nanowires exhibit abnormal melting temperature compared with that of the bulk counterparts. Herein, we put forward a general model to elucidate the melting temperature of the nanostructures with positive and negative curvatures based on the surface energy at the nanometer. Further, the surface mean square relative atomic displacement (MSRD) of these nanostructures has been studied from the perspective of the size-dependent cohesive energy consideration, which can provide the atomic understanding of the nanostructures' melting. Theoretical analyses indicate that both melting temperatures of the nanostructures with the positive and negative curvatures decrease with decreasing dimensionality, and the surface MSRDs show different size effects in the systems with the positive and negative curvatures, respectively. The melting temperature of the surface with the negative curvature is higher than that of the surface with the positive curvature, and both melting temperatures are smaller than that of the bulk counterpart when the size of nanostructures is less than a threshold value. The unique melting behaviors of nanostructures are attributed to the size- and curvature-dependent surface energy of nanostructures. These results provide new insight into the fundamental understanding of the melting temperature of nanostructures. 相似文献
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