Introduction to Polymer Physics.ppt
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1、Introduction to Polymer Physics,Prof. Dr. Yiwang Chen School of Materials Science and Engineering, Nanchang University, Nanchang 330047,Chapter 2 Solid-state properties,2.1 Interaction of Molecules in Polymer van der Waals forces and Hydrogen bonding Static force is the force between polar molecules
2、 All polar molecules have permanent dipolar moment. The strength of static force between permanent dipoles depends on strength of dipolar moment and orientation degree. The interactional potential between two polar molecules with dipolar moment 1 and 2, and R of distance is:k is the Boltzman constan
3、t and T is temperatureStatic force usually ranges from 13 to 21 kJ/mol,Induced force is the interactional force between the permanent dipole of polar molecule and induced dipolar moment of another molecule induced by polar molecule. For two molecules with dipolar moment 1 and 2, and polarizability o
4、f 1 和 2, their interactional potential is:Induced force usually ranges from 6 to13 kJ/mole,Chromoscatter force is the interaction of instant dipolar moments of molecules. It depends on ionization energy I, polarizability , and inter-distance R:It usually ranges from 0.8 to 8 kJ/mole,以上三种力统称范德华力,永久存在
5、于一切分子之间的一种吸引力。这种吸引力没有方向性和饱和性。作用范围小于1纳米,作用能约比化学键小12个数量级。,氢键是极性很强的XH键上的氢原子,与另一个键上电负性很大的原子Y上的孤对电子相互吸引而形成的一种键(XH-Y)。,氢键有饱和性和方向性,氢键与化学键相似,键能比化学键小得多,不超过40千焦/摩尔。,Cohesive Energy Density,在高聚物中,由于分子量很大,分子链很长,分子间的作用力很大,高分子的聚集态只有固态(晶态和非晶态)和液态,没有气态。 高聚物分子间作用力的大小通常采用内聚能或内聚能密度来表示。内聚能定义为克服分子间的作用力,把一摩尔液体或固体分子移到其分子间
6、的引力范围之处所需要的能量:E是内聚能,Hv是摩尔蒸发热(或摩尔升华热Hs),RT是转化为气体时所做的膨胀功。内聚能密度(Cohesive Energy Density)是单位体积的内聚能:为摩尔体积对于低分子化合物,其内聚能近似等于恒容蒸发热或升华热,可直接由热力学数据估计其内聚能密度,而高聚物不能气化,不能直接测定它的内聚能,只能用低分子溶剂相比较的办法进行估计。,2.2 The Amorphous state,Completely amorphous polymers like atactic polystyrene exist as long, randomly coiled, int
7、erpenetrating chains that are capable of forming stable, flow-restricting entanglements at sufficiently high-molecular-weight. In the melt, thermal energy is sufficiently high for long segments of each polymer chain to move in random micro-Brownian motions. As the melt is cooled, a temperature is re
8、ached at which all long-range segmental motions ceases. The characteristic temperature is called the glass-transition temperature, Tg. In the glassy state, at temp below Tg, the only molecular motions that can occur are short-range motions of several contiguous chain segments and motions of substitu
9、ent groups. These processes are called secondary relaxations.,Chain Entanglements and Reptation Polymer chains that are sufficiently long can form stable, flow-restricting entanglements. A good analogy can be made to a bowl of spaghetti. Entanglements have significant importance in relation to visco
10、elastic properties, melt viscosity, and mechanical properties such as stress relaxation, creep, and craze formation.,In the melt state, individual polymer chains can move by local Brownian motion restricted by the topological constraint of neighboring chains. Movement can be visualized as snakelike
11、motion (i.e., reptation) of the chain within a virtual tube.,2.3 The Crystalline state,Ordering of Polymer Chains Under favorable conditions, some polymers cooled from the melt can organize into regular crystalline structures. Such crystalline polymers have less perfect organization than crystals of
12、 low-molecular-weight compounds or low-molecular-weight polymers crystallized from the solution.,The basic units of crystalline polymer morphology include crystalline lamellae consisting of arrays of folded chains. Reentry of each chain in the folded structure can be adjacent or nonadjacent. A chain
13、 participating in adjacent reentry can form a tight (or regular) loop or form a loose (irregular) loop. The thickness of typical crystallite may be only 0.1 to 0.2 nm, indicating that only a portion of the complete chain (e.g., 40 to 80 repeating units in the case of polyethylene) is involved in eac
14、h fold.,For some polymers crystallized from the melt for from concentrated solution, crystallites can organize into large spherical structures called spherulites. Each spherulite contains arrays of lamellar crystallites that are typically oriented with the chain axis perpendicular to the radial (gro
15、wth) direction of the spherulite. In a few cases, such as occurs in the crystallization of polypropylene, chain folding will occur with the chain oriented along the radial direction.,球晶 (Spherulites):球晶是由无数微小晶片按结晶生长规律长在一起的多晶聚集体。球晶的直径可以达到0.5至100微米,大的可以达到厘米数量级。球晶中分子链总是垂直于分子链球晶的半径方向。这说明球晶的基本结构单元仍然是具有折叠
16、链结构的片晶。以一定的方式扭曲,同时从一个中心向四面八方生长,发展成为一个球状的多晶聚集体。,球晶是由径向发射的微纤(fibrils)组成的,这些微纤就是长条状的晶片,其厚度在 10 20 纳米之间。,The anisotropic morphology of a spherulite results in the appearance of a characteristic extinction cross, or Maltese cross, when viewed under polarized light.,Conformations of Polymer Crystallite Hi
17、gh thermal energy favors a large number of conformations in the melt. As the melt is cooled, the lower-energy conformations are favored, and chains are free to organize into lamellar structure. For many polymers, the lowest-energy conformation is the extended chain or planar zigzag conformation. Suc
18、h polymers include polyethylene, syndiotactic vinyl polymers, and polymers capable of hydrogen bonding between chains, such as poly(vinyl alcohol) and nylons.,In cases of polymers with large substituent groups, such as the methyl group in polypropylene, for most isotactic polymers, and for polymers
19、of some 1,1-disubstituted ethylenes like polyisobutylene, the lowest-energy conformation is a helix of some preferred geometry. For the examples of polypropylene, three repeat units form a single turn in the helix (i.e., a 31 or 3/1 helix) In the case of polyoxyethylene, there are 7 repeat units per
20、 two terms (i.e., 72 or 7/2 helix).,全反式聚乙烯的构象 全反式聚乙烯呈平面锯齿状,这种构象能量低。以 CC 键长为0.154nm,键角为109.5计算,一个单体单元在键轴方向上的投影为0.252nm, 其应为两个靠得最近的H原子的距离,它大 于H原子范德华半径(0.12nm) 的两倍,因此,这种结构在能量上是合理的。,聚四氟乙烯的构象 H 被F取代,而F的范德华半径为0.14nm,其两倍0.28nm已大于0.252nm,如果聚四氟乙烯同样采取全反式构象,F原子就会出现拥挤,电子云互相排斥,这种排斥作用使得聚四氟乙烯被迫采取一种稍稍偏离全反式平面构象,呈现一种
21、扭转构象。 当T 19时,旋转角为12,变成H157 的螺旋构象。,聚甲醛和聚氧化乙烯的构象 由于聚甲醛分子主链上有氧原子存在,其对应位置的空间位阻小,与全碳链不同,旁式构象的能量反而比反式构象的能量低, 其中COC 键角为112,OCO 键角为111,形成等同周期为1.73nm 的.gg.系列的H95螺旋构象。 聚氧化乙烯则形成等同周期为1.93nm 的.ttg ttg.系列的H72螺旋构象。,等规a 烯烃分子链的构象 等规a 烯烃的分子链,由于取代基的空间位阻,全反式构象的能量一般比反式旁式交替出现构象的能量高,所以,这类聚合物的分子链在晶体中通常采取交替出现的反式旁式交替构象序列的螺旋形
22、构象。,聚丁二烯在结晶中的构象 聚丁二烯有四种异构体,其中反式 1, 4 聚丁二烯、顺式 1, 4 聚丁二烯和间规 1, 2 聚丁二烯都取主链接近平面锯齿形的全反式构象,而等规 1, 2 聚丁二烯取 H31 螺旋形构象。,2.4 Solid-State Model of Polymers,Crystalline Model of Polymer The fringed-micelle model 模型要点 高聚物只能部分结晶,具有晶区和非晶区两相同时并存的特殊结构; 每一个高分子链可以贯穿几个晶区和非晶区; 在非晶区,分子链是卷曲且互相缠结的,在晶区,分子链互相平行排列形成规整结构; 晶区的取
23、向是无规的。,The loose fold-chain folded model 在结晶高聚物的片晶中,仍以折叠的分子链为基本结构单元,折叠处松散而不规则, 但在晶片中分子链仍是相邻排列的。 在多层片晶中,分子链可以跨层折叠,在一层晶片中折叠几个来回之后,再到另一层中去折叠,使层片之间存在联结链。,The power panel model 折叠链部分是由多条链组成的,而且它们的排列是任意的,相邻链属于不同的分子链。 形成多层片晶时,一条分子链可以从一个晶片,通过非晶区进入到另一个晶片中去。,2.5 Crystallization of Polymers,The chemical struct
24、ure and Crystallization In general, symmetrical chain structures, which allow close packing of polymer molecules into crystalline lamellae and specific interactions between chains that favor molecular orientation, favor crystallinity. For example, linear polyethylene and polytetrafluoethylene, which
25、 have symmetrical substituted repeating units, are highly crystalline. Atactic poly(vinyl chloride) (PVC) with its asymmetrically placed chlorine is highly amorphous. When two chlorine atoms are symmetrically located on the same carbon atom, as they are in poly(vinylidene chloride), crystallinity is
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