Physical Aspects of Polymer Self-Assembly

Wiley (Verlag)
  • erschienen am 15. November 2016
  • |
  • 384 Seiten
E-Book | ePUB mit Adobe DRM | Systemvoraussetzungen
978-1-118-99439-9 (ISBN)
Offering an overview of principles and techniques, this book covers all major categories of self-assembled polymers - properties, processes, and design. Each chapter focuses on morphology, applications, and advanced concepts to illustrate the advantages of polymer self-assembly across industrial and academic research.
* Provides an organized, comprehensive overview of polymer self-assembly, its fundamentals, principles, and applications
* Includes chapters on block copolymers, amphiphilic polymers, supramolecular polymers, rotaxenes, polymer gels, dendrimers, and small molecules in polymer matrices
* Focuses on novel applications, block copolymer assembly to nanotechnology, photonics and metamaterials, molecular machines and artificial muscle, gels that can be applied to polymer science, materials science, and nanotechnology
* Examines state-of-the-art concepts, like lithographic patterning and foldaxane
* Discusses challenges and future outlook of a popular and emerging field of study
1. Auflage
  • Englisch
  • New York
  • |
  • USA
John Wiley & Sons
  • 52,98 MB
978-1-118-99439-9 (9781118994399)
1118994396 (1118994396)
weitere Ausgaben werden ermittelt
P. R. Sundararajan, PhD, DSc, is a Professor in the Department of Chemistry at Carleton University in Ontario, Canada and has over 40 years of academic and industry experience in polymer chemistry. He has held positions as the NSERC-Xerox Industrial Research Chair Professor, Director of the Ottawa Carleton Chemistry Institute, Associate Chair of Graduate Affairs at the university, and Principal Scientist, Manager, and Project Leader at the Xerox Research Center of Canada. His current research focuses on the morphology of self-assembly systems, macromolecular nanotechnology, organo- and polymer gels and the morphology of polymer composites in confined systems. He is a winner of the Macromolecular Science and Engineering Award of the Chemical Institute of Canada, Materials Chemistry Award of the Canadian Materials Society and is a Fellow of the Chemical Institute of Canada. He was the President of the Canadian Society for Chemistry and the Chair of the Chemical Institute of Canada.
Preface xi
1 Introduction 1
1.1 Polymer Tacticity 1
1.2 Big versus Small 5
1.3 Entanglement 5
1.4 Excluded Volume 8
1.5 Free Volume 10
1.6 Self-Assembly 10
1.7 Polymer Self-Assembly 12
References 13
2 Molecular Forces 17
2.1 Van der Waals Interaction 17
2.2 Hydrogen Bond 21
2.3 C-H...pi Interaction 27
2.4 Halogen Bond 29
2.5 Other Hydrogen Bonds 30
2.6 Coulombic Interaction 31
References 33
3 Features of Self-Assembly 37
3.1 Self-Sorting--Small Molecules 37
3.2 Polymer Self-Sorting 43
3.3 Concentration-Dependent Association 48
3.4 Polymer-Guest Molecule Recognition 49
3.5 Sergeant-Soldier Phenomenon 55
3.6 Majority Rules 61
3.7 Chain Folding 65
3.8 Foldamers 79
3.9 Single Chain Polymer Crystals and Nanoparticles 91
References 99
Further Reading 104
4 Supramolecular Macromolecules and Polymers 105
4.1 Supramolecular Macromolecules 105
4.2 Supramolecular Polymers 110
4.3 Modular Supramolecules 123
4.4 Solvent Influence 127
4.5 Comb Polymers 140
References 149
Further Reading 152
5 Block Copolymers 153
5.1 Theoretical Aspects 153
5.2 Diblock Copolymers 158
5.3 Organic/Inorganic Diblocks 165
5.4 Blends of Diblock Copolymers 170
5.5 Diblock/Homopolymer Blends 172
5.6 BCP/Small-Molecular Supramolecular Association 175
5.7 Triblock Copolymers 177
5.8 Some Applications of Gyroid Morphology 190
5.9 Graphoepitaxy 201
5.10 Porous Structures 211
5.11 Crystalline Block Copolymers 223
5.12 Nanotechnology 223
References 225
Further Reading 230
6 Rotaxanes and Polyrotaxanes 231
6.1 Definitions and Early Work 231
6.2 Cyclodextrins for Inclusion 237
6.3 Selective Threading 244
6.4 Micelles of Double-Hydrophilic Block Copolymers via Rotaxane Formation 249
6.5 Homopolymer Micelles 252
6.6 Linear and Cyclic PDMS 253
6.7 Abrasion Resistance 254
6.8 Beyond Linear Polymers and alpha-, beta-, and gamma-CDs 256
6.9 Insulated Molecular Wires 258
6.10 Molecular Switches and Machines 260
6.11 Supramolecular Oligomeric and Polymeric Rotaxanes 268
6.12 Rotaxane and Polyrotaxane-Based Muscles 270
References 277
Further Reading 280
7 Polymer Gels 281
7.1 One-Dimensional Growth 281
7.2 Definitions and Classifications 283
7.3 Gels with Noncrystallizable Polymers 285
7.4 Gels with Crystallizable Polymers 295
7.5 Add a Sergeant to the Soldiers to Cause Gelation 300
7.6 pi-Interaction-Mediated Gelation 308
7.7 Polymer Compatibilized Small Molecule/Polymer Gels 316
7.8 Monomer Self-Assembly and Polymer Gels 318
7.9 Poor Man's Rheology 321
References 324
8 Small-Molecule Self-Assembly in Polymer Matrices 329
8.1 Phase Separation in Charge Transport Polymer Layers 329
8.2 Glass Transition and Diffusion of Small Molecules 331
8.3 Subsurface Self-Assembly of Small Molecules in Polymer Matrices 333
8.4 Solvent Effect on Self-Assembly of Small Molecules in Polymer Matrices 338
8.5 Polymer-Compatibilized Small-Molecule Assembly in Polymer Matrices 343
8.6 Polymerization-Induced Phase Separation and Reaction-Induced Phase Separation 344
8.7 PIPS for LC Displays 345
8.8 PIPS with Supramolecular Assembly 347
8.9 PIPS for Porous Structures 347
8.10 Surfactant/Polymer Assembly 350
References 356
Index 359


Polymers are ubiquitous in our daily lives. Natural polymers such as the DNA, RNA, and proteins have played a major role in the evolution of life itself. Cellulose, hemicelluloses, starch (amylose), and other naturally occurring polymers have been studied thoroughly, modified for useful applications and have been the key components of industrial advancement. Familiar to many is the chronological transition of the belief of these substances as colloids to the concept of "polymers." The "Rise of the Macromolecular Hypothesis" was discussed by Flory [1]. Supporting the Staudinger school of thought were, among others, the X-ray diffraction studies of cellulose by Meyer and Mark [2, 3]. Cellulose is perhaps the first polymer for which oriented X-ray fiber diffraction was recorded [2]. Synthetic polymers have also entered the scene around that time, with the synthesis of polystyrene [4] in 1839.

According to the International Union of Pure and Applied Chemistry (IUPAC) nomenclature [5], the terms polymer and macromolecule do not mean the same thing. A polymer is a substance composed of macromolecules. All macromolecules are not polymers.

1.1 Polymer Tacticity

As a polymer (Figure 1.1) is built up of many small molecular monomer units, the dimer (diad), trimer (triad), tetramer (tetrad), pentamer (pentad), and hexamer refer to two, three, four, five, and six monomers, respectively, linked together. Longer sequences of up to about 50-mers are called "oligomers." However, it is not uncommon in the studies on self-assembly to call such short chains polymers. Although natural or biopolymers such as poly(nucleic acids) (e.g., DNA), proteins and polysaccharides are also long chain molecules, the commonplace notion is that a polymer refers to the synthetic variety. Of these, vinyl polymers such as polyethylene (PE) and polystyrene are popularly known as plastics. The simplest of polymers is PE, with just a sequence of (CH2) units (Figure 1.2). Polymerization of ethylene, vinyl fluoride, vinylidene fluoride, and tetrafluoroethylene lead to PE, poly(vinyl fluoride) (PVF), poly(vinylidene fluoride) (PVF2), and poly(tetrafluoroethylene), respectively. The latter is the well-known Teflon®.

Figure 1.1 Schematics of a monomer, dimer, and a polymer.

Figure 1.2 Chemical structures of polyethylene and analogous fluorinated polymers. The dashed circles highlight the fluorine atoms.

With bulkier substituents, polymers such as polystyrene, poly(methyl methacrylate), and poly(propylene) are obtained (Figure 1.3). Note that in the case of PE, PVF2, and PTFE, the substitution is symmetric, whereas with PVF, polystyrene, PMMA, and polypropylene, it is asymmetric. In the schematics shown in Figures 1.2 and 1.3, the bulkier substituent (R) is shown above the plane of the page. A general rendition is shown in Figure 1.4. In the figure [6], with the skeletal bonds in the all-trans conformation, the configuration with R above the page at the asymmetric carbon is designated as d and as l if it is below. If the substituents on two successive asymmetric carbons are in the same dd configuration, it is known as a "meso" (m) diad.

Figure 1.3 Chemical structures of polystyrene, poly(methyl methacrylate), and polypropylene.

Figure 1.4 (a)-(c) Schematic of the definition of tacticity for asymmetric chains.

(Source: Sundararajan [6]. Reproduced with permission of Springer.)

Perpetuation of such meso sequence would lead to an isotactic chain (Figure 1.4a). If the R groups are up and down the page, that is, dl, it is the racemic (r) diad (Figure 1.4b). The repetition of the racemic diad (dl sequence) would result in a syndiotactic polymer. Random occurrence of m and r results in an atactic polymer. The designation of d and l for the configuration at the asymmetric carbon is arbitrary. It follows the convention developed by Flory [7], which then led to the formulation of statistical weight matrices to calculate the statistical chain conformations. If the chain is rotated through 180° about a vertical axis such that the ends of the chain are reversed, all the d would become l and vice versa. But the chain configuration would remain the same as long as the chain ends are indistinguishable. The ll would define the meso diad. With the diad configurations m and r defined earlier, a triad could have sequences of mm, rr, and mr (or rm). A tetrad could have sequences mmm, mmr, rmr, mrm, rrm, and rrr, of which only two of them would lead to stereoregular isotactic or syndiotactic chains. A pentad could have 10 such sequences, 8 of which will be heterotactic. Determining the distribution of such sequences in vinyl polymer chains that were prepared by various synthetic procedures was an active field, concurrent with advances in the NMR techniques [8-11]. Although synthetic methods for stereoregular polymers have been developed, some of them such as isotactic polystyrene are of academic interest rather than of commercial use. Atactic polystyrene, in the form of, for example, Styrofoam, finds widespread applications. Likewise, PMMA in its atactic form, is used as a substitution for glass in the form of Plexiglass, as well as in microelectronic chips, etc. Studies on highly isotactic or syndiotactic polymers led to the understanding of aspects such as polymer crystallization and chain folding. In the studies of self-assembly of polymers, tacticity was seldom taken into consideration.

Some of the other polymers commonly used in studies of polymer self-assembly are polyesters, polyamides, polyurethanes, and polysiloxanes, the constituent units of which are shown in Figure 1.5. A summary of the synthetic procedures adopted for various types of polymers and their primary characterization properties was given by Sundararajan [6].

Figure 1.5 Schematics of the segments of polyester, polyamide, polyurethane, and polysiloxane.

1.2 Big versus Small

As the small molecule "mono" mer units are joined together to build a "poly" mer, the properties change as the polymer increases in length. For example, ethane has boiling temperature of -89° and melts at -183°C. After growing by a few units, hexadecane melts at 18.5°C. With a further increase in chain length, triacontane [CH3─(CH2)28─CH3] melts at 65°C, and does not boil. High-molecular-weight PE melts at 138°C. While the small molecules could melt and vaporize, polymer molecules melt and degrade rather than vaporizing. Most polymers show a glass-rubber transition (Tg), whereas not all small molecules show a glass transition. Both could crystallize, but polymers should have a regular sequence of monomers (e.g., isotactic or syndiotactic) to be able to crystallize. Those with random sequence remain amorphous. The Tg is an important property of a polymer since it dictates the processing conditions for industrial applications. Small molecules such as D-glucose have a finite number of conformations, for example, the C1 chair form. However, amylose, which is a high-molecular-weight polymer of D-glucose, could have a large number of conformational sequences between contiguous D-glucose units due to rotations about the interunit C1─O─C4 single bonds. The number of accessible conformations without steric overlap determines the "flexibility" of a polymer.

1.3 Entanglement

When a small molecule is dissolved in a solvent medium (lattice model) as shown pictorially in Figure 1.6a, both molecules can move and exchange lattice points just by diffusion and thermal motion. However, when a polymer is placed in a solvent (Figure 1.6b), coordinated movement of the monomer units is necessary for the chain to diffuse. This results in loss of entropy of mixing. This would increase the viscosity of the solution compared to the small molecule/solvent mixture. One of the most important properties of a polymer is the "entanglement" between its segments. A small molecule cannot entangle. As the polymer chain grows in length, due to coiling in solution or the melt, entanglement would set in. Most text books would mention a bowl of spaghetti as an example of entangled polymer chains. The polymer must be of a certain minimum length for entanglement to occur. For a bowl of cooked spaghetti to be an entangled stock, the length of the dry noodle should be about one foot. The average length of commercially sold dry spaghetti is 12-14 in., which assures the entanglement upon cooking. The critical molecular weight Mc for entanglement for polystyrene is about 37 000, while it is only about 5000 g/mol for polycarbonate [12]. Conformational analysis showed that polycarbonate chain can adopt flat helical as well as extended chain shapes with equal probability [13]. Thus, a low molecular weight is sufficient for entanglements to occur in the case of polycarbonate. Mc varies depending on the polymer structure and conformation. Another parameter is the entanglement molecular weight, Me, which corresponds to the average molecular weight...

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