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PICTURE 001 it was found that this conductivity could be increased by doping with an electron acceptor such as bromine (-104 S cm). 1 Unfortunately, interest in this polymer was less than it would otherwise be because of the explosive nature of its precursor monomer. S2N2. By die late 1970s. researchers in Japan and the United States had shown that the electrical conductivity of an organic polymer — polyacetylene — could also be increased by a factor of 1017 (to -10s S cm-1) when it was doped with an electron donor such as an alkali- metal ion or an electron acceptor such as arsenic pentafluo-ride (AsFs) or iodine. The conductivity of doped polyacetylene is comparable to that of copper on an equal weight basis. A comparison of the electrical conductivities and specific gravities of several polymers. common metals, and carbon is made in Table 12.9. TABLE 12.9 CONDUCTIVITIES OF POLYMERS AND METALS More recently. conductivity has been demonstrated for doped versions of poly(p-phenylene). polypyrrole, polythiophene. and polyaniline. The synthesis and properties of conductive polymers were discussed in Section 10.2.7. Although the electrical conductivities of these polymers are lower than polyacetylene. Polysulfumitride has been observed to become superconductive (10-3) at temperatures approaching absolute zero (-0.3 K). TABLE 1 2.1 0 CHEMICAL STRUCTURES AND CONDUCT-IVITIES OF SOME ELECTRICALLY CONDUCTIVE POLYMERS Approximate maximum conductivity of doped polymer. polyaniline exists in four oxidation states, of which only the emeraldine salt is a good conductor requiring only protonic doping of the imine nitrogen as shown. P-Methylphenylsulfonate.

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Page 1: Ing Gris

PICTURE 001

it was found that this conductivity could be increased by doping with an electron acceptor such as bromine (-104 S cm). 1 Unfortunately, interest in this polymer was less than it would otherwise be because of the explosive nature of its precursor monomer. S2N2.

By die late 1970s. researchers in Japan and the United States had shown that the electrical conductivity of an organic polymer — polyacetylene — could also be increased by a factor of 1017 (to -10s S cm-1) when it was doped with an electron donor such as an alkali-metal ion or an electron acceptor such as arsenic pentafluo-ride (AsFs) or iodine. The conductivity of doped polyacetylene is comparable to that of copper on an equal weight basis. A comparison of the electrical conductivities and specific gravities of several polymers. common metals, and carbon is made in Table 12.9.

TABLE 12.9 CONDUCTIVITIES OF POLYMERS AND METALS

More recently. conductivity has been demonstrated for doped versions of poly(p-phenylene). polypyrrole, polythiophene. and polyaniline. The synthesis and properties of conductive polymers were discussed in Section 10.2.7. Although the electrical conductivities of these polymers are lower than polyacetylene.

Polysulfumitride has been observed to become superconductive (10-3) at temperatures approaching absolute zero (-0.3 K).

TABLE 1 2.1 0 CHEMICAL STRUCTURES AND CONDUCT-IVITIES OF SOME ELECTRICALLY CONDUCTIVE POLYMERS

Approximate maximum conductivity of doped polymer.

polyaniline exists in four oxidation states, of which only the emeraldine salt

is a good conductor requiring only protonic doping of the imine nitrogen as shown. P-Methylphenylsulfonate.

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PICTURE 002

polymers are more stable to effects of oxygen and moisture. As shown by the chemical structure of the repeating units of these polymers in Table 12.10, a common feature that makes these polymers capable of transporting electrical charge is a conjugated ɳ-electron consisting of alternating single and double bonds along the polymer chain backbone or ring structure. It is believed that doping results in an electron imbalance, and the extended ɳ -conjugated structure of the conductive polymer allows the new electron population to move along the backbone when an electric potential is applied. •

In general, conductivity increases with decreasing band gap which is the amount of energy needed to promote an electron from the highest occupied energy level or valence band to the empty band immediately above it. The empty band is the conduction band. Metals have zero band gaps, while insulators like many polymers have large band-gaps (1.5 to 4 cV) which impede electron flow. By careful design of the chemical structure of the polymer backbone, it may be possible to obtain band gaps as low as 0.5 to 1 eV. Currently. the lowest band gap observed for a polimer is -1 eV reported for polyisothianaphilialene (see Table 12.10).

Figure 12.21. Illustration of a rechargeable battery using a polymetric cathode (polyaniline). The anode is a lithium-aluminum alloy. while the electrolyte can be a solution (e.g.. propylene carbonate) of an appropriate salt or a solid polymer electrolyte Li-PEO). (Courtesy of M. G. Kanatzidis.)

Potential applications of conductive polymers are significant since they arc generally lighter, more flexible, and easier to fabricate than many of the materials they seek to replace. Current examples include the use of polymers as both cathodes and solid electrolytes in batteries for automotive and other applications as alternatives to lead-acid batteries in automotive and other applications. A diagram of a typical lithium-polymer battery is shown in Figure: 12.21. Potential advantages of polymeric batteries include high reliability, light weight, nonleakage of electrolyte solution, ultrathin-film form, flexibility, and high energy density (up can be used as the cathode material, while lithium dissolved in aluminum foil serves as the anode. Lithium-poly(p-phenylene) batteries can deliver current densities as high as 50 mA cm2 have efficiencies of 91% in charging and discharging, and have theoretical energy densities of 320 W-h kg'. Examples of polymers used in the formulation of solid electrolytes include poly(alkyl sulfide)s, polyphosphazene (see Section 10.2.5) having oligo(oxyethylene) side groups, and especially poly(ethylene oxide). Salts that are added to form the electrolyte include a number of lithium salts having low crystal lattice energies. such as lithium tetrafluoroborate (LiBF4), lithium hexafluoroarsenate (LiAsF6). lithium perchlorate (LiClO4), and lithium trifluoromethanesulfonate sometimes called lithium triflate (LiCF3SO3).

Other possible uses of conductive polymers include variable-transmission ("smart") windows, electrochromic displays, fuel cells, sensors, conductive paints. semiconductor circuits, low-current wires, electromechanical Winters, electro-magnetic shielding, light-emitting diodes, and nonlinear-optical material. Wider commercial utilization awaits further increases in intrinsic conductivity and improvements in the mechanical properties and processability of these interesting polymers.

12.3.2 Electronic Shielding

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Undesirable signals in the radio-frequency (rf) range emitted by many electrical devices such as computers can interfere with normal rf reception. This behavior is called electromagnetic interference (EMI). Recent regulations from the Federal Communications Commission (FCC) have placed restrictions on rf transmissions by computers and other electrical devices. Unfilled polymers provide very little EMI shielding capability. Generally, carbon- and metal-filled composites such as PVC filled with aluminum flakes provide suitable housings for low-emission electronic devices.

12.3.3 Encapsulation

Polymers are used to provide integrated-circuit devices with a protective seal against moisture, radiation, and ion contamination. Thermosets. thermoplastics. and elastomers are all used as encapsulants. Included among thermosets are thermosetting polyimides. epoxies, unsaturated polyesters, and alkyd resins. As reviewed in Section 9.2. Candidates among thermoplastic encapsulants are poly(vinyl chloride), polystyrene. polyethylene. fluoropolymers. and acrylics. Elastomers can include silicone rubber and polyurethanes. For the most critical applications. epoxies and polyimides have been the most favored.

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PICTURE 003

12.4 PHOTONIC POLYMERS

The next technological revolution may be the widespread use of optical rather than electronic devices for the storage and processing of data. Optical technology has the advantages of both speed and compactness of storage space. Optical storage of computer data is already common (ie. CD-ROM and WORM drives), and ways to use optical devices for processing data are being explored. Among materials that are suitable for optical technology are polymers that exhibit nonlinear-optical properties. This means that their optical properties vary with the intensity of the light compared to ordinary glass, which is linear in its optical properties. Photoresponsive sunglasses that change tint with the intensity of sunlight are examples of non-linear-optical materials.

In general. molecules with ɳ-electron structures can exhibit nonlinear-optical effects when these electrons are optically excited. In the case of polymers, these n-electron structures can be part of the main-chain backbone, as for example in the case of the 6F-polyimide (sec Section 10.2.1)

The nonlinear-optical functionality can also be incorporated as a side chain, as in the case of an acrylate polymer

having a substituent group (R) that contains a 4-methoxy-4’-nitrostilbene moiety connected by a six-carbon spacer

12.5 DRAG REDUCTION

It has been observed that dilute solutions (1 to 100 ppm) of many high-molecular-weight (>100,000), linear polymers can reduce turbulent friction in fluid flow by as much as 70% to 80%. Examples of synthetic water-soluble polymers that are very effective as drag-reducing agents include poly(ethylene oxide) and poly-acrylamide. An example of a commonly used oil-soluble polymer is polyisobutylene. Some naturally occurring polymers such as guar (from Cyamopsis tetragono-logus) and xanthan (Xanthamonas exudate) arc also effective drag reducers. It has also been observed that suspensions of some fibers. including nylons, can impart good drag reduction in turbulent flow.

Although the exact mechanism of drag reduction is still under, it is believed that drag reduction may be related to extensional flow. During flow, the long polymer chains become disentangled and oriented in the direction of flow. Extensional viscosity (see Chapter II) significantly increases and a form of strain-rate hardening occurs, which imposes a maximum limit on the strain rate. The high extensional viscosity reduces turbulent fluctuations (probably through the suppression of the roll-wave motion and vortex stretching in the sublayer) and thereby reduces friction.

Applications for drag reduction include any where reduced friction in fluid flow is desired. For example, a small amount of a water-soluble polymer can be injected into sewers during periods of heavy rain to upgrade flow and, thereby prevent flooding. Also a drag-reducing polymer can be

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injected at the bow of a ship to decrease friction and increase speed or be used to decrease pressure drop in water lines for fire fighting.

REFERENCES

I. W. R. Vieth, J. M. Howell, and J. H. Hsieh, J. Membr, Set. 1, 177 (1976).

2. D. 12. Paul and W. J. Koros, J. Petra. Set. Polyp. Phys. Ed.. 14. 675 (1976).

3. T. D. Gierkc and W. Y. Hsu, ACS Synop. Ser.. 180, 283 (1982). 4. J. M. S. Hcnis and M. K. Tripodi. J. Alembr. Set, 8. 233 (1981).

BIBLIOGRAPHY

G. Beifort, Synthetic Membrane Processes. Academic Press. Orlando. FL. 1984. J. Comp', Polpner Permeability, Elsevier Applied Science Publishers. London. 1985.