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Polymer solutions, irradiation

On the basis of the results described, there seem to be at least three processes which are responsible for the molecular weight reduction in substituted silane high polymers upon irradiation in solution (i) Chain abridgement by silylene extrusion which occurs only at short wavelengths (ii) chain scission by silicon-silicon bond homolysis and (iii) chain scission by 1,1-photochemical reductive elimination. [Pg.122]

This reference discusses new uses for UV and EB irradiation, the response of polymers to irradiation, and tests related to dosimetry and radiometry, as well as safety and hygiene. It is also fortified with new problems and worked solutions, in addition to useful figures and tables, and appendices with supplementary information on equipment manufacturers, raw materials suppliers, and principles of green chemistry and sustainability. [Pg.285]

Measurement of Photochemical Reactivity. The polymer solution in THF was cast on a KRS plate and dried. The film obtained on the plate was irradiated by a high-pressure mercury lamp (Ushio Electric Co USH-250D) without a filter at a distance of 30 cm in air. The rate of disappearance of the C=C bonds at 1640 cm 1 was measured by IR spectrometry (JASCO A-202 model). [Pg.227]

Solution Photolysis of Poly(p-Formyloxystyrene) A 2.0 g sample of poly(/7-formyloxystyrene) was dissolved in 300 mis of spectral grade acetonitrile, and the solution irradiated in the Hanovia apparatus. Small aliquots of the irradiating polymer solution were withdrawn and analyzed at regular intervals as described above. [Pg.289]

Linear polystyrene can be generated on insoluble polymers by /-irradiation of the latter in a solution of styrene [110]. Polystyrene grafted onto polytetrafluoroethylene [111-116], polyethylene [2,110,117], or polypropylene [15] can be functionalized in the same way as cross-linked polystyrene, and loadings of up to 1.0 mmol/g can be attained. These supports, which are also available as crown-shaped pins (Multipin, 2-3 mm diameter, 8-10 pmol per crown), have been used for the synthesis of peptides [2,110,111,118], oligonucleotides [112-115,117,119], and small molecules [120-122]. [Pg.25]

Here, it is worthwhile to note the difference in the response times of the dissolution and phase separation processes. This is important from the view point of energy conversion efficiency. At 19.5 °C, which is very close to Tc of the polymer solution with all trans azobenzene chromophores, the isomerization of a small number of chromophores, in other words, a small number of photons, was enough to raise Tc above 19.5 °C. Therefore, the transmittance increase took place immediately by irradiation for a very short time. The polymer chain was efficiently expanded by a small number of photons. [Pg.54]

When the leuconitrile content was 1.0 mole %, the 1 mass % aqueous polymer solution showed Tc at 29.2 °C. Upon UV irradiation, the polymer did not show any more clear phase separation. The transmittance decreased gradually with increasing temperature above 36 °C. The absence of the phase separation behavior indicates that the hydrophobic interaction of the main chain is not strong enough to overcome the hydrophilidty of the photogenerated triphenyl-methyl cations and the polymer chain cannot shrink any further even at a higher temperature. [Pg.55]

Poly(vinyl methyl ether), PVME, is a thermo-sensitive polymer. The aqueous solution has a Lower Critical Solution Temperature (LCST) of 37 °C. Therefore, PVME is soluble in water below its LCST, but insoluble above its LCST. When an aqueous solution of PVME is irradiated with y-rays the solution becomes PVME hydrogel [18, 19]. The gel shows thermo-sensitivity similar to the solution, and swells below 37 °C and shrinks above this temperature. It is important to form a fine porous gel structure to obtain quick response gels. There are two methods for the purpose. One is a method using micro-phase separation by heating. The other is a method using micro-phase separation by blending of polymer solutions. [Pg.253]

Thus, macroradicals have been obtained by stretching fibers (20), deforming plastics by compression (37), ball mill grinding (11), freezing and grinding of polymer solutions (10), ultrasonic irradiation (I), mastication (19), dispersion in a microblender (25), and other mechanical techniques (36). Many reviews on the formation of macroradicals by degradative processes have also been published (5, 12,13,16, 33). [Pg.430]

Membrane filters are usually made by casting a polymer solution on a surface and then gelling the liquid film slowly by exposing it to humid air. The size of the pores in the membranes can be varied by altering the composition of the casting solution or the gelation condition. Another common technique is to irradiate a thin polymeric film in a field of a-particles and then chemically etch the film to produce well-defined pores. [Pg.286]

Transfer of energy from ionizing radiation to the solution produces various kinds of excited state. The energy transfer processes in irradiated polymer solutions can be probed by observing the excited states of the polymers. [Pg.59]

Figure 10 CD spectra of orthocopolymer 25 (r = 1) in methylene chloride and tetrahy-drofuran (1 1) solution (T,V), meta-terpolymers 24 (r = 0.02) in rc-hexane solution (A,A), and orthoterpolymer 25 (r = 0.04) in rc-hexane solution ( , ) irradiated with CPL. The filled up-triangle, down-triangle, and square are CD spectra of the polymers irradiated with r-CPL, and the open up-triangle, down-triangle, and square are CD spectra of the polymers irradiated with /-CPL. (Reproduced from Ref. 80 2000, American Chemical Society.)... Figure 10 CD spectra of orthocopolymer 25 (r = 1) in methylene chloride and tetrahy-drofuran (1 1) solution (T,V), meta-terpolymers 24 (r = 0.02) in rc-hexane solution (A,A), and orthoterpolymer 25 (r = 0.04) in rc-hexane solution ( , ) irradiated with CPL. The filled up-triangle, down-triangle, and square are CD spectra of the polymers irradiated with r-CPL, and the open up-triangle, down-triangle, and square are CD spectra of the polymers irradiated with /-CPL. (Reproduced from Ref. 80 2000, American Chemical Society.)...
Fig. 1 Irradiation setup for pulse radiolysis consisting of a solution reservoir, a peristaltic pump, and a quartz irradiation cell. Prior and during irradiation, the polymer solution is continuously saturated with argon... Fig. 1 Irradiation setup for pulse radiolysis consisting of a solution reservoir, a peristaltic pump, and a quartz irradiation cell. Prior and during irradiation, the polymer solution is continuously saturated with argon...
The most popular way to synthesize microgel particles is via emulsion polymerization. Each micelle acts as a separate microreactor, preventing macrogelation during the reaction. Another way to obtain microgel particles is the irradiation of phase-separated polymer solutions (Fig. 5). Phase separation can be achieved by heating (for temperature-sensitive polymers) or mixing with non-solvents. [Pg.110]

Photolysis of metal compounds is a method of historical dimension as it has been used since the middle of the nineteenth century, when the light-sensitivity of silver salts was used for photographic purposes. Novel research, especially linked with the names Henglein and Belloni, led to a large extended field in the science of nanoparticles. UV-visible irradiation of Au, Ag, and Pt salts in surfactant or polymer solutions end up with nanoparticle formation. " Compared with hydrogen reduction, photolytic reactions usually give smaller particles with narrower size distribution. ... [Pg.5933]

A dilute polymer solution has a turbidity of 0.0100 cm . Assuming that the solute molecules are small compared to the wavelength of the incident light, calculate the ratio of the scattered to incident light intensities at 90° angle to the incident beam and 20 cm from 2 ml of solution. Assume that all the solution is irradiated. [Pg.117]

To evaluate photoisomerization and photo-orientation parameters, and should be known, was calculated from the absorption spectrum of the polymer solution before irradiation, assuming the same extinction coefficient in the film and in solution bq was determined by the Fisher s method, modified by Rau, which holds not only for isotropic but also for anisotropic samples when the isotropic absorbance is considered (vide infra). For this determination, the isotropic absorbance change was recorded versus the irradiating light intensity, and the sample absorbance change was extracted for an irradiation flux extrapolated to infinity for three drbierent combinations of irradiation and analysis wavelengths 488-488, 532-488, and 532-532 nm, irradiation and analysis, respectively. These experiments... [Pg.86]


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See also in sourсe #XX -- [ Pg.12 ]




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