chemical physics of discharges - Argonne National Laboratory
chemical physics of discharges - Argonne National Laboratory chemical physics of discharges - Argonne National Laboratory
h B C D 2-'? Figure 2. Infrared Spectra -7 /I/ ' !I '! i T A = Polystyrene film B = Solid polymer from benzene C = Liquid polymer from benzene D = Solid polymer from styrene
observed. The polystyrene (10% solution in ccl4) spectrum simply showed two broad peaks - one centered at 6 = 1.50 due to aliphatic protons and one at 6 = 7.08 (with a small companion peak at 6 = 6.58) due to aromatic protons. The spectrum of the liquid polymer (lo”/. solution in cc14) was quite similar with the peaks appearing at 6 = 1.60 and 7.04 (no peak at 6 = 6.58). In addition, a very small peak at 6 = 5.70 was observed. This is probably due to protons on olefinic double bonds, and suggests either that some unspturation is present in the polymer backbone, or that some unpolymerized vinyl groups are present. An attempt was made to increase the resolution of the NMR spectra by using a time averaging computer on very dilute solutions of the polymers, but the resolution was unchanged. Though of limited value, the NMR data do support a polystyrene type Structure. Coupled with the infrared data, it seems quite likely that the pOlyITIerS are both polystyrenes. Mode of Formation of Polymer The most likely route from benzene to polystyrene involves several steps, the first of which is the establishment of an equilibrium between benzene and acetylene: This interconversion has been observed in many high energy systems including electrical discharges. In the next step, the benzene and acetylene, one or both of which may be in a reactive state, combine to give styrene which then polymerizes: The simple linear polymer thus formed, limited to small chains such as pentamers, hexamers, etc., would explain the liquid polymer product. The formation of the highly cross-linked solid polymer can be explained by postulating the formation of polyvinylbenzenes which, when polymerized, would yield an extensive, irregular structurer 4. Highly cross-linked polystyrene
- Page 227 and 228: Figure 5.- Paschen's law curves. 2-
- Page 229 and 230: \ '? I The water-free product gases
- Page 231 and 232: N I + 0" ON i I + 0 u / 0 0 I 0 cu
- Page 233 and 234: - 233 SOME PROBLEMS OF THE KINETICS
- Page 235 and 236: .. . :. ,. .I , . i ? .. . , ... .
- Page 237 and 238: 237 Table 2 Experimental Variables
- Page 239 and 240: 239 Zhbie I Eerccnt Consumption of
- Page 241 and 242: 241 Discussion The systematic varia
- Page 243 and 244: I \ 1 243 FORMATION OF HYDROCARBONS
- Page 245 and 246: h z - a o m a 20 T IME, minutes . F
- Page 247 and 248: I 1 I I I I 0 I 2 3 4 5 TIME, minut
- Page 249 and 250: The next five coluws in table 1 sho
- Page 251 and 252: \ .\ t 251 Given the existence of t
- Page 253 and 254: I L 253 Epple, R. P. and C. M. Apt.
- Page 255 and 256: 1 ' Fig. 1 Schematic of flow discha
- Page 257 and 258: 5' . ' I 1 257 co, with excess H2,
- Page 259 and 260: 1 1 1 moo 1400 1300 c V' I IPOO I I
- Page 261 and 262: i 25i The Dlssocfatior of ToIuere V
- Page 263 and 264: L ! , c PRODUCTS FROM A 28 MC. DISC
- Page 265 and 266: '\ J ?. , .. . : PRODUCT FORMATION
- Page 267 and 268: '9 / I '\ "1 BENZYL CATION AND RADI
- Page 269 and 270: a
- Page 271 and 272: 271 tube serve? as the high voltare
- Page 273 and 274: 273 ion (1L.). Zxcitei-ion by colli
- Page 275 and 276: Apparatus and Procedure 275 EXPERIM
- Page 277: . 277 6. A freshly prepared sam le
- Page 281 and 282: i i (12) c (11) (14) I 281 LITERATU
- Page 283 and 284: FLOW- METER I ADDITIVE SUPPLY * ,28
- Page 285 and 286: 285 TABLE 2 Effect of Haloqenated A
- Page 287 and 288: ANALYTICAL RESULTS Some evidence wa
- Page 289 and 290: DISCUSSION 289 The salient features
- Page 291 and 292: ? ~ MENBERSHIP IN THE DIVISION OF F
- Page 293 and 294: 292 flow of the reactant gas stream
- Page 295 and 296: 294 have suitable residence times i
- Page 297 and 298: 0 E < h( E l! d K c 0 .- Y 0 t u t
- Page 299 and 300: 298 yields of many chemical product
- Page 301 and 302: - ;i Y . 15. Pressure lOmm 5 > 10-
- Page 303 and 304: 302 the best and in many practical
- Page 305 and 306: GENERATION AND MEASUREMENT OF AUDIO
- Page 307 and 308: . The transformer secondary and the
- Page 309 and 310: Vaccum-Tube Amplifier The mobile co
- Page 311 and 312: 310 f = Power supply frequency in c
- Page 313: FUFARCI! INSTITUTE OF TFYDLC UNIVER
- Page 316 and 317: J # I / 4) I . . '8 r4 0 r( P
- Page 318 and 319: 317 i Cuencb svsten w.nnar;itus use
- Page 320 and 321: epcrte? the noss~kil.itv of nroduct
- Page 322 and 323: 1' b t +
- Page 324 and 325: 323 ....... - . . . . . . . . . . .
- Page 326 and 327: 1 \ i I i , / / / 8 3 1 325 To205 +
observed. The polystyrene (10% solution in ccl4) spectrum simply<br />
showed two broad peaks - one centered at 6 = 1.50 due to aliphatic<br />
protons and one at 6 = 7.08 (with a small companion peak at 6 = 6.58)<br />
due to aromatic protons. The spectrum <strong>of</strong> the liquid polymer (lo”/.<br />
solution in cc14) was quite similar with the peaks appearing at<br />
6 = 1.60 and 7.04 (no peak at 6 = 6.58). In addition, a very small<br />
peak at 6 = 5.70 was observed. This is probably due to protons on<br />
olefinic double bonds, and suggests either that some unspturation is<br />
present in the polymer backbone, or that some unpolymerized vinyl<br />
groups are present. An attempt was made to increase the resolution<br />
<strong>of</strong> the NMR spectra by using a time averaging computer on very dilute<br />
solutions <strong>of</strong> the polymers, but the resolution was unchanged. Though<br />
<strong>of</strong> limited value, the NMR data do support a polystyrene type Structure.<br />
Coupled with the infrared data, it seems quite likely that the pOlyITIerS<br />
are both polystyrenes.<br />
Mode <strong>of</strong> Formation <strong>of</strong> Polymer<br />
The most likely route from benzene to polystyrene involves<br />
several steps, the first <strong>of</strong> which is the establishment <strong>of</strong> an<br />
equilibrium between benzene and acetylene:<br />
This interconversion has been observed in many high energy systems<br />
including electrical <strong>discharges</strong>. In the next step, the benzene and<br />
acetylene, one or both <strong>of</strong> which may be in a reactive state, combine<br />
to give styrene which then polymerizes:<br />
The simple linear polymer thus formed, limited to small chains such<br />
as pentamers, hexamers, etc., would explain the liquid polymer<br />
product.<br />
The formation <strong>of</strong> the highly cross-linked solid polymer can<br />
be explained by postulating the formation <strong>of</strong> polyvinylbenzenes which,<br />
when polymerized, would yield an extensive, irregular structurer<br />
4.<br />
Highly cross-linked polystyrene