chemical physics of discharges - Argonne National Laboratory
chemical physics of discharges - Argonne National Laboratory chemical physics of discharges - Argonne National Laboratory
494 mechanisms. However, the voltade dependence for the current at a relatively low electric field is linear, indicating that Ohm's law is valid (Fig. 3). I This adherence to Ohm's law supports the belief that the conduction is electronic (19). The fact that the asphaltene-iodine sample exhibits (Fig. 6) strong enhancement of absorption near 1080 crn'l suggests that an iodine molecule forms a donor-acceptor complex with the aromatic portion of the asphaltenes. It is known that the iodine molecule forms such a charge- transfer complex with benzene and other alkylated benzenes, and that these complexes, in general, exhibit bands from 9 9 cm'l to 1200 cm'l (24,25). Arguing from analogy, it is plausible that the complex assumes the axial model (model A of Mulliken) while the acceptor molecule is sitting perpendicular to the plane. of the aromatics (26). Further, our failure to' locate any C-I stretching frequencies in the 400-600 cm-1 region sup- ports the view that iodination of the asphaltene samples did not occur'. crystalline. Xost charge-transfer complexes of iodine with aromatics are An exception to this is the violanthrene-iodine system, which x-ray diffraction indicates to be amorphous (2). X-ray results also indic'ate a low degree of order for the asphaltene- iodine Complexes. If the acceptors (I2) are homogeneously distributed in the host matrix (asphaltene), these systems may be considered analogous to the impurity or valence-controlled semiconductor systems. Disappearance of the 3.5i spacing of the (002) band means that the layered structure of asphaltene must have been altered (Fig. 7). The 4.68, y-band, due to the saturated carbon in the structure, did not change in the complexing process.
d :- / I i' I 495 :"ne ~CIJ hznd A: S.?h thcn nay bo iuc to the cx;>ansion of the zironatic intcrplsnzr. distazia to aliow for coir,plexing by the iodine no;ecule. 0 thc case of the ;>eryicnc-iodinc systcns, Liie spacing found at 10.7A was interpreced (3) as the distance bctwecn perylene moleculcs when iodine moiccnlcs were sandwiched between tiic aromatic layers. The present ob- served value of &.?A can be viewed as the sua of the intcrplanar distance (5.5.:) and the iodine length '(4 x l.j$). linked layers resembles that oi an intercalation compound of graphite (Fig. 6). Tile picture of these inter- . . Beferring again to Fig. 4, the room temperature resistivities for the two nztive asphaltenes are seen to be in tne insulator range (>lo14 Ohm). Upon addition of the iodine, the resistivity decreases about six decades or a niLlion fold. This is essentially the same behavior as that observed for polymeric charge-transfer complexes such as poly(viny1pyridium TCNQ) ar.6 its derivatives. These polymeric salts are dependent upon the TCNQ con- centration wnicn at best increases the conductivity six decades. Here !lave to point out that it is not easy to prepare a polymeric charge- rransfer complex with good semiconduction. In Slough (5) nade a number of polymeric complexes.from arosatic-containing polymers, with acceptors such GS cetracyanoechylene, chloranil, etc., and found the conductivities of these conplexes were not measurably higher than those of the original poly- meric donors. These mesomorphic materials may lack the order of the K- systems needed to open a path for charge carriers. More likely, the aroGtic systems are too small to form stable charge-transfer complexes.
- Page 448 and 449: helium 444 CORONA REACTOR SYSTEM Fi
- Page 450 and 451: 446 The ultraviolet spectrum. for t
- Page 452 and 453: Biphenyl Fraction 448 The low molec
- Page 454 and 455: LUd The actual structural definitio
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- Page 458 and 459: ’. 454 Mechanism I The available
- Page 460 and 461: 456 , , . The relatively low yield
- Page 462 and 463: 458 h/lethylacetylene, allene and b
- Page 464 and 465: Introduction VAPOR PHASE DECOMPOSIT
- Page 466 and 467: 462 more efficient hydrogenation. T
- Page 468 and 469: 464 place in parallel with fragment
- Page 470 and 471: 466 P rl 0, k 7 rnI rn al k a I hl
- Page 472 and 473: 458 TABLE I. COMPOSI'IION OF GASEOU
- Page 474 and 475: REFERENCES 1. C. Hirayama and D. A.
- Page 476 and 477: i 472 Reciprocal Arc Enthalpy ,-> F
- Page 478 and 479: 474 be pumped down without altering
- Page 480 and 481: 476 Instead a hydrogen deficient fi
- Page 482 and 483: i 478
- Page 484 and 485: 480 FATTY ACIDS AND n-ALKANES IN GR
- Page 486 and 487: 482 TA5L,E 2. - Carbon number distr
- Page 488 and 489: 6. 7. a. 9. 484 Lawlor, D. L., and
- Page 490 and 491: ' I ' Sample No. 6 ' 12 IO 8 6 z 4
- Page 492 and 493: . 488 uiolecular weight of which ca
- Page 494 and 495: Xississippi (Sample GS). Stock solu
- Page 496 and 497: 492 found at 5.7 and 4.9& for the W
- Page 500 and 501: For pure polynuclcar arom.i;ic hydr
- Page 502 and 503: - '-'. . ' . . values are listed in
- Page 504 and 505: 500 (1;) Ten, T. 17.: a;1d,Dic;
- Page 506 and 507: - ~ Resistivity Czlculation 2: 1 j:
- Page 508 and 509: 504 o ' C 0s 2 0 v x i 8 2 0 ! P -
- Page 510 and 511: 506 i
- Page 512 and 513: d 601 L P LL
- Page 516 and 517: I I I I I I I I m W N W N 0 (D ? 0
- Page 518 and 519: 514 was heated under nitrogen in a
- Page 520 and 521: The line broadening at 79OK of the
- Page 522 and 523: 13. 14. 15. 16. 17. 18. 19. 20. 21.
- Page 524 and 525: W L, Z 6 m (1: 0 6 d j o 2 ' 1 0.0
- Page 526 and 527: Coals 522 Studies of the 1600 cm-l
- Page 528 and 529: L in ole i c a c id - 0' Two sample
- Page 530 and 531: 526 Table 1.- Ultimate analyses of
- Page 532 and 533: 528 6. Friedel, R. A., and H. Retco
- Page 534 and 535: egeneration. The system can be seen
- Page 536 and 537: 532 and can be expressed in terms o
- Page 538 and 539: 534 in the vapor increases with inc
- Page 540 and 541: NH3 NH3 NH3 NH3 Pyridine Pyridine P
- Page 542 and 543: Mole Ratio of Test No. Quinoline to
- Page 544 and 545: IXPROFJCTION D; M. Mason Institute
- Page 546 and 547: -4:c~rciiny to recent studies o ;i4
494<br />
mechanisms. However, the voltade dependence for the current at a relatively<br />
low electric field is linear, indicating that Ohm's law is valid (Fig. 3).<br />
I<br />
This adherence to Ohm's law supports the belief that the conduction is<br />
electronic (19).<br />
The fact that the asphaltene-iodine sample exhibits (Fig. 6)<br />
strong enhancement <strong>of</strong> absorption near 1080 crn'l suggests that an iodine<br />
molecule forms a donor-acceptor complex with the aromatic portion <strong>of</strong> the<br />
asphaltenes. It is known that the iodine molecule forms such a charge-<br />
transfer complex with benzene and other alkylated benzenes, and that<br />
these complexes, in general, exhibit bands from 9 9 cm'l to 1200 cm'l<br />
(24,25).<br />
Arguing from analogy, it is plausible that the complex assumes<br />
the axial model (model A <strong>of</strong> Mulliken) while the acceptor molecule is sitting<br />
perpendicular to the plane. <strong>of</strong> the aromatics (26).<br />
Further, our failure<br />
to' locate any C-I stretching frequencies in the 400-600 cm-1 region sup-<br />
ports the view that iodination <strong>of</strong> the asphaltene samples did not occur'.<br />
crystalline.<br />
Xost charge-transfer complexes <strong>of</strong> iodine with aromatics are<br />
An exception to this is the violanthrene-iodine system,<br />
which x-ray diffraction indicates to be amorphous (2).<br />
X-ray results also indic'ate a low degree <strong>of</strong> order for the asphaltene-<br />
iodine Complexes. If the acceptors (I2) are homogeneously distributed in<br />
the host matrix (asphaltene), these systems may be considered analogous<br />
to the impurity or valence-controlled semiconductor systems. Disappearance<br />
<strong>of</strong> the 3.5i spacing <strong>of</strong> the (002) band means that the layered structure <strong>of</strong><br />
asphaltene must have been altered (Fig. 7).<br />
The 4.68, y-band, due to the<br />
saturated carbon in the structure, did not change in the complexing process.