chemical physics of discharges - Argonne National Laboratory
chemical physics of discharges - Argonne National Laboratory chemical physics of discharges - Argonne National Laboratory
492 found at 5.7 and 4.9& for the W asphaltene-iodine complex shifts were observed to 5.5 and 4.7A, respectively. The spacing is reproducible to I 9. ai. Eleztron S?in Resonance ESR spectra were taken with a Varian V-4502 x-brand EPR spectrometer system in conjunction with a 12-inch magnet and a "Fieldial." intenslty observed was used as a guide for the spin concentration of the asphaltene (VY)-iodine complexes and native asphaltene (VY) (13). RESULTS The relative All asphaltene-iodine samples studied gave repeatable linear relations in the temperature range investigated as shown in Fig. 2. is no significant deviation from Ohm's law through the range 2.5 to 97 V as indicated by Fig. 3 in the temperature interval 313" to 372"K. insulator range. There The native asphaltenes (Points 1, Fig. 4) fall generally in the Upon the addition of iodine the resistivity f;Lls, 5 to - b, then increases sharply, to c, and finally drops, 5 to a, as iodine content rises. Both complexes appear to yield curves of similar shape. The gap energy values for the asphaltene-iodine complexes are plotted versus their iodine contents (Fig. 5). . The smallest energy gap measured in each case was -Q.5eVf but the absolute minimum is uncertain, These minima (points b) correspond to the sharp transitions of resistivity shown in Fig. 4.. Scanning in the far IR region revealed no C-I stretching frequencies for those iodine complexes for which 0 was determined. However, the dif- ferential IR measured in the 7OO-l2OO cm-1 did show an additional band at
i' I Y ' 493 .. 10E.G ~r,~-l {i;ig. 6) , and freshly ;,rc,,ar'cd asi'i~alecl-ic-iodine cosplexes in CSz also csiiibited an enhanccmcnr in absorprion 'in the regiofi of lOC0 to 11 jO cn-1, w:IicIi is generally ascl-iilcu to complex iormation. Tile x-ray spectrograms in rile region 20 = 2 - 42" of the asphaltene' (mi)-iodine 'systca yielded in aiiior;),ious pattern with broad halos as shown . . in Xg. 7. For samples with an iodinc content of less tian 5 per cent, the j. ji band.stil1 appeared as ii siioulder. was fornad at a;oound 8.7a. In thc meantime a new band AT bigher'iodine conhenis (>IO$), the 3.5i band. has apparently disappeared and the 8.7x band became clearly visible. ". liisrc is a general overall decrease of total intensity as $1 increases since the iodine itself absorbs an increasingly large fraction of the .. . diffracted x-rays. In the present case, the noise Level coupled with the intensity reduction has made the disappearance of the 3.51 shoulder dif- ficult KO detect. In gcnera1,the . . ESR,spectra obtained froqthe asphaltene-iodine samples indicated an incre,ase in free radical concentration with increase -in iodine content. The increase in relacive intensity for an asphaltene (Wj-iodine complex ,.containing 2@ I over the corresponding native asphal- . . tenes is about 3.8 fold. DISCUSSIOX' In all the samples studied, including both.native asphalcenes and their iodine. adducts, a negative temperature coefficient of resistivity was obtained. by the plots shown.in Fig. 2: The linearity of log D vs. reciprocal T .is substantiated The resistivity is inversely related to the concentration of the charge carriers (holes and electrons), but the fact that the number of charge-carriers increases exponentially with tempera- ture does not enable a choice to be made between electronic or ionic conduction "
- Page 446 and 447: 442 CHEMICAL REACTIONS IN A CORONA
- 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
- Page 456 and 457: I I I I I In m 9 In 2 , I: r- In m
- 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 498 and 499: 494 mechanisms. However, the voltad
- 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
492<br />
found at 5.7 and 4.9& for the W asphaltene-iodine complex shifts were<br />
observed to 5.5 and 4.7A, respectively. The spacing is reproducible to<br />
I<br />
9. ai.<br />
Eleztron S?in Resonance<br />
ESR spectra were taken with a Varian V-4502 x-brand EPR spectrometer<br />
system in conjunction with a 12-inch magnet and a "Fieldial."<br />
intenslty observed was used as a guide for the spin concentration <strong>of</strong> the<br />
asphaltene (VY)-iodine complexes and native asphaltene (VY) (13).<br />
RESULTS<br />
The relative<br />
All asphaltene-iodine samples studied gave repeatable linear<br />
relations in the temperature range investigated as shown in Fig. 2.<br />
is no significant deviation from Ohm's law through the range 2.5 to 97 V<br />
as indicated by Fig. 3 in the temperature interval 313" to 372"K.<br />
insulator range.<br />
There<br />
The native asphaltenes (Points 1, Fig. 4) fall generally in the<br />
Upon the addition <strong>of</strong> iodine the resistivity f;Lls, 5 to<br />
- b, then increases sharply, to c, and finally drops, 5 to a, as iodine<br />
content rises. Both complexes appear to yield curves <strong>of</strong> similar shape.<br />
The gap energy values for the asphaltene-iodine complexes are plotted<br />
versus their iodine contents (Fig. 5). . The smallest energy gap measured<br />
in each case was -Q.5eVf but the absolute minimum is uncertain, These<br />
minima (points b) correspond to the sharp transitions <strong>of</strong> resistivity shown<br />
in Fig. 4..<br />
Scanning in the far IR region revealed no C-I stretching frequencies<br />
for those iodine complexes for which 0 was determined. However, the dif-<br />
ferential IR measured in the 7OO-l2OO cm-1 did show an additional band at