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chemical physics of discharges - Argonne National Laboratory

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Y<br />

'<br />

493<br />

..<br />

10E.G ~r,~-l {i;ig. 6) , and freshly ;,rc,,ar'cd asi'i~alecl-ic-iodine cosplexes in<br />

CSz also csiiibited an enhanccmcnr in absorprion 'in the regi<strong>of</strong>i <strong>of</strong> lOC0 to<br />

11 jO cn-1, w:IicIi is generally ascl-iilcu to complex iormation.<br />

Tile x-ray spectrograms in rile region 20 = 2 - 42" <strong>of</strong> the asphaltene'<br />

(mi)-iodine 'systca yielded in aiiior;),ious pattern with broad halos as shown<br />

. .<br />

in Xg. 7. For samples with an iodinc content <strong>of</strong> less tian 5 per cent,<br />

the j. ji band.stil1 appeared as ii siioulder.<br />

was fornad at a;oound 8.7a.<br />

In thc meantime a new band<br />

AT bigher'iodine conhenis (>IO$), the 3.5i<br />

band. has apparently disappeared and the 8.7x band became clearly visible.<br />

".<br />

liisrc is a general overall decrease <strong>of</strong> total intensity as $1 increases<br />

since the iodine itself absorbs an increasingly large fraction <strong>of</strong> the<br />

.. .<br />

diffracted x-rays. In the present case, the noise Level coupled with the<br />

intensity reduction has made the disappearance <strong>of</strong> the 3.51 shoulder dif-<br />

ficult KO detect.<br />

In gcnera1,the . . ESR,spectra obtained froqthe asphaltene-iodine<br />

samples indicated an incre,ase in free radical concentration with increase<br />

-in iodine content. The increase in relacive intensity for an asphaltene<br />

(Wj-iodine complex ,.containing 2@ I over the corresponding native asphal-<br />

. .<br />

tenes is about 3.8 fold.<br />

DISCUSSIOX'<br />

In all the samples studied, including both.native asphalcenes<br />

and their iodine. adducts, a negative temperature coefficient <strong>of</strong> resistivity<br />

was obtained.<br />

by the plots shown.in Fig. 2:<br />

The linearity <strong>of</strong> log D vs. reciprocal T .is substantiated<br />

The resistivity is inversely related to<br />

the concentration <strong>of</strong> the charge carriers (holes and electrons), but the<br />

fact that the number <strong>of</strong> charge-carriers increases exponentially with tempera-<br />

ture does not enable a choice to be made between electronic or ionic conduction<br />

"

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