STRUCTURAL VARIATIONS IN CHRYSOTILE ASBESTOS FIBERS REVEALED BY SYNCHROTRON X-RAY-DIFFRACTION AND HIGH-RESOLUTION TRANSMISSION ELECTRON-MICROSCOPY

Citation
Ba. Cressey et al., STRUCTURAL VARIATIONS IN CHRYSOTILE ASBESTOS FIBERS REVEALED BY SYNCHROTRON X-RAY-DIFFRACTION AND HIGH-RESOLUTION TRANSMISSION ELECTRON-MICROSCOPY, Canadian Mineralogist, 32, 1994, pp. 257-270
Citations number
32
Categorie Soggetti
Mineralogy
Journal title
ISSN journal
00084476
Volume
32
Year of publication
1994
Part
2
Pages
257 - 270
Database
ISI
SICI code
0008-4476(1994)32:<257:SVICAF>2.0.ZU;2-6
Abstract
Four samples of chrysotile asbestos have been studied by synchrotron X -ray diffraction, One of these samples exhibits asymmetrical 00l diffr action profiles, and also shows characteristics of ''Povlen-type'' chr ysotile in X-ray fiber photographs. The 00/ peak asymmetry is interpre ted as indicating the presence of two layer-spacings, one about 7.3 an gstrom, in common with the other chrysotile samples, and one about 7.2 angstrom. TEM images of the chrysotile with two apparent layer-spacin gs show the presence of fibers with both curved and flat layers in a v ariety of disordered tubular structures having only approximate cylind rical symmetry. The flat layers in these fibers may have a smaller int erlayer-spacing (7.2 angstrom) relative to the curved layer-spacing (7 .3 angstrom) because of the possibility of increased hydrogen bonding between flat layers that are stacked in register with one another. In this sample, fibers with flat layers parallel to one direction only, j oined at each end by curved layers are observed to occur commonly. Als o present are fibers with polygonal-tube cores made up from flat layer s, with outer layers that are curved in a more normal way. This type o f structure appears to be the closest that has been observed to the al ternative structural model proposed by Middleton & Whittaker (1976) fo r ''Povlen-type'' chrysotile. In the same specimen, cylindrical chryso tile fibers that possess 5-fold symmetry have been imaged, in which th e layer stacking is apparently in register radially at 15 points aroun d the circumference, arising from the b/3 repeat of the hydroxyl layer .