Jf. Banfield et Sw. Bailey, FORMATION OF REGULARLY INTERSTRATIFIED SERPENTINE-CHLORITE MINERALS BY TETRAHEDRAL INVERSION IN LONG-PERIOD SERPENTINE POLYTYPES, The American mineralogist, 81(1-2), 1996, pp. 79-91
Serpentinite from Lancaster County, Pennsylvania, consists of a variet
y of fine-grained serpentine minerals, chlorite, randomly interstratif
ied serpentine-chlorite, and a series of phases based on regular inter
stratification of serpentine and chlorite (SxCy, where x and y are int
egers). Within the resolution of the AEM technique, all layer silicate
s have the same Mg-rich, Al-rich, Cr-rich, and Fe-poor compositions. R
egularly interstratified serpentine-chlorite minerals are frequently i
ntimately intergrown with serpentines that have repeat distances ident
ical to those of the regular interstratifications. Thus, dozyite (S1C1
, beta = 90 degrees) is intimately associated with serpentine with thr
ee-layer octahedral order (I,I,II). Longer period polysomes (S2C1, S1C
2, S2C2, S1C3, S3C2, and S1C4, all with beta = 90 degrees) are each ac
companied by serpentines with equivalent c-axis periodicities. SxCy ph
ases apparently form by selective growth of Ibb chlorite units from I,
II octahedral sequences in long-period serpentines. All microscopic st
ructural evidence is consistent with the formation of regular interstr
atifications by tetrahedral inversion within existing serpentine. Atom
ic resolution images reveal that the tetrahedral sheet is displaced by
a/3 where it inverts to form the 2:1 layer. A +/- a/3 shift is requir
ed for hydrogen bonding between OH of the newly formed brucite-like in
terlayer and O atoms of the 2:1 layer. The sense of the shift is deter
mined by the strong interactions between the octahedral cations in the
brucite-like interlayer and the Si in the 2:1 layer (direct superimpo
sition, previously described as a type-a interaction, is strongly unfa
vorable). Distortion at the inversion point probably lengthens Si-O bo
nds in the next tetrahedra, facilitating relocation of Si on the other
side of the basal O plane. Reversal of the octahedral slant in the 2:
1 layer occurs because the +a/3 tetrahedral shift necessitates reposit
ioning of O and OH coordinating octahedral cations, requiring movement
of octahedral cations from type-II to type-I positions. Except in the
2:1 layers, the stacking and octahedral slants are inherited. The res
ult is a series of regular interstratifications characterized by a sin
gle octahedral slant (specifically, Ibbb,I) and b/3 stacking disorder.
This analysis reveals the importance of cation-cation interactions in
determining the relative stability of pairs of 1:1 layers and in cont
rolling the detailed structures of layer silicates formed in solid-sta
te serpentine-to-chlorite reactions. Because similar constraints apply
to formation of serpentine from chlorite by direct structural modific
ation, the common 1T lizardite polytype may be produced from both IIbb
and Ibb chlorites.