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Geologic Studies in Alaska by the U.S. Geological Survey, 1992

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STRUCTURAL EVOLUTION OF THE CHUGACH-PRINCE WILLIAM TERRANE 147<br />

southwestern marg<strong>in</strong> and <strong>in</strong>ferred faults on its o<strong>the</strong>r mar-<br />

g<strong>in</strong>s. A nor<strong>the</strong>ast-southwest-strik<strong>in</strong>g fault corresponds with<br />

<strong>the</strong> boundary between doma<strong>in</strong> D and doma<strong>in</strong>s F and H. A<br />

fault with a similar orientation roughly corresponds with<br />

<strong>the</strong> doma<strong>in</strong> I-J boundary.<br />

FOLDS<br />

Fold<strong>in</strong>g <strong>in</strong> <strong>the</strong> study area is <strong>in</strong>dicated <strong>by</strong> rocks dipp<strong>in</strong>g<br />

<strong>in</strong> opposite directions, but hav<strong>in</strong>g <strong>the</strong> same strike and fac-<br />

<strong>in</strong>g direction. The wavelength of <strong>the</strong>se folds based upon<br />

our mapp<strong>in</strong>g (fig. 2) is commonly 1.5 to 2.5 krn, but may<br />

range from 1 to 4.5 krn. The amplitude of <strong>the</strong> folds is not<br />

known, although it is almost certa<strong>in</strong>ly greater than <strong>the</strong>ir<br />

wavelength. Because <strong>the</strong> wavelength is so large, fold<br />

h<strong>in</strong>ges were not generally observed. However, between<br />

M<strong>in</strong>ers Lake and Wells Bay <strong>in</strong> doma<strong>in</strong> C <strong>the</strong>re are gentle<br />

undulations of bedd<strong>in</strong>g with a wavelength of about 100 m<br />

that are probably at <strong>the</strong> crest of an anticl<strong>in</strong>e (M-folds). We<br />

generally do not have enough data to trace fold axes later-<br />

ally more than 2 to 3 km. In doma<strong>in</strong> C, however, con-<br />

glomerate marker beds allow a fold to be traced for 12 km.<br />

Stereograms of poles to bedd<strong>in</strong>g <strong>in</strong> each doma<strong>in</strong> help<br />

to def<strong>in</strong>e <strong>the</strong> geometry of <strong>the</strong> folds, and we determ<strong>in</strong>ed a<br />

best-fit fold axis for each doma<strong>in</strong>, if enough data had been<br />

collected to def<strong>in</strong>e a girdle. Four of <strong>the</strong> eleven doma<strong>in</strong>s did<br />

not have sufficient data (N r 20) to clearly discrim<strong>in</strong>ate<br />

fold axes. Although <strong>the</strong> trends of <strong>the</strong> best-fit fold axes are<br />

variable between doma<strong>in</strong>s, <strong>the</strong>se fold axes are sub-<br />

horizontal, except <strong>in</strong> doma<strong>in</strong> F, which has a different struc-<br />

tural style and is discussed separately below. Outside of<br />

doma<strong>in</strong> F, 12 mesoscale fold axes were measured, and <strong>in</strong><br />

most cases <strong>the</strong>se fold axes do not co<strong>in</strong>cide with <strong>the</strong> best-fit<br />

fold axes determ<strong>in</strong>ed from <strong>the</strong> girdle of poles to bedd<strong>in</strong>g.<br />

In correlative rocks to <strong>the</strong> southwest Bol and Gibbons<br />

(<strong>1992</strong>) (fig. 1) found that mesoscale fold h<strong>in</strong>ges were ori-<br />

ented similarly to <strong>the</strong> best-fit fold axis determ<strong>in</strong>ed from <strong>the</strong><br />

Figure 3. Form-l<strong>in</strong>e map of <strong>in</strong>terpretive strike of bedd<strong>in</strong>g (solid l<strong>in</strong>es) and structural doma<strong>in</strong>s, A to K (dotted l<strong>in</strong>es).<br />

Data for doma<strong>in</strong>s A and B also taken from unpublished mapp<strong>in</strong>g <strong>in</strong> Anchorage A-2 and Seward D-2 quadrangles<br />

north and west of study area <strong>by</strong> S.W. Nelson, M. Miller, J. Dumoul<strong>in</strong>, G. W<strong>in</strong>kler, S. Karl, and J. Case.

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