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.
-
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-
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--
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-
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5. GLACIAL MODELS 95
areas. Sediment gravity flows and other
mass movements are the dominant pro-
cesses in both Alaska and eastern
Canada. Active channels typically tend
to fill with graded gravels (Fig.
34C).
Abandoned channels are plugged by
muds and rain-out diamict facies (see
base of log shown in Fig. 33; Eyles,
1987), recording the release of coarse
glacial
outwash from glaciers that have
advanced to the shelf break (Fig. 3).
Interchannel areas receive large vol-
umes of suspended sediment, together
with debris bulldozed over the shelf
break by the ice sheet. Interpretation of
seismic profiles suggests the presence
of massive debris flow facies (reworked
muds with scattered clasts; Figs.
34A,
B, D) that are broadly channelled in
cross section and which thin downslope
and interfinger with laminated muddy
turbidites. The term till tongue is unfortu-
nately still used to describe such debris
flow units. Large-scale slumping of the
upper and mid slope areas generates
large rafts of slumped sediment, and
creates an irregular slope relief subse-
quently
infilled and smoothed by sedi-
ment ponding.
The formation of ice sheets results in
global lowstands of sea level, with shore-
lines close to the shelf-slope break. The
sediment delivered directly to the
shelf-
slope break is largely resedimented
downslope as turbidity currents. Conse-
quently, base of slope and basin plain
settings during periods of global
lowstand
are dominated by thick, sandy turbidites,
as discussed in Chapter 13.
FACIES SUCCESSIONS AND
BOUNDING DISCONTINUITIES
IN GLACIATED BASINS
The concepts of sequence stratig-
raphy allow the subdivision of the sedi-
mentary record into depositional se-
quences bounded by unconformities
(Chapters 1, 2). The unconformities
are thought to have formed as a result
of globally synchronous (eustatic) sea
level changes and have been used to
construct worldwide stratigraphic corre-
lations. However, the recognition of
eu-
static sea level changes in glaciated
basins is very difficult, given the num-
ber of other processes which create
relative changes in sea level. The de-
velopment of large continental ice
sheets produces global changes in sea
level (glacio-eustacy) because large
volumes of water are locked up as ice
(Chapter
2).
In addition to glacio-eu-
static changes,
glacio-isostatic sea lev-
el changes are caused by ice loading
and unloading of the Earth's crust. This
results in elevation or depression of
the
seafloor and thus creates relative
changes in sea level and water depths
local to the glaciated basin. Variation
in the magnitude of crustal loading ac-
ross a glaciated basin can cause one
part of the basin to experience a fall in
relative sea level at the same time as
water depths are increasing elsewhere
in the basin. The combination of these
effects in glaciated basins makes as-
sessment of the stratigraphic signifi-
cance of individual unconformity sur-
faces extremely difficult.
A simple model for the deposition of
sequences on glaciated shelves is
based on the movement of ice out onto
the shelf at times of glacio-eustatically
lowered sea level. This erosional event
creates a sequence boundary.
Ice-
contact depositional systems (Fig.
3)
deposited against the advancing ice
margin will not survive glacial advance
but will be reworked subglacially as de-
formation till and/or be recycled to the
ice front as a morainal bank. The shelf
break and deep water will ultimately
stop the advance of the ice margin.
Much of the sediment pushed across
the continental shelf by advancing ice
will be discharged down the slope.
The position of ice margins that have
moved onto continental shelves is con-
trolled not so much by climate but by
crustal downwarping below and
around the ice sheet (Fig. 35). Down-
ward flexing of the crust, and displace-
ment of mantle material beneath and
immediately adjacent to the ice sheet,
is reflected in the formation of a pe-
ripheral forebulge (Fig. 35, top right
and left). The crust can be depressed
by as much as 600 m below the ice
sheet and for some distance beyond
the ice margin. Such crustal depres-
sion far exceeds the magnitude of
glacio-eustatic sea level drop (approxi-
mately 150 m; see Chapter 2) and so
creates the situation where high rela-
tive sea levels occur around the ice
margin at times of global glacio-eu-
static sea level low stand. The
fore-
bulge migrates away from a growing
ice sheet to a distance of several hun-
dred kilometres from the ice margin,
and collapses as the ice sheet re-
treats. This gives rise to a very complex
succession of sea level changes (re-
sulting from both glacio-eustatic and
glacio-isostatic adjustments) through-
out the glacial cycle and across
glaciated continental shelves.
In the simple model of an ice sheet
margin that has moved out to the conti-
nental shelf edge, the increase in water
depths caused by glacio-isostatic
downwarping
(i.e. a deepening of rela-
tive sea level) may be sufficient to ini-
tiate deglaciation by extensive calving
along the ice margin. This situation pro-
duces high ice flow rates (Hughes,
1987) which cause large volumes of
subglacial debris and meltwater to be
flushed to the ice margin (Eyles et al.,
1991). Poorly integrated networks of
tunnel valleys composed of
steep-
sided, flat-floored channels, and cut by
meltwater or fluidized sediment, may
result from this process. These valleys
are a common feature of unconformity
surfaces on glaciated shelves (Boulton
and Hindmarsh, 1987).
Most glaciomarine sedimentation
occurs during glacier retreat when large
volumes of meltwater are available.
Thick fining-upward successions, con-
sisting of relatively coarse-grained
ice-
contact deposits overlain by finely la-
minated proglacial silts, result from
glacier retreat. At the end of the glacial
cycle when ice has retreated from the
marine environment, crustal rebound
results in rapid shallowing of the coastal
margin (Fig. 35, bottom). Deeper water
muds will be uplifted and eroded,
thereby creating sequence bounding
un-
conformities in shallower parts of the
basin. Initial rates of rebound are ex-
tremely rapid and may approach several
metres per year. Thereafter, rates de-
crease exponentially and about 10,000
years after the end of the glacial cycle,
isostatic rebound is essentially complete
(Fig. 35, bottom). The coastal margin
may subsequently be flooded by
continuing postglacial eustatic sea
level rise (Fig. 35, bottom). In offshore
areas that escaped rebound into
shallow water, postglacial flooding of
the shelf results in mud deposition.
Thus, erosion in one part of the basin
can be coeval with flooding and depo-
sition elsewhere. Boulton (1990) pre-
sents a very useful summary of com-
plex sea level variations across gla-
ciated basins and describes the re-
sulting architecture of glaciomarine
sedimentary sequences and their