SEDIMENTARY EVIDENCE FAVOURING
THE FORMATION OF ROGEN LANDSCAPES BY OUTBURST FLOODS
John Shaw
Department of Earth and Atmospheric Sciences
University of Alberta
Edmonton, Alberta, Canada, T6G 2E3
E-mail: John.Shaw@ualberta.ca
ABSTRACT
Rogen landscapes are defined by the morphology
of the ridges and troughs and their locations in areas of former glaciation.
They are transitional with hummocky and drumlin landscapes in associations
of subglacial bedforms. This paper concentrates on the sediments within
Rogen ridges and approaches their interpretation by way of the fundamental
mechanics of high Reynolds Number flow beneath a wavy ice bed. The morphology,
sedimentary characteristics and landscape associations of Rogen terrain
are interpreted to record outburst flood from beneath the mid-latitude
Pleistocene ice sheets. Analogous sediments to those in Rogen ridges are
found around violently eruptive volcanoes and in areas inundated by outburst
floods in modern environments. These sediments are deposited from highly
turbulent, hyperconcentrated flows. Flood volumes of the order 106
km3 have implications for ice-sheet/climate/ocean interactions
that are not recognized in present models. These implications are presented
as speculations assuming the reality of outburst floods of huge magnitudes
and short duration.
INTRODUCTION
Rogen "moraines", like drumlins, are familiar
to the point where they are easily and confidently recognized - see Hättestrand
(1997) for an excellent review of the characteristics and the history of
ideas on Rogen moraines. Such familiarity commonly leads to a loose definition
of Rogen landscapes. The resulting problems are compounded when definitions
imply genesis.
A simple definition of the Rogen landscape
is adopted here, using the term
landscape to include geomorphology
and sedimentology. Thus, the Rogen landscape is defined as: Fields of ridges
and troughs arranged transverse to flow (Figs. 1
and 2). Some ridges may be fluted or drumlinized,
and some troughs may contain large, circular depressions. Ridges may contain
beds truncated at the land surface or beds that are conformable with the
ridge surface. It is common to find angular boulders of the underlying
bedrock in the troughs and on ridge surfaces. The Rogen landscape is found
in areas of former glaciation.
Qualifications regarding distance from
ice divides or the thermal regime of the ice during formation of the Rogen
fields would introduce inference and unduly complicate the definition.
The Rogen landscape has analogs in deserts, on the seabed of continental
shelves, and in ripples eroded upwards into river ice (Fig.
1).
Since the surface rocks and unlithified
sediments of Rogen landscapes are highly variable (see Hättestrand
1997, his Table 1), a universal depositional mechanism for Rogen
formation is ruled out. From theory and observation Rogen ridges may form
in different ways: (i) by erosion of the adjacent troughs (e.g., ridges
with truncated beds (Munro and Shaw 1997) and giant ripples cut in bedrock
(Cox 1998)); (ii) by deposition (e.g., ridges containing sedimentary beds
conformable with the surface morphology (e.g., Fisher and Shaw 1992));
or (iii) by a combination of erosion and deposition (Fig.
1). Rogen ridges composed of angular blocks of locally derived bedrock
in a finer grained matrix are the main topic of this paper (Fig.
3).
Many Rogen ridges contain folds and thrust
planes that are generally assumed to have resulted from direct glacial
action (Shaw 1979; Hättestrand 1997). Since bed shear stresses and
lift (Gerhardt and Gross 1972) generated by high velocity fluids may also
produce large folds and thrusts, it is best not to assume a glacial origin
for these tectonic features.
SUBGLACIAL MELTWATER PROCESSES:
FUNDAMENTALS
Yalin (1972) illustrated waveforms in fluids
and explained bed formation in terms of varying rates of deposition and/or
erosion with distance (Fig. 4). Similarly,
Allen (1982) described erosional and depositional bedforms caused by preferential
erosion around obstacles and/or deposition or reduced erosion to the lee
of the obstacles (Fig. 5). The principles
illustrated in Figures 4 and 5
are fundamental to the understanding of Rogen landscapes - the creation
of bedforms is simply the result of rates of change of bed height over
distance (Fig. 4). Such bedforms may result
from the action of different agents (e.g., wind, flowing water) and different
processes (e.g., abrasion by tools in flowing ice or sand blasting by saltating
grains).
The meltwater hypothesis presented here
for Rogen terrain assumes there were waves, similar to those beneath
river ice (Fig. 1), carved into the underside
of former ice sheets by broad meltwater flows (Fig.
6). Flow depicted in
Figure 6 is a generalization
of extremely complex, turbulent and turbid flows. As well, the locations
of erosion and deposition are derived from this generalization which, by
considering only time-averaged characteristics, is deceptively simple.
It is also qualitative - a complete physical and mathematical analysis
of such flow requires an understanding of: (i) the non-linear flow of ice
under high pressure gradients; (ii) non-uniform, unsteady, and highly turbulent,
meltwater flow with a hyperconcentrated suspension load; and (iii) non-uniform
rates of erosion, sediment transport, and deposition which are non-linear
functions of bed shear stress. While such problems cannot be solved at
present, we can safely assume that constrictions are zones of erosion and
expansions are zones of deposition. Furthermore, the Bernoulli principle
dictates that zones with high fluid velocities experience low pressures
(Fig. 6). Application of the Bernoulli equation,
using previous estimates for discharge per unit width, flow depth and overburden
pressure (Shaw 1996), gives lift capable of plucking slabs of bedrock 1.5
m thick.
Local low pressures associated with vertical
vortices or kolks (Matthes 1947) would generate much larger lift forces,
capable of plucking thicker slabs and creating folds and diapirs in soft
beds. Bed shear stress exerted by flowing water, which increases with v2
(where v is velocity) (Gerhardt and Gross 1972), may then stretch diapirs
in flame structures several tens of metres long.
SEDIMENTARY ROGEN RIDGES
Description
Greater erosion at troughs than at ridges
is implicit where underlying beds are truncated by extensive, landscape
unconformities. Troughs commonly contain large boulders or exposed bedrock,
and ridges are composed of remnant materials (till, fluvial sediments,
organic deposits or bedrock) and large boulders transported from the trough
immediately upflow are found perched on ridge surfaces (Fig.
3). The perched boulders are very angular with sharp edges.
Tectonic features, thrust and normal faults,
folds and overfolded diapirs are common in the remnant materials of erosional
ridges (Shaw 1979); Munro and Shaw 1997). By contrast, many Rogen ridges
with conformable architecture (internal structure corresponding to external
form) contain angular blocks of local bedrock (Fig.
7a), graded sand with minor deformation around large clasts (Fig.
7b) and graded beds in granules, sand or silt (Fig.
7c). Angular slabs of bedrock, which may be as much as one metre thick
and five metres long, are usually imbricate with upstream dip (Fig.
7d) (Shaw 1979).
Interpretation
Ridges with truncated strata of earlier geological
formations are evidently remnants around which depressions were eroded
into the surrounding bed. Those with conformable architecture and sorted
sediments are more likely depositional. Angular blocks in a fine grained
matrix suggest erosion by hydraulic plucking, transportation in hyperconcentrated
flow and rapid deposition from suspension (Maizels 1989). High flow velocities
are required to generate the lift forces for hydraulic plucking (Matthes
1974) and high shear stresses generated by fluid flow combined with high
lifting forces best explain the diapirism and flame structures. Fast deposition
is expected at expansions where flow decelerates quickly (Fisher and Shaw
1992) (Fig. 6). Thus, bedrock eroded from
an up-flow trough is deposited in the ridge immediately down flow (Fig.
6).
Angular bedrock blocks arranged like currents
in a cake in a finer, polymodal matrix are seen in other depositional environments:
(i) overlying landscape unconformities (erosional surfaces) and along probable
outburst flood paths (Fig. 8); (ii) around
eruptive volcanoes (Fig. 9), and (iii) along
well documented outburst flood paths (Fig. 10).
Violently turbulent, hyperconcentrated flows characterize these environments
and, although the details of transport and depositional processes are beyond
our understanding, the resulting sediments tell of rock slabs torn from
the bed, enormous concentration of suspended sediment, and extremely fast
deposition. As well, the tectonic structures are explained in this hypothesis
by the enormous lift and drag forces associated with flows of high Reynolds
Number.
CONCLUSIONS
It is clear that Rogen landscapes result from
coherent flow patterns at the regional scale (100's km, Fig.
2). Ridges record flows that were confined to valleys or diverged over
plateaus and plains (Fig. 2). Since such ridges
are observed at great distances from ice divides (Fig.
1c), their distribution is not, as is commonly believed (see review
by Hättestrand 1997), restricted to the inner zones of former ice
sheets. On the other hand, Rogen landscapes are best developed near proposed
divides of the Laurentide and Fennoscandian ice sheets. Scoured bedrock,
extending down flow from the Rogen landscapes, implies erosion, perhaps
corresponding to flow acceleration where isostatic effects caused the land
surface to rise towards the ice bed and reduced the flow cross-sectional
area.
Subglacial landscapes indicate a continuum
between fluting, drumlins, Rogen, and hummocky terrain (Shaw 1996; Munro
and Shaw 1997) and these subglacial landforms were probably formed by regional-scale
flows. The bedding and architecture of these ridges and the postulated
flow conditions presented here strongly support a meltwater origin for
Rogen landscapes.
Large, angular blocks of local bedrock
and fine-grained suspension deposits are explained well by hydraulic plucking
at flow constrictions and rapid sedimentation in areas of flow expansion
(Fig. 6). Thus, meltwater processes best explain
field observations of form, pattern and internal composition. Other mechanisms
such as a combination of polythermal beds and flow extension where warm-based
ice passes upflow into cold-based ice (Hättestrand 1997) do not account
for the full range of Rogen landscape characteristics. A reconstruction
of subglacial bed formation by outburst floods, including Rogen landscapes
forming beneath waves eroded into the overlying ice portrays a vivid picture
of the imagined scene (Fig. 11). Figure
11 also illustrates the surface material in various areas of the reconstruction.
IMPLICATIONS
-
If drumlin, Rogen and hummocky landscapes
record floods on the scale of the former ice sheets, then the ice sheets
themselves must have been partly floating on water sheets.
-
Volumes of water required to sustain such
floods would have been on the order 106 km3 equivalent
to a rise of several metres in sea level over a matter of weeks (Shaw 1996).
-
Hyperconcentrated, freshwater turbidity currents
of this magnitude would have extended beneath much of the North and South
Atlantic Oceans. Deposition would have resulted in cold, freshwater plumes
rising through the ocean water column causing abrupt changes in sea surface
temperature and salinity. Such changes, had they occurred, hold significant
implications for climate modelling (cf. Peng et al. 1995).
-
Rapid sea level rise is also expected to have
destabilized ice sheets extending over continental shelves.
As far as I know, there has been no
attempt to model events of the magnitude of the outburst floods postulated
by the meltwater hypothesis for subglacial landscapes. Perhaps, these speculations
will prompt some brave numerical analyst to give it a try.
ACKNOWLEDGEMENTS
Mandy Munro-Stasiuk, Alanna Vernon, Michael
Fisher, and Randy Pakan provided much needed help with the final preparation
of this paper. Many people, particularly Bruce Rains, have supported me
when I needed it most. I would like to thank NSERC Canada for financial
support.
REFERENCES
Allen, J.R.L. 1982. Sedimentary
Structures. Elsevier, Amsterdam, 663 pp.
Carey, N.C. 1991. Transportation and deposition
of tephra by pyroclastic flows and surges. In Fisher, R.V. and Smith, G.A.,
Editors. Sedimentation in Volcanic Settings. Society for Sedimentary
Geology, Special Publication 45, 39-57.
Cox, D.E. 1998. Transverse
drift ridges - giant current ripples? www.sentex.net/~tcc/moraine.html
Fisher, T.G. and Shaw, J. 1992. A depositional
model for Rogen moraine, with examples from the Avalon Peninsula, Newfoundland,
Canada. Canadian Journal of Earth Sciences, 29, 669-686.
Gerhardt, P.M. and Gross, R.J. 1972.
Fundamentals of Fluid Mechanics. Addison Wesley, Reading, 856 pp.
Hättestrand C. 1997. Ribbed moraine
in Sweden B distribution pattern and paleoglaciological implications. Sedimentary
Geology, 111, 41-56.
Maizels, J. 1989. Sedimentology, paleoflow
dynamics and flood history of jökulhlaup deposits: paleohydrology
of Holocene sediment sequences in southern Iceland sandur deposits.
Journal of Sedimentary Petrology, 59, 204-223.
Matthes, G.H. 1947. Macroturbulence in
natural stream flow. EOS American Geophysical Union Transactions,
28, 255-262.
Munro, M. and Shaw, J. 1997. Erosional
origin of hummocky terrain in south- central Alberta, Canada. Geology,
45(11),
1027-1030.
Peng, S.L. , Mysak, L.A., Ritchie H., Derome,
J., and Dugas, B. 1995. The difference between early and mid-winter atmospheric
responses to sea surface temperature anomalies in the northwest Atlantic.
Journal of Climate, 8(2), 137-157.
Shaw, J. 1979. Genesis of the Sveg till
and Rogen moraines of central Sweden: a model of basal melt out. Boreas,
8,
409-426.
Shaw, J. 1994. A qualitative view of sub-ice-sheet
landscape evolution. Progress in Physical Geography, 18, 159-184.
Yalin, M.S. 1972. Mechanics of Sediment
Transport, Pergamon, Oxford, 290 pp.
List of
Figures
Figure 1.
(a) Ripples on the underside
of river ice exposed by surface melt(courtesy of G. Ashton).
(b) Rogen landscape, Boyd
Lake, N.W.T., Canada
(c) Hummocky terrain including Rogen
landscapes, Stettler, Alberta, Canada. Note that the original air photograph
is enhanced by infilling depressions with black ink, as though they are
filled by water.
Figure 2.
Rogen landscape, Avalon Peninsula,
Newfoundland. The map represents all ridges observed on 1:50 000 scale
air photographs. The coherent, regional flow pattern (inset) was constructed
by assuming that flowlines were orthogonal to ridge crests (revised from
Fisher and Shaw 1992).
Figure 3.
Sediment exposed in Rogen ridge,
Anåkröken, central Sweden distal is to the left in the photographs.
(a) Panoramic view of the cross-section
(small car for scale), showing major erosional surfaces, boulder lag, and
forest bedding.
(b) Lower part of the exposure.
Crudely bedded, angular boulders derived from the local shale bedrock in
a multimodal matrix (gravel to silt). The boulders are imbricate with major
planes dipping proximally (Shaw 1979).
(c) Upper part of the exposure;
the sediment is finer and better stratified than that below. Sand and silt
in graded and cross laminae are common in this part of the section (see
(d)).
(d) Interbedded poorly sorted gravel
to silt with angular clasts and graded, fine sand and silt.
Figure 4.
Bedforms originating from imposed
surface waves (after Yalin 1972). t is time, x is distance from the start
of the erodible bed, qs is sediment transport rate, dqs/dx
is rate of change of qs with respect to distance, l is water
surface wavelength, L is bed wave length, and D is bed amplitude. Note
the direct relationship between zones of erosion and deposition and dqs/dx.
Figure 5.
Bedforms resulting from flow around
bluff obstacles (after Allen 1982). This figure provides a framework for
testing hypotheses on bedform genesis related to obstacles.
Figure 6.
Flow in ice and water related
to waveforms eroded in the ice roof. The Bernoulli principal dictates the
locations of high and low pressure and water velocities, which ultimately
control rates of ice drawdown and of bed erosion, sediment transport, and
deposition.
Figure 7.
Sediment in Rogen ridges.
(a) Poorly sorted boulders
to silt with angular, locally derived clasts, Lillholmsjö, Jämtland,
Sweden. Clean sand beneath boulder (arrowed).
(b) Graded, slightly deformed sand
with deformation structures around a boulder, Metagamie, Quebec. Graded
sand and silt laminae (arrowed).
(c) Parallel laminated silt and
fine sand overlying poorly sorted gravel to silt with angular clasts. Note
that some large clasts "float" in parallel bedded silt and fine sand (arrowed),
Anåkröken, Jämtland, Sweden.
(d) Imbricate, angular boulders
of local bedrock, Brigus Junction, Avalon Peninsula, Newfoundland. Scale
bar 20 cm.
Figure 8.
(a) Pyroclastic flow (after
Cary 1991).
(b) Pyroclastic base flow deposits.
Poorly sorted, crude bedding and very angular clasts, New Mexico (courtesy
of George Morris).
Figure 9.
(a) Poorly sorted gravel
to silt with angular clasts of local bedrock. Possible flood deposits Aberystwyth,
Wales.
(b) Poorly sorted boulders to silt
with large angular blocks and slabs of local bedrock. The upper face of
the large slab (left of figure) is striated and sculpted. Flow from right
to left. These beds lie on a landscape unconformity defining the surface
of drumlins. Pigeon Point, Clew Bay, Ireland.
Figure 10.
(a) Dry Falls, Washington
Scablands, the rock face of the falls is about 120 m high.
(b) Flood deposits of the Washington
Scablands. Poorly sorted, gravel to fine sand with angular clasts of locally
derived basalt interbedded with horizontally stratified medium to fine
sand. The conformable bedding indicates rapid sedimentation.
Figure 11.
Reconstructed flow conditions
during the formation of subglacial bedforms by outburst floods. The accompanying
photographs illustrate details of the landscape depicted in the reconstruction.
(a) Sediment in a depositional Rogen
ridge, Anåkröken, Jämtland, Sweden.
(b) Erosional drumlin, the Ovens,
Nova Scotia. Note: boulders similar in size to those on the modern beach
must have been transported by the drumlin forming process.
(c) Fluted bedrock adjacent to the
drumlin in (b) (courtesy of B. Taylor).
© 1998 John Shaw
11 December 1998