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| AGU Fall Meeting, Presentations | Cite abstracts as Eos
Trans. AGU, 83(47), Fall Meet. Suppl., Abstract xxxxx-xx, 2002 |
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HR: 16:10h
* Strong, N
Sheets, B Kelberer,
M Kim,
W Paola,
C We use results from an experimental study conducted in the XES subsiding-floor basin at St. Anthony Falls Laboratory to examine changes in valley width and depth during base-level fluctuations. We find that during a slow base level cycle, where the time scale of base level change was greater than the basin's theoretical equilibrium time, no clear incised valley formed, but rather a series of broad erosional surfaces. During rapid base level cycles, where the time scale of base level change was considerably less than the basin equilibrium time, incised valleys formed via a complex, step-like process: autogenic incision interacted with the externally imposed base-level change to produce multiple discrete down-cutting episodes, despite continuous base-level fall. Downstream deposition during the fall helped widen the valley downstream, producing a tapered planform comparable to that found in many natural estuaries. Deposition during the rise produced continued valley widening. Shoreline migration for both cycle frequencies was well predicted by a simple geometric model and showed no tendency to drift out of phase with base level.
http://www.safl.umn.edu/ |
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HR: 16:40h
* Hasbargen, L Paola,
C
Drainage basins experiencing long term uplift and erosion can evolve
to a statistically stable form (a steady state), where the average erosion
rate balances the average uplift rate. The possibility that this state
develops has been demonstrated by numerical and experimental models, and
by some natural drainage basins. In this paper we investigate erosion
rate variability in numerical and physical experiments of drainage basin
scale erosion. For numerical models, the ultimate state at steady forcing
conditions is a landscape that erodes everywhere at the same rate. Prior
to reaching this static steady state, numerical landscapes undergo some
evolution, such that the landscape experiences adjustments that lead to
lateral movement of ridges and valleys, and subsequent stabilization of
the network. For small scale physical experiments, such adjustments at
statistical steady state can be prolonged, and a static steady state is
never reached. We focus on several mechanisms that result in local variability
of erosion rate for landscapes at a statistical steady state. Such mechanisms
include 1) upstream area capture; 2) hillslope failures; 3) knickpoint
generation and propagation; and 4) temporary deposition in valleys. Each
mechanism operates at varying time scales. Upstream area capture typically
involves closure of a valley, with higher erosion rates on hillslopes
in adjacent valleys, and occurs over longer time scales. Divide migration
is an integral part of upstream area capture. Hillslope failures are shorter
time scale processes, and involve local fluctuations in erosion rate.
In our physical experiments, we have observed episodes of widespread deposition
in valleys, followed by knickpoint generation and excavation of the stored
sediment. Such cycles occur over the time required for a knickpoint to
propagate through the network. Temporary depositional cycles in our experiment
are autocyclic, that is, they arise from local process interactions. The
interaction of these processes leads to fairly significant variances in
erosion rate across the landscape. Characteristic patterns of erosion
rate exist for ridge migration, and to a lesser degree, for temporary
sediment storage and knickpoint propagation. Hillslope failure patterns
do not appear to have any structure. Advances in topographic measurement,
surface exposure dating, and rock exhumation rates are offering the possibility
that we can measure erosion rates in field settings on a very detailed
basis. Theoretical and experimental data can provide valuable insights
for interpreting erosion rate variability in natural settings. 1815
Erosion and sedimentation |
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