modeling hyporheic zone processes
TRANSCRIPT
Advances in Water Resources 26 (2003) 901–905
www.elsevier.com/locate/advwaters
Preface
Modeling hyporheic zone processes
1. Introduction
Stream biogeochemistry is influenced by the physical
and chemical processes that occur in the surrounding
watershed. These processes include the mass loading ofsolutes from terrestrial and atmospheric sources, the
physical transport of solutes within the watershed, and
the transformation of solutes due to biogeochemical
reactions. Research over the last two decades has iden-
tified the hyporheic zone as an important part of the
stream system in which these processes occur. The
hyporheic zone may be loosely defined as the porous
areas of the stream bed and stream bank in whichstream water mixes with shallow groundwater. Ex-
change of water and solutes between the stream proper
and the hyporheic zone has many biogeochemical im-
plications, due to differences in the chemical composi-
tion of surface and groundwater. For example, surface
waters are typically oxidized environments with rela-
tively high dissolved oxygen concentrations. In contrast,
reducing conditions are often present in groundwatersystems leading to low dissolved oxygen concentrations.
Further, microbial oxidation of organic materials in
groundwater leads to supersaturated concentrations of
dissolved carbon dioxide relative to the atmosphere.
Differences in surface and groundwater pH and tem-
perature are also common. The hyporheic zone is
therefore a mixing zone in which there are gradients in
the concentrations of dissolved gasses, the concentra-tions of oxidized and reduced species, pH, and temper-
ature. These gradients lead to biogeochemical reactions
that ultimately affect stream water quality. Due to the
complexity of these natural systems, modeling tech-
niques are frequently employed to quantify process
dynamics.
This special issue of Advances in Water Resources
presents recent research on the modeling of hyporheiczone processes. To begin this preface, a brief history on
modeling hyporheic zone processes is presented. This
background information is by no means complete; ad-
ditional information may be found in Streams and
Groundwaters [17] and the references therein. The
preface concludes with an overview of current re-
0309-1708/$ - see front matter � 2003 Published by Elsevier Ltd.
doi:10.1016/S0309-1708(03)00079-4
search needs and a summary of the articles in the special
issue.
2. Background
Twenty years ago, Bencala and Walters [1] analyzed
the results of a stream tracer experiment using a tran-
sient storage solute transport model (also know as a
�dead zone� model, e.g. [32]). Subsequent work by Ben-
cala, Jackman, McKnight, and coworkers [2,3,16,20]
established the use of stream tracers and the transient
storage model as a standard approach to quantifyingsmall stream hydrodynamics. In its simplest form, the
transient storage model consists of a one-dimensional
advection–dispersion equation [24] with an additional
term to account for transient storage. Transient storage
is defined as the movement of solutes from the free-
flowing main channel into zones of stagnant water,
temporary retention in the stagnant zones, and the
subsequent movement of solute mass back into the mainchannel. Stagnant zones include both surface features
(pools and eddies) and water within the hyporheic zone.
These stagnant zones are lumped together as a concep-
tual storage zone within the transient storage model.
Exchange of solute mass between the main channel and
the transient storage zone is controlled by an exchange
coefficient, a, and the cross-sectional area of the storage
zone, As.Concurrent with the establishment of the transient
storage paradigm, researchers began to recognize the
ecological importance of the hyporheic zone and the
effects of groundwater/surface water interaction on
biogeochemical reactions. In particular, studies of nu-
trient cycling [12,23,34] illustrated the close coupling
between hydrologic transport and biogeochemical pro-
cesses. The transient storage solute transport modelprovided a means to quantify this coupling, with the
transient storage parameters (a and As) providing a
means of quantifying hyporheic exchange [30]. In addi-
tion, the use of conservative stream tracers allowed re-
searchers to distinguish between the effects of hydrologic
and biogeochemical processes. Since the time of the
902 Preface / Advances in Water Resources 26 (2003) 901–905
Stream Solute workshop [30], numerous applications of
stream tracers and the transient storage model have
appeared in the literature [4,5,8,9,14,18,21,22,26,35]. In
addition, advances have been made in regard to field
techniques and modeling tools, e.g. [6,25].
3. Areas of research
Although much progress has been made in model-ing hyporheic zone processes, many challenges remain.
Three areas of research relevant to this special issue
are described here. As discussed by Bencala and
Walters [1], the transient storage model is an empirical
approach that does not attempt to model exchange in
a mechanistic manner. Further, surface storage and
hyporheic exchange are lumped together in a single
storage zone. Although it is sometimes possible to ruleout one of the mechanisms (e.g., a reach affected by
beaver dams may be dominated by surface storage,
whereas a shallow reach with a well defined channel
and porous streambed may be dominated by hypo-
rheic exchange), it is often difficult to distinguish be-
tween surface and subsurface storage. This distinction
is of paramount importance given the differences in
surface and groundwater biogeochemistry noted ear-lier and the ultimate goal of studying stream water
quality. On one hand it may seem trivial to formulate
model equations for multiple storage zones, but it is
quite another matter to develop practical field tech-
niques to correctly parameterize such a model. The
existing stream tracer approach [1] is unlikely to
provide sufficient information for the separation of
surface storage and hyporheic exchange.A second research issue is that of scale. Harvey
et al. [15] conclude that the standard modeling ap-
proach is only capable of identifying hyporheic ex-
change over relatively short-time scales (minutes to
hours). Exchange processes at longer time scales (tens
of hours to days), while important chemically, may
not be properly identified using stream tracer data.
Characterization of long time scale exchange has im-portant implications as solutes entering long hyporheic
flow paths have extended contact with reactive sur-
faces and attached microorganisms that conceivably
leads to enhanced biogeochemical transformation. In
addition to the issue of temporal scale, further work is
needed to identify the spatial scales at which hypo-
rheic exchange is important. With some notable ex-
ceptions [9,18], most investigations of hyporheicexchange have been conducted in low-order streams.
The importance of exchange in these small systems is
presently clear, e.g. [22]. Additional research in higher-
order streams will be needed before similar conclu-
sions can be drawn at larger spatial scales.
The final research issue discussed here is the need for
improved field and modeling techniques to more accu-
rately quantify biogeochemical processes. Biogeochem-
ically reactive solutes may undergo transformation in
the main channel and/or storage zone and the rates oftransformation may vary considerably given the bio-
geochemical gradients noted above. Although separa-
tion of main channel and storage zone processes is
possible using first-order rate coefficients [25], further
refinement in quantifying process dynamics remains a
challenge due to the possible range of storage zone
microenvironments. Processes and rates in surface
storage zones may be significantly different than thoseassociated with the hyporheic zone, and the residence
time (and thus reaction time) of solutes undergoing
short-time scale hyporheic exchange may be consider-
ably less than that for solutes entering longer hyporheic
flow paths. As noted above, multiple storage zone
models may be formulated, but estimation of the phys-
ical and biogeochemical parameters for each storage
zone may not be tractable using existing tracer tech-niques. At the other extreme, lumping the multiple
hydrologic and biogeochemical processes into a single
storage zone with average, aggregate properties may
not provide meaningful results for heterogeneous sys-
tems.
4. Overview of the special issue
The papers in this special issue address many areas
of needed research. With respect to the issues raised
above, several comments are in order. First, the pa-pers of Gooseff et al. [11] and Salehin et al. [27] em-
ploy alternate models of transient storage that may
provide a means of distinguishing between surface
storage and hyporheic exchange. Second, the papers of
Fox and Durnford [10] and Lin and Medina [19]
present approaches that more accurately describe the
groundwater system; these approaches may allow for
the consideration of hyporheic exchange at longertemporal and larger spatial scales. Third, Thomas et al.
[33] present a technique for distinguishing between
main channel and storage zone nutrient uptake, while
Sheibley et al. [29] present a modeling approach for
the transformation of nitrogen in hyporheic sediments.
Additional details on all of the papers in the special
issue are provided below.
Edwardson et al. [7] quantified hyporheic zone in-teractions in seven streams, ranging from first to fifth
order, in the Alaskan tundra. Despite the constraints of
cold temperatures and permafrost, they found that
hyporheic zone interactions were substantial from a
hydrologic and biogeochemical perspective. The hypo-
Preface / Advances in Water Resources 26 (2003) 901–905 903
rheic zone was a zone of degradation of dissolved or-
ganic nitrogen and a source of nitrate, carbon dioxide,
and ammonium in upwelling areas. Concurrent sam-
pling of interstitial waters indicated that parts of the
hyporheic zone did not fully equilibrate with the in-jected stream tracer during the duration of the exper-
iment.
Fox and Durnford [10] investigated the occurrence of
partially saturated conditions within the hyporheic zone
that occur when the water table in the aquifer drops
below the stream bed. Stream–aquifer interaction was
analyzed and the stream depletion rate was quantified
for three types of partially saturated conditions. Streamdepletion rates were incorporated into an analytical
solution of a pumping well adjacent to a stream, re-
sulting in partially saturated conditions beneath the
stream. The transient solution tracked the length along
the stream over which perched conditions develop.
Unsaturated conditions within the hyporheic zone may
lead to higher dissolved oxygen concentrations, limiting
transformation processes that are favored under anaer-obic conditions.
Gooseff et al. [11] characterized hyporheic exchange
processes in three reaches of Lookout Creek (Oregon,
USA). Parameters describing storage and exchange were
estimated using tracer data and two transport models: a
transient storage model with an exponential residence
time distribution and an alternate model based on a
general power-law residence time distribution. Resultssuggest that the transient storage model fit the short-
time tracer response adequately, but not the longer-term
behavior. The long tails in the tracer response were fit
reasonably well by the generalized residence time dis-
tribution model, except at very late times, when the
observed concentrations drop off steeply in contrast to
the model predictions.
Harvey et al. [13] analyzed changes in hydrologicretention by the hyporheic zone in a small desert stream.
During a five year period, growth of aquatic macro-
phytes resulted in a decreased flow rate and average
velocity and an increase in stream width. These hydro-
logic changes were associated with an order of magni-
tude increase in hydrologic retention. Temporal changes
in hydrologic retention in this desert stream and in other
streams were shown to correlate well with the Darcy–Weisbach friction factor, providing a potential guide for
evaluating changes in hyporheic zone characteristics
over time or at other locations.
Lin and Medina [19] developed a conjunctive stream–
aquifer model that couples the transient storage equa-
tions with modules for groundwater flow, groundwater
transport, and unsteady streamflow routing. The resul-
tant modeling framework considers the large-scale ex-change of solute between the stream and the underlying
aquifer and the effects of flood waves on groundwater/
surface water interaction. The coupled model was used
to illustrate the potential contamination of the ground-
water system during high flow events, and the subse-
quent release of solutes back into the stream during
recession of a flood wave.Salehin et al. [27] compared solute transport and
hyporheic exchange in vegetated and unvegetated
reaches of an agricultural stream using tracer data and
the advective storage path model. The stream reaches
analyzed were subject to extreme variations in vegeta-
tion and morphology due to seasonal effects and channel
excavation. Variation of solute storage time in non-
excavated reaches was attributable to differences instream flow depth, velocity, and hydraulic conductivity
of the streambed. Excavation altered stream channel
geometry, increasing the storage time and reducing the
effective exchange rate. Reach comparisons were facili-
tated by scaling model exchange parameters.
Schmid [28] developed analytical expressions for the
temporal moments of the transient storage equations,
for the case of an arbitrary upstream boundary condi-tion. Whereas previous expressions for the temporal
moments were developed for the case of an instanta-
neous slug release, the new expressions allow for the
specification of any concentration-versus-time distribu-
tion at the upstream boundary. Given the upstream
boundary values, the temporal moments may be routed
downstream for comparison with field data or as a check
on the accuracy of numerical models.Sheibley et al. [29] modeled nitrogen transforma-
tions in sediment perfusion cores from the Shingobee
River in Minnesota over an annual cycle. Their results
indicate that ammonium concentrations in the river
were controlled by nitrification of ammonium from
groundwater in hyporheic sediments, and that the rate
of this process was strongly temperature dependent.
This study shows that hyporheic zone biogeochemi-cal processes can change in potentially predictable
ways due to seasonal shifts in temperature, as well as
hydrology.
Supriyasilp et al. [31] developed a statistical technique
for the calibration of water quality models. The tech-
nique, known as quantitatively directed exploration
(QDE), uses the variance of model input parameters to
identify the parameters and sampling locations thatproduce the most uncertainty in model results. QDE was
applied to a hypothetical problem using a model that
considers advection, chemical reaction, settling, and
hyporheic exchange. Statistical results were used to de-
termine which parameters result in the largest variance
in predicted concentration; these parameters were
identified as the focus of additional data collection ef-
forts.Thomas et al. [33] developed the regression parti-
tioning method (RPM), a method for estimating the
904 Preface / Advances in Water Resources 26 (2003) 901–905
portion of solute uptake occurring within the transient
storage zone. Under RPM, whole stream uptake is de-
termined from the spatial pattern of plateau tracer
concentrations and main channel uptake is determined
using data from the rising limb of the tracer profile.Storage zone uptake is then determined by difference.
The method was demonstrated using data from two
tracer additions, where 44–48% of the nitrate uptake
occurred within the storage zone.
Acknowledgements
Work on this special issue was initiated after con-
versations with Marc Parlange, former co-editor of
Advances in Water Resources. The lead editor was sup-
ported in part by funding from the US Geological
Survey�s Toxic Substance Hydrology Program. Helpful
reviews of this preface were provided by Marisa Cox
and Jim Tesoriero.
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Robert L. Runkel
United States Geological Survey
Denver, CO, USA
Tel.: +1-303-236-4882; fax: +1-303-236-4912
E-mail address: [email protected]
Diane M. McKnight
Institute of Arctic and Alpine Research
University of Colorado
Boulder, CO, USA
Harihar Rajaram
Department of Civil, Environmental, and
Architectural Engineering
University of Colorado, Boulder, CO, USA