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Natural Flood Storage and Extreme Flood
Events Final Report
3 Modelling and gis analysis
3.1 Natural storage and attenuation
The objective of this study was to assess the scope for
using 'natural' flood storage within a river system. The
focus on 'natural' storage means that we have investigated
only areas that would flood naturally (according to model
predictions). There is generally greater resistance to flow
over the floodplain than in the river channel. Floodplains
also provide 'storage' in the form of volumes of water that
become disconnected from the main channel flow. The net
effect is to attenuate the peak of a flood hydrograph, or
'event', as it passes downstream.
This project aims to quantify the amount (volume or
extent) of water that would have to be held back to
mitigate against downstream flooding given a specified
hydrological event. For example, consider a town where
flooding occurs for flows greater than the 100 year flow.
If the target is to limit a 200 year event to a 100 year
peak flow, then we are interested in the difference between
the 100 year and 200 year events.
A conventional way to tackle this problem is to model
hydrographs for the two events and to calculate the
difference in the volume of water between the larger event
and the peak of the smaller event. Graphically, this can be
described as 'slicing the top off the larger hydrograph'
(see Figure 3-1). Typically, a feasibility study would then
involve a search of the upstream floodplain to find areas
that may be suitable for impounding water. Embankments can
be placed across the river valley in a GIS analysis, and
the volume and area of the impoundments calculated from a
DEM. This type of analysis would indicate how much storage
volume could be found at those locations, which can be
compared with the hydrograph analysis. As a final step, the
most promising impoundments could be added to a routing
model as reservoirs or ponds, allowing their effectiveness
to be tested.
Figure 3-1: Simple
hydrograph volume analysis

Because we are looking at potential 'natural' storage,
we have not used this approach (although it would be needed
as a follow-up to the type of analysis described here for
more detailed scheme design).
3.2 Flood events
We can assign a probability or return period to the flow
that causes flooding at a downstream risk location.
However, the 'event' that causes this flood cannot be
assigned a return period without some ambiguity. This is
because there are many possible combinations of rainfall
events and antecedent conditions that could generate the
same downstream outcome. These different conditions could
also involve different durations, storm tracks or multiple
peaks that could cause different responses on the
floodplain.
Whilst the definition of a T-year flow is reasonably
clear, the concept of the 'T-year' event, as it is commonly
understood in engineering hydrology in the UK, is based on
a relationship between the probabilities of rainfall and
peak flood flows derived under strong assumptions about the
shape and uniformity of the rainfall profile, antecedent
conditions and losses during an event.
There are three approaches that can be used to generate
a suitable flood event for analysis of storage or
attenuation. The first is continuous simulation of
synthetic flow sequences. This is the preferred approach
scientifically because it can account for the multiple
rainfall and soil moisture histories that can combine to
produce a given flood flow. However, it is not yet a
standard method in engineering practice and was beyond the
scope of this project. The second approach is the
event-based 'rainfall-runoff' model described in the Flood
Estimation Handbook (FEH, Institute of Hydrology, 1999),
which is the standard approach in UK practice. Both
continuous simulation and event approaches can be applied
as boundary conditions to a model of the river flow.
A third approach is a purely hydrological one in which
statistical estimates of peak flows are made a regular
intervals along the river network and a standardised
hydrograph shape applied to simulate an 'event'. This
approach has been adopted for national-scale flood outline
modelling in England and Wales because it is relatively
generalised and can therefore be applied without needing
local data. It does not guarantee hydrologically consistent
changes in hydrograph shape or magnitude in a downstream
direction (although significant work has been done to
enhance the spatial consistency of the statistical
estimates, as reported by Morris, 2003).
We have used the event-based approach because it remains
the approach most likely to be used in existing models. For
the sake of simplicity we have assumed that the
flood-producing event is in effect a uniform rainstorm, but
that the return period of the flow at the downstream
location defines the return period of the 'event'. We can
note that this is a simplification and that in nature the
return period of the flow generated by this 'event' would
vary with location in the catchment.
3.3 Event modelling
We have used two approaches to simulate flood events in
this study, namely one-dimensional and two-dimensional
models.
3.3.1 One-dimensional models
The simpler approach is one-dimensional (1-D) flow
routing, in which event hydrograph inputs, generated using
FEH methods, are applied as upstream or lateral boundary
conditions on a 1-D model of the river. The routing model
then represents the movement of the hydrograph downstream
as a flood wave. (The flood is referred to as a 'wave'
since its movement downstream is a wave motion; the wave is
a disturbance in the flow, representing the passage of the
flood peak.)
There are many routing models. The most commonly used
are:
- Muskingum or Muskingum-Cunge
- Kinematic wave
- Hydrodynamic modelling (e.g. HEC-RAS, ISIS)
The Muskingum model is often known as hydrological
routing, in which flow down the river can be thought of as
a series of conceptual stores. The resulting computer model
requires only a few conceptual parameters (related to the
speed of the flood wave and the degree of attenuation). The
kinematic wave and hydrodynamic models can be thought of as
hydraulic models that include differing degrees of process
detail (see below). The Muskingum-Cunge is a useful routing
model that can be shown theoretically to be essentially the
same as some forms of hydraulic model.
River flow can be described by unsteady, 1-D,
differential equations (known as the St. Venant equations)
that can be solved numerically if the river cross section
is known. These can be expressed as

where the first equation is the continuity equation and
the second the momentum equation, Q is the cross-sectional
average flow rate, A is the wetted area of the cross
section, y the depth, x the distance down river, S0 the
slope of the river bed, and Sf the friction slope. The last
term is a measure of the friction force acting on the flow
and is expressed as a slope for convenience. The equation
assumes that the baseflow or tributary inflows are equal to
q.
The kinematic wave solution is a simplified solution of
these equations that assumes the gravitational force is
exactly balanced by the friction as it neglects the first
three terms - the local acceleration, convective
acceleration and the pressure (i.e. the second equation
reduces to S0= Sf).
In the diffusion wave model, the pressure term is added
to this, meaning that flow can be driven by the water
surface slope as well as the bed slope and friction. The
dynamic wave model includes all terms. The Muskingum-Cunge
method is a solution of a type of diffusion wave equation
based on the Muskingum equation. These methods are covered
in detail in most river hydraulics text books.
The advantage of using the simpler approaches is that
they require less data than a more complex model. In this
study, we are aiming to incorporate existing models where
available, but cannot assume that detailed data such as
river channel and structure surveys are available.
There are three ways in which an existing (or new) 1-D
model can be used to assist with the 2-D modelling of the
floodplain, as follows
- routing of the flood hydrograph through the river
network
- calculation of channel capacity
- conversion of flow to level at the downstream risk
location
Routing the flood hydrograph - event
definition
A model capable of routing a flood hydrograph (but not
necessarily of calculating water levels) is a useful
starting point to establish the hydrological event inputs
that lead to a prescribed probability of exceeding a given
flood flow at the downstream risk location. The steps to be
taken are linking flood estimates at key locations
(headwaters, lateral inflows, tributaries) and establishing
a combination of rainfall intensity, profile and duration
that generates a flow of given probability downstream.
Channel capacity
If a model is available that includes river survey data,
then this can also be used to estimate the capacity of the
channel at each cross section, and hence the rate of flow
that should be allowed onto the floodplain. This
calculation may be straightforward where there are
well-defined bank elevations, or more uncertain if only
coarse cross section data exist. An alternative approach is
to use LiDAR to set up a river valley cross section, with
an assumed standard channel shape. This will not provide as
good an estimate of channel capacity as surveyed cross
sections, although it may be helpful, especially if banks
can be seen clearly in the LiDAR grid.
Establishing flood levels at the downstream
location
A hydraulic model covering the downstream risk location
will always be useful to provide a rating curve so that the
threshold level for flooding can be expressed accurately in
terms of flow rate, and hence as an exceedance
probability.
3.3.2 2-D floodplain modelling
The second approach used to model flood flows is a 2-D
cellular inundation model, JFLOW, which was developed by
JBA Consulting as a flood extent modelling tool. It has
been tested and validated for large scale automated flood
mapping (JBA Consulting, 2003) and also applied
successfully at a much more detailed scale in flood mapping
studies, to model breaches in defences and also for coastal
inundation modelling. It is based on an approach developed
by Bates and De Roo (2000).
JFLOW represents the movement of water over the
floodplain as a discretised diffusion wave, which means
that (a) flow is driven locally by the difference between
the water surface slope and frictional resistance over the
ground and (b) the calculations are carried out over fixed
grid cells on an element-by-element basis. The approach is
often referred to as 'raster' modelling because it is
designed to take advantage of raster (i.e. gridded) DEM
data.
One of the main motivations for this type of modelling
approach is the observation that, in many situations,
topography is the key control on the routing of floodplain
flow, with frictional resistance being the next most
important factor. Both of these controls are represented in
the 2-D model used here. Other processes, such as momentum
exchanges between floodplain and channel flows, are not
explicitly included in the modelling, which means that the
roughness parameter Manning's
n may have to take a value that compensates for
neglecting these energy transfer mechanisms, but which also
tends to improve efficiency and numerical stability. A
value of
n = 0.1 was used in this study. The generic
approach has been shown to be effective both in modelling
the maximum extent of flooding and also the passage of a
flood hydrograph when combined with a diffusive wave
channel model (Horritt and Bates, 2001, 2002).
Another reason for using JFLOW (or another raster-based
model of this type) is that good quality DEM data suitable
for floodplain modelling are now available for the whole of
Scotland. JFLOW was designed to model the flow of water
over the floodplain, and does not currently include a model
for flow within the river channel itself, which is regarded
as the volume contained within the river banks. This was in
part motivated by the needs of large-scale automated flood
extent mapping, where the detailed river channel survey
data needed to set up a conventional 1-D hydraulic model
would be too expensive and time-consuming to collect.
3.4 Model development
For each study catchment, the first step was to estimate
peak flow magnitudes for flooding downstream using FEH
methods. Only the fluvial flood probabilities were
considered, but it is noted that Perth in fact floods from
a combination of fluvial and tidal sources.
The main objective of the study was to assess the
potential to reduce the downstream effects of a 100 or 200
year event. We have therefore taken the 200 year event as
our starting point to define available 'natural' storage
areas in each study catchment.
For the White Cart catchment, the existing White Cart
Millennium study investigated options to reduce a 200 year
flood event so that the downstream flow was limited to the
current 5 year flow. We have therefore adopted the 5 year
flood flow as the 'threshold' flow. In addition, we have
modelled the 100 year flow to compare against the 200 year
event, as this is one of the project objectives.
For the South Esk, the recent Brechin flood study
considered storage options to reduce a 200 year event to
the current 100 year downstream flow. We have therefore
modelled these two events only. For the Tay, there is no
obvious equivalent 'threshold' downstream flow. However,
past flooding on the Tay has caused agricultural damages.
There are some embankments in the lower Tay that are
thought to offer around a 5 year standard of protection. We
have adopted this value as a target downstream peak flow in
at Ballathie gauging station, in addition to the 100 year
event.
A routing model was set up for each of the study
catchments. This was calibrated such that the modelled peak
flows agreed (at least to a close approximation) with the
FEH flood peak estimates or the corresponding return
period.
The downstream hydrographs for the larger events were
then compared with the peak flow for the 'threshold' event,
and the volume that would have to be stored was calculated
using the simple approach illustrated in Figure 3-1. For
the Clyde, a volume frequency analysis was used instead, as
described in Section 8). These figures can be considered as
minimum required volumes of flood storage (strictly
speaking assumed to exist immediately upstream of the risk
location).
As noted in Section 1, this study is concerned with
'natural' flood attenuation, which is interpreted to refer
to areas contributing to flood attenuation that appear
under existing conditions for a larger event. We would
therefore consider the difference between, for example, the
extents of the current 200 year and 100 year floods to
represent potential 'natural' storage that could be used to
mitigate the 100 year flood and restrict downstream flows
to those of the current 5 year return period flood.
The starting point for the analysis was therefore to
simulate the extents of flooding for each of the flood.
This was done using JFLOW as a flood extent modelling tool
for flows greater than bankfull. Inflows were taken from
the 1-D routing models. For the White Cart, where existing
model data were available, we estimated the bankfull flow
using the channel cross sections. For the other catchments,
we approximated bankfull flow as QMED, estimated using FEH
methods. For the experimental work in this study, we have
aggregated the DEM up to a 50m scale to improve model run
times over the large areas to be modelled. Initial results
suggested that this coarser grid did not introduce
significant inaccuracies at the catchment scale.
The resulting flood outlines were saved as tables in
MapInfo GIS format and can be plotted in map form. However,
at the catchment scale the differences in extents are not
always visually large. It is therefore useful to summarise
the results by computing and plotting the area of
inundation as a function of distance upstream from the risk
location. We have then calculated the differences between
the areas of the larger and smaller events to represent the
'natural' area in which water could be held back to
mitigate the larger event. The graphs show the cumulative
areas available for 'natural' storage as a function of
distance upstream from the 'risk location'. The areas are
marginal areas between the 200 year and 100 year events,
where available (that is, they represent potential
'additional' natural storage during an event of return
period ²1 in 100 years). Steep sections of the graphs
indicate locations along the river where there are large
differences between the inundation extents for the two
return periods. These locations may therefore offer the
greatest potential to hold water back during the larger
event within the 'natural' flood extent.
3.5 Scope for utilising the natural
floodplain
To fully realise the 'natural' flood attenuation in
practice would of course require interventions to impound
water in order to store the difference in volume identified
from the hydrograph analysis.
To permit a general, catchment-scale analysis, it has
been necessary to adopt only very simple methods for
analysing the potential to store the required volume within
the river system. We have made the simplest possible
assumption that the volume required at the downstream
location can be divided by the modelled flooded area to
give a notional average storage depth. In each case study,
we have calculated the required average storage depth using
both the total extent of the 200 year flood, and also the
marginal extent between the 100 year and 200 year
outlines.
The figures give an indication of the average depth to
which water would have to be stored to utilise the natural
floodplain for the events specified above. Based on these
figures and the distribution of floodplain extent
(expressed with respect to distance upstream), we have
calculated the average depth of water that would be
required on the floodplain to achieve the required volume
of storage.
The required depth is of course large close to the
downstream limit since only a small area is available for
storage immediately upstream of the limit. As the available
area increases with distance upstream, so the required
average depth falls. The depth curves have been truncated
at 15.0m, which is taken as a pragmatic maximum storage
depth.
The depth-distance curves can be used as a broad guide
to the feasibility of using the natural flood extent to
provide the storage needed to reduce a 100 year event to
the 5 year flow downstream. In general, storage is most
effective if it is located immediately upstream of the
flood risk location. If the average storage depth falls to
a practically-attainable value within a few kilometres of
the downstream location, then there may be scope to use
land in the natural 200 year extent to provide the required
storage.
It is clear that these average depths depend critically
on the area assumed to be available as 'natural
floodplain'. In this case, we have used simulations of a
200 year flood extent. It would be useful to repeat the
analysis using a much larger extent from a more extreme
event, say for a 1000-year flood.
A second issue is that the concept of an average depth
ignores the role of topography in determining where storage
might be best located. This is much more difficult to
address because it requires the assumption of a water
surface, which would depend on the exact location(s) and
height(s) of one or more flood banks. Options for building
flood banks require location-specific investigations, and
cannot be assessed using the type of generalised analysis
presented here.
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