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Estimation of preferred water flow
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African Journal of Aquatic Science 2006, 31(2): 261–269
Printed in South Africa — All rights reserved
AFRICAN JOURNAL OF
AQUATIC SCIENCE
EISSN 1727–9364
Estimation of preferred water flow parameters for four species of Simulium
(Diptera: Simuliidae) in small clear streams in South Africa
Nicholas A Rivers-Moore1*, Ferdinand C de Moor2, Sharon A Birkholz1 and Robert W Palmer3
1
Institute for Water Research, Rhodes University, PO Box 94, Grahamstown 6140, South Africa; current address: KZN
Wildlife, PO Box 13053, Cascades 3202, South Africa
2 Albany Museum (Department of Freshwater Invertebrates, Makana Biodiversity Centre) and Rhodes University, PO Box 94,
Grahamstown 6140, South Africa
3 Nepid Consultants, PO Box 4349, White River 1240, South Africa
* Corresponding author, e-mail: riversmn@kznwildlife.com
Received 19 April 2006, accepted 14 July 2006
Blackfly larvae typically occur in fast-flowing riffle sections of rivers, with different blackfly species showing preferences for
different hydraulic conditions. Very little quantitative data exist on hydraulic conditions linked to the blackfly species occurring in
South African streams. Stones-in-current biotopes (i.e. fast riffle flows over cobbles) were sampled from four sites in three small
clear streams in the Eastern and Western Cape provinces of South Africa. Mean water column velocities at each sampled stone
were measured using a mini current meter, while flow velocities closer to the boundary layer where blackfly larvae occurred were
estimated using indirect techniques (standard hemispheres and aerating tablets). Standard hemispheres were also used to calculate more complex hydraulic parameters such as Froude and Reynolds numbers. Four species of Simuliid were sampled in sufficient numbers to show trends in flow velocity preferences. Simulium impukane and S. rutherfoordi both occurred at their highest
densities at velocities of 0.3m s–1, while S. merops preferred velocities of 0.7m s–1. Simulium nigritarse SL attained the highest
densities of all the blackfly species sampled, and its relative abundances were greatest at velocities of 0.8–0.9m s–1. Within the
streams surveyed, all blackfly species occurred in subcritical-turbulent flows — based on a classification using Froude and
Reynolds numbers — although two of the species were also found in high densities in supercritical flows where these existed at
the sites. Local hydraulics within the stones-in-current biotope are complex, but in the absence of fine-scale equipment for measuring micro-velocities, standard hemispheres are a useful, cost-effective technique for the initial quantification of hydraulic parameters in small, clear streams. Such an approach facilitates further understanding of links between hydraulics and aquatic invertebrates in South African streams.
Keywords: aerating tablets, blackfly, flow velocity, Froude number, hydraulics, Reynolds number, standard hemispheres
Introduction
Hydraulic properties of stream flow are valuable descriptors
of the physical environmental template of lotic organisms
(Statzner and Higler 1986), whose zonation patterns typically
relate to downstream changes in hydraulic properties
(Statzner and Higler 1986, Statzner et al. 1988, Statzner and
Borchardt 1994). In general, abiotic processes are considered one of the major determinants of river communities
(Hildrew and Giller 1994). The stone/water column interface
is of particular importance to aquatic invertebrates, as it is a
gradient region where flow velocity changes from zero at the
stone surface to that experienced in the water column (Vogel
1981). Within this gradient region, or boundary layer, various
factors including drag, the extent of laminar versus turbulent
flow, and viscosity, affect aquatic invertebrates by affecting,
inter alia, access to food and mobility (Gordon et al. 1992).
Boundary layer thickness has considerable implications for
filter-feeding aquatic macroinvertebrates, such as blackfly
larvae (Diptera: Simuliidae), which depend on the accessibility of micro-particles of food in this layer.
Blackflies are ubiquitous and occur in most riverine systems
worldwide (Snaddon and Davies 2000), their larvae usually
being found on hard substrata in fast flowing conditions (de
Moor 1982). Carlsson (1967) found that the distribution of
blackfly larvae depended largely on flow velocity, although
depth, type of substratum, light and water temperature also
contributed to habitat preference. For example, de Moor
(1982) illustrated the link between blackfly densities,
discharge, mean water column velocity and colonisable
area in the Vaal River. His study showed that an increase in
discharge provides more habitat, higher velocities, and
better dispersion capacity, while falling water levels and
unpredictable flows reduce suitable habitat. He also
showed that the abundance of S. chutteri increased with
increasing flow velocities (0.18–1.32m s–1), with 0.56m s–1
considered as a suitable lower threshold for colonisation. A
small tributary of the Vaal River with slower velocities
(0.3–0.4m s –1 ) had a lower prevalence of S. chutteri.
Conversely, S. adersi showed a preference for flow velocities
262
of 0.3–0.6m s–1 (de Moor 1982). Similarly, Palmer (1997)
observed that low flows in the Orange River (<21m3 s–1)
were ideal for S. adersi, S. damnosum and S. mcmahoni,
flows of around 200 m3 s–1 were suboptimal for S. chutteri,
while discharges in excess of 300 m3 s–1 were ideal for
forming large populations of S. chutteri. These discharges
relate directly to flow velocities and stream depths, where
the greater the discharge the higher the flow velocity and
the greater the amount of available habitat for S. chutteri.
Palmer and Craig (2000) showed that a relationship existed
between labral fan structures of different species of blackfly
larvae and habitat parameters (flow velocity). This relationship was useful in predicting distribution patterns of different
species of blackfly larvae relative to flow velocities.
For ecological purposes, flow velocities near the bottom
of a channel, or at the water surface, are of greater significance than averages across a river channel cross-section
or over a reach. Variations of flow velocity with time may
also be critical to aquatic insects (Gordon et al. 1992) and,
at smaller scales, velocity governs the hydraulic conditions
that mediate biotic interactions (Hilldrew and Giller 1994).
Additional hydraulic parameters of interest to understanding
distribution patterns of aquatic freshwater invertebrates are
the dimensionless Reynolds (Re) and Froude numbers. Re
numbers, central to biological fluid mechanics (Vogel 1981),
describe the ratio of inertial to viscous forces and assist in
characterising the microhabitat of lotic organisms. Large Re
numbers indicate turbulent conditions, while small Re
numbers indicate laminar flows (Gordon et al. 1992). The
Froude number is the ratio of inertial to gravitational forces
and is useful in describing ‘bulk flow characteristics such as
surface waves’ (Gordon et al. 1992: 276). For example,
under conditions of high turbulence (i.e. higher Re
numbers), Simulium chutteri feeds more efficiently than S.
nigritarse SL (Barber-James 2004), due to differences in
their labral fan structures and in how efficiently food particles are intercepted under different flow conditions (Palmer
and Craig 2000).
Estimating flow velocity at the surface of an in-stream
stone, as well as associated hydraulic, parameters —
including viscosity and laminar versus turbulent flows — are
critical to understanding the abiotic templates that structure
the zonation patterns of simuliids. One challenge is to use
appropriate sampling techniques to collect invertebrate data
and relate these to hydraulic parameters. The aims of this
study were to evaluate the use of standard hemispheres for
characterising the hydraulic habitat of Simulium spp. occurring in small clear streams, and to estimate the preferred
flow velocities of these species.
Study area
Data were collected from two small clear streams in the
Eastern Cape province, and one stream in the Western
Cape province, South Africa. Two of the Eastern Cape sites
were on the Bloukrans River, a tributary of the Kowie River,
in the Belmont Valley 6.5km east of Grahamstown. Site 1
(BV1) (33°19’25.2”S; 26°36’00.8” E; 480m amsl) was downstream of a small bridge, while Site 2 (BV2) (33°19’21.4”S;
26°36’49.7” E; 470m amsl) was 1.5km further downstream.
Rivers-Moore, de Moor, Birkholz and Palmer
These sites were chosen because the downstream site
represented a less polluted replicate of the upstream site.
The third site in the Eastern Cape, Site 3, was located on the
Palmiet River, a tributary of the Kariega River, at Howison’s
Poort (33°22’05”S; 26°28’30”E; 400m amsl) 8km west of
Grahamstown. Site 4 (33°58’30.6”S; 23°31’17.9”E; 20m
amsl), in the Western Cape province, was located on the
Salt River in the De Vasselot Nature Reserve.
Methods
Collection of invertebrates and hydraulic data
Aquatic invertebrate communities were sampled between 2
and 12 August 2005, from 6–10 stones at each site from
the stones-in-current biotope (i.e. fast riffle flows over
cobbles). Stones that could be lifted with one hand were
removed from riffle habitat, and their positions marked
using polystyrene floats attached to lead sinkers. Each
stone was visually assessed (after lifting) to determine
where the highest concentration of simuliid larvae was to be
found, relative to flow velocity. These densities were rated
according to Palmer’s (1994) 10-point semi-logarithmic
scoring system, where a score of 1 represents no blackfly
larvae on a stone, and a score of 10 represents in excess of
500 000 larvae m–2. The lifted stones were held over a 250
µm mesh hand net, before being scrubbed over a bucket
(Chutter 1968, de Moor 1982). Bucket contents were sieved
through a 250 µm mesh hand net into collecting jars
containing 70% ethanol. Aquatic invertebrates were identified to family and, where possible, to species level before
being counted.
Discharges (m3 s–1) at each site were calculated using
standard hydrological techniques, as detailed below
(Gordon et al. 1999). Discharges at Sites 3 and 4 were
calculated using a Scientific Instruments (1980) mini current
meter. In this method, the number of revolutions of the
current meter at 0.4 of the water depth (measured from the
river bed) were counted over one minute, at 0.25m intervals
of the stream width at a site where the channel was
constrained to account for all the flow. These counts were
converted to velocities using calibration curves (Scientific
Instruments 1980), and discharge was calculated using flow
velocities and channel surface areas. Discharges at Sites 1
and 2, which were downstream of a bridge where all the
flow flowed through eight pipes, were estimated using
Equations 1a–c, which is an appropriate discharge estimation in partially-filled pipes:
Q = vA
(1a)
A = 0.5r 2 (θ − Sinθ )
(1b)
⎛r−d ⎞
θ = 2 cos −1 ⎜
⎟
⎝ r ⎠
(1c)
where Q is discharge (m3 s–1), v is average flow velocity (m
s–1), A is cross-sectional area of pipe (m2), θ is in radians, d
is depth of water in pipe (m), and r is radius of pipe (m).
The following water quality parameters were also
African Journal of Aquatic Science 2006, 31(2): 261–269
recorded: total dissolved salts (TDS) (WTW LF95 conductivity/TDS meter), pH (Cyberscan 20 pH meter, or Lovibond
Comparator), conductivity (WTW LF95 conductivity/TDS
meter) and water temperature (glass alcohol thermometer).
Turbidity was not measured, since all streams had clear water.
Mean water column velocities at each selected stone
were determined, using the mini current meter, by recording
the number of revolutions recorded by the current meter
over one minute and converting these to flow velocities.
Flow velocities, as close to the stone surface as possible,
were also measured using two indirect methods. In the first,
standard hemispheres were placed on a levelled plexiglass
plane at each site which had previously been marked with a
float showing where a stone had been removed. In this
approach, the maximum density of the last hemisphere to
move within the current was used to calculate velocity,
using the relationship between density and flow velocity
defined by Statzner and Müller (1989). Additional hydraulic
parameters considered to be of greatest significance to the
larval simuliids in this study, namely Froude and Reynolds
numbers, were calculated using standard hemispheres and
associated relationships (Statzner and Müller 1989). In the
second method, after the scrubbed stones had been
replaced, flow velocities close to the stone surface were
estimated, based on mass loss of Livoxine ® aerating
tablets, using an approach described by Madsen and
Warncke (1983). A calibration curve was established
between the mass loss of aerating tablets over a fixed time
period (5min) and flow velocity measured using a mini
current meter. Aerating tablets were held in place between
two dowels (Ø = 3mm X 300mm long), attached at 90° to a
wooden pole (Ø = 20mm X 1m) which was able to slide up
or down a second pole. Using this system, the aerating
tablets could be positioned in-stream at any chosen locality
and depth, thus allowing the estimation of mean water
column velocities, or velocities at the surface of in-stream
stones. Flow patterns were also visualised using dye (red
food colourant mixed with milk) (Clayton and Massey 1967,
Vogel 1981), which provided an indirect measure of how
flow velocities changed as water passed around the stones.
This mixture provides a rough visual estimate of flow
patterns, since the dye remains as a dark stain around the
instream object for varying amounts of time, depending on
flow velocity — less than 1sec for fast (1m s–1) flows, and
more than 5sec for slow flows (<1m s–1), particularly around
rocks covered with filamentous algae.
Substratum size classes and substratum roughness were
also calculated, using the methods of Statzner et al. (1988).
In this method, stone sizes were visually assessed by size
class, and ranked from most dominant to third most dominant size class, in order to estimate a weighted contribution
to substratum roughness.
Data analyses
Larval densities (number of larvae m–2 of stone) were calculated by using an averaged value of 42% colonisable area
on stones. Colonisable area was defined as the amount of
stone surface exposed to flows, and excluded surfaces
embedded in the river bed or colonised by algae. The
proportion of colonisable area on stones-in-current biotope
263
was estimated from a pooled subsample of stones removed
from high-velocity biotopes from each of the four sites.
Areas on stones actually colonised by larvae were marked
with a permanent marker. Each rock was wrapped in
aluminium foil in such a way as to avoid foil overlaps, and
from this pieces were cut out to approximate the colonised
areas. The percentage of colonisable surface area actually
used by simuliid larvae was estimated using a linear relationship between foil mass and surface area. Mean (± standard deviation) larval densities, as well as their coefficients
of variation (%), provided estimates of the uniformity of
distribution within the stones-in-current biotopes for the
Simulium species collected.
Owing to the non-normal distribution of blackfly larvae, relative abundances of blackfly larvae were log(x + 1) transformed prior to further analyses in testing for correlations
against flow velocity data. Evaluation of the different techniques to measure flow velocities was achieved through
correlations using simple linear regressions. Estimated microhabitat velocities (i.e. velocities calculated using the standard
hemispheres and the aerating tablets) were regressed against
measured average water column velocities to determine the
relationship between mean flow velocities in the water column
and velocities closer to the boundary layer. Also, flow velocity
estimates using standard hemispheres were regressed
against those estimated using the aerating tablets, to determine how similarly each of these techniques estimated velocities close to the boundary layer. In considering the hydraulic
habitat of blackfly larvae, flow velocities estimated using the
standard hemispheres were used in the graphs of blackfly
larval abundances. This allowed for the calculation of
Reynolds and Froude numbers associated with larval abundances based on a single measurement using the standard
hemispheres. The preferred flows of individual simuliid
species were classified according to Davis and Barmuta
(1989), by relating maximum relative abundances to corresponding Reynolds numbers and Froude numbers.
Results
All river sites were less than 6m wide and 0.42m deep, with
similar slopes (0.03‰), substratum roughness (2.78), and
water temperatures (Table 1). Of the three river sites
sampled, the Palmiet was the most acidic and oligotrophic
system (Table 1). Both sites on the Bloukrans River were
typical of highly eutrophic systems, with visible evidence of
algal filamentous blooms (Kleynhans et al. 2005).
Aquatic invertebrate communities in the Salt and Palmiet
Rivers showed the greatest species diversity (Table 2). The
Bloukrans River sites had few species present in relatively
high abundances, and only one species of blackfly (S. nigritarse SL) which had relatively high abundances of both
larvae and pupae (Table 2). The Palmiet River had the highest number of blackfly species, supporting three species
typical of small streams, but all were present in low
numbers, with only one species (S. medusaeformae) being
found at more than one site.
Coefficients of variation of larval densities of blackfly
varied from 40% (S. merops) to 270% for S. impukane
(Table 3). The distribution of larval S. nigritarse SL showed
264
Rivers-Moore, de Moor, Birkholz and Palmer
Table 1: Spot values for physical and water quality variables at four sites in three river systems in the Eastern and Western Cape provinces
in August 2005, and the number of stones sampled per site
Parameters\Rivers
Bloukrans
(Site BV1)
Water temperature (°C)
TDS (mg l–1)
Conductivity (µS cm–1)
pH
Discharge (m3 s–1)
Width (m)
Substratum particle size (m)
No. of stones sampled
10.5
874
1 020
7.6
0.073
3.5
0.15
6
Bloukrans
(Site BV2)
Salt
Palmiet
11.0
1 220
1 420
7.6
0.103
3.1
0.20
10
9.8
299
350
6.3
0.006
6.0
0.20
8
11.5
128
149
5.7
0.006
1.0
0.08
10
22
Orientation
20
FREQUENCY/DENSITY CLASS
18
Density class
Class 4 = 49 larvae 4mm2
Class 5 = 1022 larvae 4mm2
16
14
12
10
8
6
4
2
Top
Bottom
Front (upstream) Back (downstream)
ORIENTATION
Left
Right
Figure 1: Orientation of blackfly larvae on stone surfaces, and median class values of highest larval density (larvae m–2) on substratum
particles. Larval density classes are on a 1–10 scale after Palmer (1994). Black bars represent absolute frequency of orientation of blackfly
larvae on stones
uneven clumping on substrata at the two sites on the
Bloukrans River, which was probably caused by variations
in algal coverage on stones at these two sites; the site with
higher algal coverage showed more uniform distribution of
blackfly larvae.
Of the 32 stones sampled, 21 (65.6%) had their highest
densities of blackfly larvae on their upper surfaces, with the
next most common orientation (12.5%) being the ‘front’ of
the stone, facing into the current (Figure 1). In two
instances, where stones were shaped in such a way as to
have water flowing underneath them, the highest density of
larvae was underneath the stone. Median larval densities
corresponded to Palmer’s (1994) Class 4 (3 750 larvae
m –2). In all observations, the blackfly larvae orientated
themselves in a uniform fashion, attaching themselves to
the stones with their longitudinal axes (from posterior proleg
to cephalic fans) in an upstream/downstream orientation
along water-flow streamlines, as illustrated in Figure 2.
The relationship between percentage mass loss of
oxygen tablets and flow velocity was significant (n = 13; r2 =
0.81; P < 0.05) (Figure 3). However, this relationship
became more variable at higher velocities.
Correlations between average water column velocities
measured using a mini current meter, and velocities close to
each sampled stone, measured indirectly using standard
hemispheres and aerating tablets, were weak but significant
(n = 32; r2 = 0.51 and 0.53 respectively; P < 0.05) (Figure 4).
Both indirect techniques generally overestimated flow velocities, with the standard hemispheres yielding higher flow
velocity estimates than did the aerating tablets. Velocities
estimated using aerating tablets were closer to the measured average water column velocities than were those esti-
African Journal of Aquatic Science 2006, 31(2): 261–269
265
Table 2: Species collected at four sites, and class values for relative abundances. Average number of individuals per stone is shown by
class (X = 1; XX = 2–10; XXX = 11–100; XXXX = >100). (L) = larva; (P) = pupa; (A) = adults; * = all larvae or nymphs
Taxa
Higher Taxa
Family/species
Ephemeroptera*
Baetidae
Baetis harrisoni (Barnard)
Afroptilum sudafricanum (Lestage)
Pseudocloeon vinosum (Barnard)
Demoreptus capensis (Barnard)
Small nymphs
Leptophlebiidae
Castanophlebia calida (Barnard)
Adenophlebia peringueyella (Lestage)
Caenidae gen. sp. indet
Teloganodidae
Lestagella penicillata (Barnard)
Simuliidae
Simulium impukane (de Meillon) (L)
S .impukane (P)
S. merops (de Meillon) (L)
S. merops (P)
S. nigritarse (Coquillett) (L)
S. nigritarse (P)
S. medusaeforme Pomeroy (L)
S. medusaeforme (P)
S. rutherfoordi (de Meillon) (L)
S. rutherfoordi (P)
Chironomidae gen. sp. indet. (L)
Athericidae gen. sp. indet. (L)
Hydropsychidae
Cheumatopsyche afra (Mosely)
C. maculata (Mosely)
Philopotamidae
Dolophilodes sp.
Leptoceridae
Oecetis sp.
Aeshnidae gen. sp. indet.
Elmidae gen. sp. indet. (L)
Elmidae gen. sp. indet. (A)
Helodidae gen. sp. indet. (L)
Notonemouridae gen. sp. indet.
Corydalidae gen. sp. indet. (L)
Oligochaeta gen. sp. indet.
Planaria sp.
Ancylidae
Burnupia sp.
Physidae gen. sp. indet.
Planorbidae gen. sp. indet.
Fam. gen. sp. indet.
Hydrachnellae Fam. gen. sp. indet.
Diptera
Trichoptera*
Odonata*
Coleoptera
Plecoptera*
Megaloptera*
Annelida
Turbellaria
Mollusca
Collembola
Hydracarina
mated using the standard hemispheres. Correlations between
flow velocities estimated using standard hemispheres and
aerating tables were also poor, but significant (n = 32; r2 =
0.28; P < 0.05) (Figure 5). In addition, correlations between
water depths where each stone was sampled, and those
estimated using standard hemispheres at the same point,
were not significant (n = 34; r2 = 0.0003; P > 0.05).
Of the five species of Simulium sampled, S. medusaeforme was excluded from analyses, since only three data
points were obtained for it. The densities of the four remaining
blackfly species peaked at different flow velocities (Figure
Rivers sampled
Bloukrans BV1
Bloukrans BV2
Salt
Palmiet
XXX
XXX
XXX
X
X
X
XX
X
X
X
XX
X
XX
XX
XX
X
XXX
XX
XXXX
XX
XXXX
XXX
XXX
X
X
XX
XXXX
XXX
X
XX
XX
X
X
XX
XX
X
XXX
XXX
X
X
X
X
XX
X
XX
X
X
X
X
X
X
X
X
X
XXX
X
XX
X
X
X
X
Table 3: Mean densities (m–2), standard deviations and coefficients
of variation (%) of five species of blackfly larvae at all sites
combined
Species
Mean
SD
CV (%)
S. merops
S. medusaeforme
S. impukane
S. rutherfoordi
S. nigritarse (BV1)
S. nigritarse (BV2)
904
398
1 858
349
2 574
5 310
361
866
5 022
391
1 238
6 417
40
218
270
112
48
121
266
Rivers-Moore, de Moor, Birkholz and Palmer
Figure 2: Blackfly (Simulium medusaeforme) larvae orientating according to the direction and strength of flow along the surface of a
rounded boulder in a small clear stream in the Eastern Cape (photograph by FC de Moor)
FLOW VELOCITY (m s1)
0.8
0.7
0.6
changed the local hydraulic conditions by slowing down flow
velocities and increasing the size of the boundary layer, thus
making the hydraulic habitat unsuitable for S. nigritarse,
possibly by excluding suspended particles from the water
column. All four species favoured hydraulic habitats with
Froude numbers of less than one, and Reynolds numbers of
less than 125 000 (Figure 7).
y = 0.012x 0.0706
R2 = 0.8129
0.5
0.4
0.3
Discussion
0.2
0.1
0
0
10
20
30
40
50
MASS LOSS OF TABLET (%)
60
70
Figure 3: Relationship between percentage mass loss of aerating
tablets and flow velocity
6). Simulium impukane and S. rutherfoordi favoured microhabitats with similar, low velocities (~
~ 0.3m s–1), while S.
merops showed preferences for faster flows (0.7m s–1). At
the Palmiet site, populations of S. impukane had colonised
leaves caught on top of stones-in-current. Simulium nigritarse SL favoured the highest velocities (0.8–0.9m s–1), and
also occurred at the highest larval densities. Based on dye
movement patterns, it was observed that thick algal mats
Characterisation of hydraulic habitat
While flow velocities may be the ‘fundamental abiotic factor
controlling ecological processes and patterns in streams’
(Hart and Finelli 1999: 375), the complexity of the hydraulic
environment at the boundary layer, particularly in rapids and
riffle biotopes, presents difficulties in their measurement
(Davis and Barmuta 1989). To overcome these challenges
may ultimately require instruments with fine spatial resolution to measure basic hydraulic parameters (Carling 1992,
Hoover and Ackerman 2004). This complexity, with associated gradients of velocities over small distances, may be
one reason why we found no significant correlations
between average water column velocities measured using
a mini current meter, and those estimated closer to the
boundary layer using indirect techniques. Similarly, Hart et
al. (1996) found no correlation between velocities meas-
1.2
AT
1 to 1
Linear (SH)
Linear (AT)
y = 1.2851x + 0.1471
r2= 0.5127
1.0
0.8
y = 0.6708x + 0.173
r2 = 0.5255
0.6
0.4
0.2
0.2
0.4
0.6
0.8
1.0
1.2
MEASURED FLOW VELOCITY (m s1)
S. nigritarse
1.5
1.0
0.5
0.2
1.4
Figure 6: Relative abundances of four Simulium species versus
flow velocities estimated using standard hemispheres
Reynolds
FROUDE NUMBER
FLOW VELOCITY (m s1)
:aerating tablets
0.4
0.6
0.8
1.0 1.2
FLOW VELOCITY (m s1)
Froude
150 000
2.5
1.2
100 000
2.0
1.0
A
1.5
0.8
50000
1.0
0.6
0.5
0.4
0.2
S. rutherfoordi
2.0
3.0
1.4
S. merops
2.5
1.4
Figure 4: Correlation between average water column velocity
measured using a mini current meter, and flow velocities calculated
using indirect techniques (aerating tablets (AT) and standard hemispheres (SH)). Dashed line represents 1:1 correlation
S. impukane
3.0
y = 0.2926x + 0.2384
r2 = 0.2786
0.2
0.4
0.6
0.8
1.0
1.2
1.4
FLOW VELOCITY (m s1): standard hemispheres
Figure 5: Correlation between flow velocity estimated using aerating tablets and that estimated using standard hemispheres
ured 2mm above a stone and those measured 10mm
above it. Where larvae are found without the need for
removal from their stones, the use of hot-wire anemometers
— which are small enough to measure flow velocities in a
0.25mm space — would be one approach to resolve these
uncertainties. However, such technology is not always
readily available or cheap (Davis and Barmuta 1989).
In the absence of such technology, Davis and Barmuta
(1989) proposed a classification of stream flows useful to
ecological studies, where complex hydraulic parameters are
calculated from relatively simple measures, including measurement of velocity profiles, depth, slope and substratum
roughness. This is a similar approach to that of Statzner et
al. (1989), who described a useful approach for calculating
hydraulic parameters, also based on simple hydrological
measurements. This approach was useful in categorising
hydraulic requirements of larvae of the pest blackfly, S.
chutteri, in the Great Fish River (Rivers-Moore et al. in
press), where velocity was the major hydraulic determinant
of larval blackfly distribution. The lack of instruments with
fine spatial resolution was therefore not a limiting factor in
describing the hydraulic environment of the blackfly larvae
sampled in the present study. The average depth of the
0.2
0.4 0.6 0.8 1.0 1.2
FLOW VELOCITY (m s1)
REYNOLDS NUMBER
CALCULATED FLOW
VELOCITY (m s1)
SH
1.4
267
Log (Relative Abundance + 1)
African Journal of Aquatic Science 2006, 31(2): 261–269
1.4
Figure 7: Relationship between flow velocity, and the biologically
significant hydraulic parameters Reynolds and Froude numbers,
estimated using standard hemispheres. Note that the threshold
Froude number separating subcritical-turbulent from supercriticalturbulent flows is indicated by point A, as defined by Davis and
Barmuta (1989)
sites in this study (<0.42m) made it difficult to measure flow
velocities within the water column but, nevertheless, the
small size of the streams provided an opportunity to use
and evaluate standard hemispheres and aerating tablets to
measure and describe the hydraulic habitat of blackfly
larvae in small, clear streams.
Cost-effective techniques, such as aerating tablets and dye,
offer limited usefulness in characterising local hydraulic conditions. The mass loss of aerating tablets at different flow velocities is a useful principle, although the method would need to
be refined — primarily through refining the apparatus which
holds the tablets. The 3mm Ø dowels which held the aerating
tablets could be replaced with thinner (<0.5mm) sprung steel
callipers to allow for placement of the tablets closer to the
stone surfaces. For visualising flow patterns around stones-incurrent biotopes, coloured dyes mixed with milk are of limited
value in stream systems with discharges in the order of
0.01m3 s–1 (10 l s–1). They become of increasingly less value
at velocities exceeding 0.26m s –1 and at discharges in
streams, such as the Bloukrans River, which have average
daily flows above 0.1m3 s–1 (100 l s–1). This is because the
268
dyes are dispersed so rapidly that it is difficult to visualise
streamlines and areas of laminar versus turbulent flow.
Standard hemispheres are useful as an initial technique
for quantifying local hydraulic conditions, which can then be
related to aquatic invertebrate distribution patterns, particularly in the absence of more expensive micro-velocity
meters. Such hemispheres are effective integrators of local
hydraulics around a point (Statzner and Müller 1989), and
provide a cost-effective approach for initial research in this
area for South African rivers. Standard hemispheres are a
simple technique for use in the field, even though their one
important disadvantage is that it was sometimes not possible to position a hemisphere in situ where blackfly larvae
had been collected. We assumed that a hemisphere would
approximate the hydraulic conditions of the stone for which
it was a ‘place-holder’, in spite of differences in height
between the stone and hemisphere translating into differences in local hydraulic conditions, as shown by the use of
coloured dye. However, it is also important that, since the
hydraulic parameters calculated from the densities of the
standard hemispheres are all highly correlated, multi-colinearity in multivariate ordinations would be an issue. One
simple measure (such as velocity) is therefore more pragmatic to use as a ‘place-holder’ in such analyses, and from
the statistical relationships between standard hemisphere
densities and key hydraulic characteristics (including
Reynolds and Froude numbers), which can be used to estimate the local hydraulic habitat of target aquatic invertebrates. The usefulness of standard hemispheres lies in
describing the hydraulic environment of those aquatic invertebrates of interest, since the hemispheres integrate sitespecific hydraulic effects through their design and in situ
placement.
Preliminary hydraulic preferences of blackfly larvae
sampled
Froude numbers of less than 1 characterise subcritical flow,
whereas supercritical flow occurs at Froude numbers exceeding 1 (Vogel 1981, Gordon et al. 1992). All blackfly species in
this study preferred subcritical flow regions of the river. Using
the classification system of Davis and Barmuta (1989), highest densities of all five species of simuliids occurred within
subcritical-turbulent flows (i.e. Froude numbers <1 and Re
numbers >2000), although there are indications from these
data that S. nigritarse and S. merops tolerate supercriticalturbulent flows. According to Chow (1982), these two flow
types are the most common ones in streams and rivers. Since
hydraulic preferences for S. nigritarse in this study approach
supercritical conditions, it is not surprising that this species is
also encountered in more turbulent, larger river systems (relative to South African river systems; mean daily discharge
>5m3 s–1) (see, for example, studies by O’Keeffe and de Moor
1988, Palmer and O’Keeffe 1990). This is in contrast to S.
chutteri, which is unlikely to occur at densities large enough to
result in pest outbreaks at flow velocities of less than 1m s–1
(Rivers-Moore et al. in prep.) and which typically occurs in
supercritical-turbulent flows in large, turbid, regulated rivers
(de Moor 1994). Thus, certainly within southern Africa,
hydraulic properties of streams determine longitudinal macrodistribution patterns of larval blackfly species, which is
Rivers-Moore, de Moor, Birkholz and Palmer
reflected in feeding efficiency and labral fan patterns (Palmer
and Craig 2000).
This research also showed that those blackfly species
that prefer relatively low flow velocities occurred in lower
numbers, while higher velocities and more turbulent conditions sustained higher larval densities. This may be related
to food availability and to the ability of different blackfly
species to filter feed at different efficiencies under different
hydraulic conditions (Harrod 1964, Barber-James 2004).
Further research is recommended to obtain a better understanding of the links between turbulence, larval densities
and feeding efficiency.
Morphology and surface roughness of individual stones
are important determinants of local hydraulic conditions. At
these fine scales, small changes in hydraulic conditions
caused by minor changes in discharges, or even the presence of entrapped leaves (as with S. impukane), may be
significant enough to have large impacts on habitat suitability and larval densities of blackfly larvae. We were unable to
measure these in this study, although we believe this needs
further research, using more sensitive techniques.
Furthermore, at these small scales, changes in water
temperatures are likely to impact on water viscosity, and
consequently on the size of the boundary layer, which is
likely to impact on feeding efficiencies.
Acknowledgements — We thank the National Research Foundation of
South Africa for financial assistance. Geoff and Gill McIlleron and Julie
Carlisle of the Nature’s Valley Trust are thanked for hospitality and
assistance with fieldwork in the Salt River. Helen Barber-James of the
Albany Museum, Grahamstown, is thanked for identification of
Ephemeroptera. We also thank the anonymous referees for their
constructive criticism and comments.
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