This document provides guidance on using the area-slope method to estimate stream discharge indirectly when direct measurement is not possible. It describes the principles and steps of the area-slope method, including selecting a study reach, measuring the cross-sectional area and water surface slope, evaluating velocity using Manning's formula, and computing discharge. Guidelines are given for selecting sites, measuring cross-sections and slope, determining roughness coefficients, and performing calculations. The area-slope method provides a rough estimate of discharge but has limitations due to uncertainties in roughness coefficients.
In this study the kinematic wave equation has been solved numerically using the modified Lax
explicit finite difference scheme (MLEFDS) and used for flood routing in a wide prismatic channel and a nonprismatic
channel. Two flood waves, one sinusoidal wave and one exponential wave, have been imposed at the
upstream boundary of the channel in which the flow is initially uniform. Six different schemes have been
introduced and used to compute the routing parameter, the wave celerity c. Two of these schemes are based on
constant depth and use constant celerity throughout the computation process. The rest of the schemes are based
on local depths and give celerity dependent on time and space. The effects of the routing parameter c on the
travel time of flood wave, the subsidence of the flood peak and the conservation flood flow volume have been
studied. The results seem to indicate that there is a minimal loss/gain of flow volume whatever the scheme is.
While it is confirmed that neither of the schemes is 100% volume conservative, it is found that the scheme
Kinematic Wave Model-2 (KWM-II) gives the most accurate result giving only 0.1% error in perspective of
volume conservation. The results obtained in this study are in good qualitative agreement with those obtained in
other similar studies.
Through the lack of technical instruments for construction and measurement. A small attempt was made by the team to demonstrate the working of Parshall Flume and Discharge measuring Accessories with support for Dr.-Ing Ramesh Kumar Maskey, Kathmandu University (KU) as part of our hydro-power project.
Flow Equations for sluice gate.Introduces different flow equations to students which are widely utilized for the design of sluice gates connected to open channel.This tutorial will help to understand and articulate the basic flow equation utilized by designers all over the world.
Overbank Flow Condition in a River SectionIDES Editor
When the flows in natural or man made channel
sections exceed the main channel depth, the adjoining
floodplains become inundated and carry part of the river
discharge. Due to different hydraulic conditions prevailing in
the river and floodplain of a compound channel, the mean
velocity in the main channel and in the floodplain are different.
This leads to the transfer of momentum between the main
channel water and that of the floodplain making the flow
structure more complex. Results of some experiments
concerning the overbank flow distribution in a compound
channel are presented. Flow sharing in river channels is
strongly dependant on the interaction between flow in the
main channel and that in the floodplain. The influence of the
geometry on velocity and flow distribution and different
functional relationships are obtained. Dimensionless
parameters are used to form equations representing the over
bank flow sharing in the subsections. The equations agree
well with experimental discharge data and other published
data. Using the proposed method, the error between the
measured and calculated discharge distribution for the a
compound sections is found to be the minimum when compared
with that using other investigators.
OPEN CHANNEL FLOW AND HYDRAULIC MACHINERY
Open channel flow: Types of flows – Type of channels – Velocity distribution – Energy and momentum correction factors – Chezy’s, Manning’s; and Bazin formula for uniform flow – Most Economical sections. Critical flow: Specific energy-critical depth – computation of critical depth – critical sub-critical – super critical flows
Non-uniform flows –Dynamic equation for G.V.F., Mild, Critical, Steep, horizontal and adverse slopes-surface profiles-direct step method- Rapidly varied flow, hydraulic jump, energy dissipation
In this study the kinematic wave equation has been solved numerically using the modified Lax
explicit finite difference scheme (MLEFDS) and used for flood routing in a wide prismatic channel and a nonprismatic
channel. Two flood waves, one sinusoidal wave and one exponential wave, have been imposed at the
upstream boundary of the channel in which the flow is initially uniform. Six different schemes have been
introduced and used to compute the routing parameter, the wave celerity c. Two of these schemes are based on
constant depth and use constant celerity throughout the computation process. The rest of the schemes are based
on local depths and give celerity dependent on time and space. The effects of the routing parameter c on the
travel time of flood wave, the subsidence of the flood peak and the conservation flood flow volume have been
studied. The results seem to indicate that there is a minimal loss/gain of flow volume whatever the scheme is.
While it is confirmed that neither of the schemes is 100% volume conservative, it is found that the scheme
Kinematic Wave Model-2 (KWM-II) gives the most accurate result giving only 0.1% error in perspective of
volume conservation. The results obtained in this study are in good qualitative agreement with those obtained in
other similar studies.
Through the lack of technical instruments for construction and measurement. A small attempt was made by the team to demonstrate the working of Parshall Flume and Discharge measuring Accessories with support for Dr.-Ing Ramesh Kumar Maskey, Kathmandu University (KU) as part of our hydro-power project.
Flow Equations for sluice gate.Introduces different flow equations to students which are widely utilized for the design of sluice gates connected to open channel.This tutorial will help to understand and articulate the basic flow equation utilized by designers all over the world.
Overbank Flow Condition in a River SectionIDES Editor
When the flows in natural or man made channel
sections exceed the main channel depth, the adjoining
floodplains become inundated and carry part of the river
discharge. Due to different hydraulic conditions prevailing in
the river and floodplain of a compound channel, the mean
velocity in the main channel and in the floodplain are different.
This leads to the transfer of momentum between the main
channel water and that of the floodplain making the flow
structure more complex. Results of some experiments
concerning the overbank flow distribution in a compound
channel are presented. Flow sharing in river channels is
strongly dependant on the interaction between flow in the
main channel and that in the floodplain. The influence of the
geometry on velocity and flow distribution and different
functional relationships are obtained. Dimensionless
parameters are used to form equations representing the over
bank flow sharing in the subsections. The equations agree
well with experimental discharge data and other published
data. Using the proposed method, the error between the
measured and calculated discharge distribution for the a
compound sections is found to be the minimum when compared
with that using other investigators.
OPEN CHANNEL FLOW AND HYDRAULIC MACHINERY
Open channel flow: Types of flows – Type of channels – Velocity distribution – Energy and momentum correction factors – Chezy’s, Manning’s; and Bazin formula for uniform flow – Most Economical sections. Critical flow: Specific energy-critical depth – computation of critical depth – critical sub-critical – super critical flows
Non-uniform flows –Dynamic equation for G.V.F., Mild, Critical, Steep, horizontal and adverse slopes-surface profiles-direct step method- Rapidly varied flow, hydraulic jump, energy dissipation
The time required for the rain falling at the most distant point in the drainage area (i.e., on the fringe of the catchment ) to reach the concentration point is called the concentration time.
This is a very significant variable since only such storms of duration greater than the time of concentration will be able to produce runoff from the entire catchment area and cause high intensity floods.
The characteristics of the drainage net may be physically described by:
The number of streams
The length of streams
Stream density
Drainage density
The country’s annual renewable fresh water resources amount to some 122 BCM/yr in the twelve river basins.
However, only 3% remains in the country.
The rest, 97% is lost in runoff to the lowlands of neighboring countries.
Hydrographic survey is the survey of physical features present underwater.
This slide briefs you about the definition of the survey, its application, use, etc. It also discusses the sounding process used in the hydrographic survey.
In this work the impact of the tidal wave on pollutant residence time within Nador
lagoon has been computed using an Eulerian approach and a 2D hydrodynamical model.
The model is based on the finite volume method; it solves the shallow water equations on
spatial domain that represents the Nador lagoon. The residence time has been defined
through the remnant function of a passive tracer released inside the lagoon. The renewal
capacity of the Nador Lagoon has been investigated when forced by the astronomic tide.
The influence of tidal wave on residence time has been defined by the return flow, and
computed for two scenarios during winter and spring periods.
The Art of the Pitch: WordPress Relationships and SalesLaura Byrne
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1. Insights into SAP testing best practices
2. Heatmap utilization for testing
3. Optimization of testing processes
4. Demo
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Execution from the test manager
Orchestrator execution result
Defect reporting
SAP heatmap example with demo
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Paper presented at SYNERGY workshop at AVI 2024, Genoa, Italy. 3rd June 2024
https://alandix.com/academic/papers/synergy2024-epistemic/
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GraphRAG is All You need? LLM & Knowledge GraphGuy Korland
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The IoT and OT threat landscape report has been prepared by the Threat Research Team at Sectrio using data from Sectrio, cyber threat intelligence farming facilities spread across over 85 cities around the world. In addition, Sectrio also runs AI-based advanced threat and payload engagement facilities that serve as sinks to attract and engage sophisticated threat actors, and newer malware including new variants and latent threats that are at an earlier stage of development.
The latest edition of the OT/ICS and IoT security Threat Landscape Report 2024 also covers:
State of global ICS asset and network exposure
Sectoral targets and attacks as well as the cost of ransom
Global APT activity, AI usage, actor and tactic profiles, and implications
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Attacks on counties – USA
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In-depth analysis of the cyber threat landscape across North America, South America, Europe, APAC, and the Middle East
Why are attacks on smart factories rising?
Cyber risk predictions
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Connector Corner: Automate dynamic content and events by pushing a buttonDianaGray10
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Have the message received by managers and peers along with a test email for review
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If the “Approve” button is clicked, a Jira/Zendesk ticket is created for the marketing design team
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Session Overview
-------------------------------------------
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1. GOVERNMENT OF INDIA
CENTRAL WATER COMMISSION
CENTRAL TRAINING UNIT
HYDROLOGY PROJECT
TRAINING OF TRAINERS
IN
HYDROMETRY
ESTIMATION OF DISCHARGE BY
AREA-SLOPE METHOD
D.S.CHASKAR
DEPUTY DIRECTOR
CENTRAL TRAINING UNIT
CENTRAL WATER COMMISSION
PUNE - 411 024
2. HYDROLOGY PROJECT ESTIMATION OF DISCHARGE BY AREA-SLOPE METHOD
CTU, PUNE TRAINING OF TRAINERS IN HYDROMETRY PAGE NO. 2
3. HYDROLOGY PROJECT ESTIMATION OF DISCHARGE BY AREA-SLOPE METHOD
CTU, PUNE TRAINING OF TRAINERS IN HYDROMETRY PAGE NO. 3
ESTIMATION OF DISCHARGE BY AREA-SLOPE METHOD
1.0 INTRODUCTION :
Streamflow representing the run-off phase of the hydrologic cycle is the most
important basic data for hydrologic studies precipitation, evaporation and
evapotranspiration are all difficult to measure exactly and various methods of
measurements have severe limitations. In contrast the measurement of
streamflow is amenable to fairly accurate assessment. Interestingly, streamflow is
the only part of the hydrologic cycle that can be measured accurately.
A stream can be defined as a flow channel into which the surface run-off from a
specified basin drains. Streamflow is measured in units of discharge (m3
/s)
occurring at a specified time and constitutes historical data. The measurement
of discharge in a stream forms an important branch of "Hydrometry", the
science and practice of water measurement. This topic deals with one of the
many streamflow measurement techniques to provide an appreciation of this
important aspect of engineering hydrology.
Streamflow measurement techniques can be broadly classified into two categories
as (i) direct determination and (ii) indirect determination. Under each category
there are a host of methods, the important ones are listed below :
1. Direct determination of stream discharge :
a) Area-velocity method
b) dilution techniques
c) electronic method
d) ultrasonic method
2. Indirect determination of streamflow :
a) Hydraulic structures, such as weirs, flumes and gated structures, and
b) Area-slope method
2.0 SCOPE AND APPLICATION OF THE AREA-SLOPE METHOD :
Area-slope method provides an approximate estimate of discharge in the streams
and is used when measurement of discharge by accurate method like the area
4. HYDROLOGY PROJECT ESTIMATION OF DISCHARGE BY AREA-SLOPE METHOD
CTU, PUNE TRAINING OF TRAINERS IN HYDROMETRY PAGE NO. 4
velocity method is not possible. Such situation may arise due to reasons like non
availability or break down of means or equipment required for making current
meter measurements, inaccessibility of the site due to floods, presence of debris
and floating matter in the flood, flow preventing the use of current meter, etc. In
flashy streams, high floods may pass without being measured due to their short
duration. If the magnitude of such floods are required to be assessed after their
occurrence, we resort to area slope method.
In the event of the failure of routine methods for measuring discharges in open
channels, due to either rapid rise and fall of floods or lack of equipment required
for discharge measurements, the slope-area method provides a rough estimate of
the discharge in spite of many limitations, the major limitation being the difficulty
of a correct assessment of the rugosity coefficient `n' for application of
Manning's formula. The value of rugosity coefficient depends on stage of flow,
bed material, the nature of the channel, etc.
This method can be used with some degree of accuracy in channels with stable
bed and banks having relatively coarse bed material. This method may also be
used in other cases, such as alluvial channels, subject to the acceptance of larger
errors involved in the selection of the value of the rugosity coefficient `n'. It is,
however, not desirable to use this method in the case of very large channels or
channels with very flat slopes and high sediment concentration or channels with
significant curvature.
The method explained here deals only with adhoc measurements of discharge
and such discharge values should not be used for establishing rating curves.
3.0 PRINCIPLE OF THE METHOD OF MEASUREMENT
A measuring reach of the stream is chosen for which the mean area of such
cross section and the surface slope of the flowing water in that reach are
determined. The mean velocity is then worked out by using the known open
channel flow formulated such as the Manning's formula by selecting appropriate
rugosity coefficient depending on the physical conditions of the channel. The
approximate discharge is then computed as the product of the mean velocity and
the average cross-sectional area of the reach.
5. HYDROLOGY PROJECT ESTIMATION OF DISCHARGE BY AREA-SLOPE METHOD
CTU, PUNE TRAINING OF TRAINERS IN HYDROMETRY PAGE NO. 5
4.0 SELECTION OF SITE
1. The river reach should be fairly straight having stable bed and banks and
uniform cross-section over a length of at least five times the width of the
channel. In any case, the length should not be less than about 300m.
2. The slope should be such that surface drop is as large as possible but not
less than a minimum of 15 cm. in the length of the reach selected.
3. The flow in the reach should be free from significant disturbances,
draw-down or back-water effect of any structure or tributary joining
upstream or down stream.
4. The orientation of the reach should be such that the direction of the flow is
as closely as possible normal to that of the prevailing wind.
5. The flow in the channel shall be contained within its banks for all stages at
which this method is used.
6. The site should not be unduly exposed to wind.
7. The site chosen should be easily accessible at all times.
8. If no uniform reach is available, the reach should preferably be
converging rather than diverging.
5.0 MEASUREMENT OF SLOPE
Gauges should be installed at least in three cross-sections, on either bank of the
river. If three cross-sections are chosen two should be at the ends of selected
reach and one at the centre. The alignment of each cross-section should be
normal to the general direction of flow.
Before the start of each discharge measurement, information regarding the date,
time, weather conditions, direction of wind, current etc. should be recorded. All
gauges should be observed at suitable intervals and recorded through the period of
measurement including initial and terminal readings.
6. HYDROLOGY PROJECT ESTIMATION OF DISCHARGE BY AREA-SLOPE METHOD
CTU, PUNE TRAINING OF TRAINERS IN HYDROMETRY PAGE NO. 6
Slope of water surface is computed from the average of gauge observations at
either of the reach. The intermediate gauge is used to confirm that the slope is
uniform throughout the reach.
When accurate gauges do not exist or have been destroyed, flood marks on the
banks may be used for estimation of the slope. In such cases, an effort should
be made to locate, investigate and fix as many flood marks as possible in the
reach with least possible delay after occurrence of the flood.
6.0 CROSS-SECTIONAL AREA AND WETTED PERIMETER OF STREAM
Generally average area of cross-section in the observation reach is taken as the
mean of three sections - two end sections and the central section. If for any
reason, it is not possible to measure more than one cross-section, the central one
only may be observed.
The cross-sections should be measured for each discharge observations at or as
near the time as possible, at which the gauge observations are made. It is often not
possible to meausre the cross section during flood and therefore, to this extent an
error may be introduced due to an observed and temporary change in
cross-sections. However, rivers with rocky bed and banks, and carrying little
bed charge are least susceptible to these changes. In such cases, it will be
sufficient to observe the cross-sections before and after the floods.
If the reach is substantially uniform and there are insignificant differences in
the cross-sectional areas, A1, A2 _........ Am at the chosen sections, the mean
area of cross- section for the reach of the stream may be taken as
A = A1 + 2A2 + ........... 2Am - 1+ Am
---------------------------------------
2 ( m - 1)
Similarly, if P1, P2 .......... Pm are the corresponding wetted perimeter of the
chosen cross-sections, the mean wetted perimeter for the reach may be taken as
P = P1 + 2P2 + .............. + 2 Pm-1 + Pm
-------------------------------------------------
2(m-1)
7. HYDROLOGY PROJECT ESTIMATION OF DISCHARGE BY AREA-SLOPE METHOD
CTU, PUNE TRAINING OF TRAINERS IN HYDROMETRY PAGE NO. 7
7.0 EVALUATION OF VELOCITY
The mean velocity representing the cross-section of the flow area in the reach
may be computed using Manning's formula as given below :
V = R2/3
S ½
(Matric units)
n
V = 1.486 R2/3
S ½
(FPS units)
n
where
V - Mean velocity
R - Hydraulic mean depth = A/P
n - Rugosity coefficient having a value given in Table 1 & 2.
s - Slope corrected for the Kinetic energy difference at the two ends.
= Z1
- Z2
+ (V1
2
- V2
2
)
( 2g 2g )
-------------------------------
L
L - Length of the reach
Z1 & Z2 are static heads (water levels) at the end sections.
V1
2
& V2
2
2g 2g are the corresponding velocity heads
V1 & V2 are mean velocities at the end sections at (1) and (2) as shown in
Fig. 1.
8.0 VALUE OF RUGOSITY COEFFICIENT :
Where a reasonable value of rugosity coefficient (also called roughness
coefficient or retardation coefficient) can be determined from actual discharge
measurements at the nearest lower stages by a more accurate method, say the
area velocity method using current meter, the value so obtained may be chosen.
In the absence of measured data, the values given in table I may be assumed for
open channels with relatively coarse bed material.
8. HYDROLOGY PROJECT ESTIMATION OF DISCHARGE BY AREA-SLOPE METHOD
CTU, PUNE TRAINING OF TRAINERS IN HYDROMETRY PAGE NO. 8
Table I Value of Rugosity coefficient 'n’ for open channels with
relatively coarse bed material not characterized by bed
formation
Sl.
No.
Type of bed material Size of bed material
equivalent diameter
in mm
Rugosity coefficient
'n’
1 Gravel 4 to 8
8 to 20
20 to 60
0.019 to 0.020
0.020 to 0.022
0.022 to 0.027
2 Cobbles and Shingle 60 to 110
110 to 250
0.027 to 0.030
0.030 to 0.035
In the case of alluvial open channels with other than coarse bed material and
channels having vegetations, clay and rocky banks etc. values given in Table II
may be used as a guide.
9.0 COMPUTATION OF DISCHARGE :
The discharge shall be calculated by multiplying the mean velocity obtained from
7.0 by the mean cross-sectional area obtained from 6.0.
The discharge computation using energy gradient rather than water surface slope,
has to be carried out by method of successive trials. To start with, discharge is
computed by using surface slope in Manning's formula. With this discharge,
knowing the upstream and downstream cross-sections, velocities and velocity
heads are computed from which energy gradient is obtained. In the next trial,
this energy gradient is substituted for water surface slope in the Manning's
formula. A few more trials will give reasonably good result.
References :
1. I.S. Recommendation for Liquid Flow Measurement in open channels by
Slope-Area Method. (IS 2912-1964).
2. "Stream Gauging" Manual by H.G. Hiranandani and S.V. Chitale.
3. W.H.O. Operational Hydrology Report NO. 13, "Manual on stream
gauging" Vol. I.
4. Chow, V.T., "Handbook of Applied Hydrology".
5. Subramanya K., "Flow in Open Channels".
9. HYDROLOGY PROJECT ESTIMATION OF DISCHARGE BY AREA-SLOPE METHOD
CTU, PUNE TRAINING OF TRAINERS IN HYDROMETRY PAGE NO. 9
Table II Value of Rugosity Coefficient 'n’ for open channels with other than
coarse bed material
Type of channel and Description Rugosity
Coefficient
'n’
Excavated or Dredged
a) Earth, straight and uniform
1) Clean, recently completed
2) Clean after weathering
3) With short grass, few weeds
b) Rock Cuts
1) Smooth and Uniform
2) Jagged and Irregular
0.016 to 0.020
0.018 to 0.025
0.022 to 0.033
0.025 to 0.040
0.035 to 0.050
Natural Streams
a) Minor streams (top width at flood Stage less than 30 m ( or 100 ft.)
1) Streams on plains - clean, straight full stage, no rifts or deep pools
b) Flood on plains
1) Pasture, no brush
i) Short grass
ii) High grass
2) Cultivated areas
i) No crop
ii) Nature row crops
iii) Nature field crops
3) Brush
i) Scattered brush, heavy weeds
ii) Light brush and trees (without foliage)
iii) Light brush and trees (with foliage)
iv) Medium to dense brush (without foliage)
v) Medium to dense brush (with foliage)
4) Trees
i) Cleared land with tree stumps, no sprouts
ii) Same as above, but with heavy growth of sprouts
iii) Heavy stand of timber, a few down trees, little undergrowth
flood stage below branches
iv) Same as above, but with flood stage reaching branches
v) Dense willows, summer, straight
0.025 to 0.033
0.025 to 0.035
0.030 to 0.050
0.020 to 0.040
0.025 to 0.045
0.030 to 0.050
0.035 to 0.070
0.035 to 0.060
0.040 to 0.080
0.045 to 0.110
0.070 to 0.260
0.030 to 0.050
0.050 to 0.080
0.080 to 0.120
0.100 to 0.160
0.110 to 0.200
10. HYDROLOGY PROJECT ESTIMATION OF DISCHARGE BY AREA-SLOPE METHOD
CTU, PUNE TRAINING OF TRAINERS IN HYDROMETRY PAGE NO. 10
V1
2/2g
Z1
hL(1-2)
V2
2/2g
Z2
LONGITUDINAL PROFILE
L
River Bed
FLOW
Datum
ENERGY GRADIENT
11. HYDROLOGY PROJECT ESTIMATION OF DISCHARGE BY AREA-SLOPE METHOD
CTU, PUNE TRAINING OF TRAINERS IN HYDROMETRY PAGE NO. 11
LEFT BANK
RIGHT BANK
PLAN VIEW
RIVER REACH SELECTED FOR SLOPE AREA METHOD
V1 V2
SECTION 1 SECTION 2
12. HYDROLOGY PROJECT ESTIMATION OF DISCHARGE BY AREA-SLOPE METHOD
CTU, PUNE TRAINING OF TRAINERS IN HYDROMETRY PAGE NO. 12
PROBLEMS
1. During a high flow water-surface elevations of a small stream were noted at two
sections A and B, 10 km apart. These elevations and other salient hydraulic
properties are given below:
Section Water-
Surface
elevation
(m)
Area of cross-
section
(m
2
)
Hydraulic
radius
(m)
Remarks
A 104.771 73.293 2.733 A is
upstream
of B
B 104.500 93.375 3.089 n = 0.020
The eddy loss coefficient of 0.3 for gradual expansion and 0.1 for gradual
contraction are appropriate. Estimate the discharge in the stream.
2. A small stream has a trapezoidal cross section with base width of 12 m and side
slope 2 horizontal : 1 vertical in a reach of 8 km. During a flood a flood the high
water levels recorded at either ends of the reach are as below :
Section Elevation of bed Water surface
elevation
Remarks
Upstream 100.20 102.70 Manning’s n =
0.030
Downstream 98.60 101.30
Estimate the discharge in the stream.
3. During a flood flow the depth of water in a 10 m wide rectangular channel was
found to be 3.0 and 2.9 m at two sections 200 m apart. The drop in the
water-surface elevation was found to be 0.12 m. Assuming Manning's
coefficient to be 0.025, estimate the flood discharge through the channel.
13. HYDROLOGY PROJECT ESTIMATION OF DISCHARGE BY AREA-SLOPE METHOD
CTU, PUNE TRAINING OF TRAINERS IN HYDROMETRY PAGE NO. 13