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砂防ダムを用いた土石流被害抑制のための研究

Study on prevention against debris flow by using Sabo Dam

15N3100021B ファークチァンサー クリスダ Fargseingsa Krisda

Key Words : debris flow, sabo dam, kanako model, rational equation

1. Background and Purposes

In 2011, The southern provinces of Thailand suffered from landslides by flash flood on 24-31 March. More than 1200 mm of precipitation was recorded within a few days. The effect of landslides causing devastating property damage and loss of life, at least 3 villages were seriously damaged and 10 peoples lost their lives. The infrastructure such as roads and overflow weirs have been destroyed.

The topographic of the area has been changed, especially along the debris flow paths. The debris flow length is about 2-3 kilometers with the largest wide of 500 meters ( Soralump Suttisak 2011).

From these problems, the present study wants to evaluate the effect of landslides and debris flow by using the real data when the structure countermeasures (Sabo dam) are constructed. Comparing the result data in some cases and find the proper way to prevent or mitigate this disaster in study area.

2. Study area

Near the end of March 2011, A heavy storm hit the eastern part of the Phanom Mountain. Three sub-basins have suffered from large precipitation and finally the debris flows were occurred on the 28

th

of March. Large granitic boulders of up to 10 meter in diameter were found at 2km from the landslide source (Landslide hazard map and study area as shown in Fig.2). These granite boulders destroyed the houses and structure in their path.

The mountain consists of the extrusion of granitic rock through sedimentary rock. The center area of the mountain is formed by granitic rock with steep slopes and high elevation. The area surrounding the peak of the mountain is a colluvium zone of granite debris. The outer area is highly fractured sandstone, mudstone, and other sedimentary rocks. Metamorphic rock is also found near the contact zone between the extruded granite and sedimentary rock.

3. Method 3.1 Model

Because of the characteristics of Phanom mountain consists of the granite rock and sedimentary rock and the stony debris flow occurred in the study area. Kanako 1D model was used to apply numerical simulations of debris flow, controlled with close, slit and grid sabo dams, to model variations in mountainous riverbeds. The model uses one-dimensional governing equations to simulate stony debris flows and the erosion (Satofuka and Mizuyama 2005). During simulations, users can view real-time images of debris flows, hydrographs, and the effects of sabo dams.

3.2 Governing equations

The continuity equation for the total volume and particles of the debris flow, as shown in Eq.1 and Eq.2:

Fig.1 Flow chart

Fig.2 Landslides occurrence probability and study area in Krabi province map.

( source : Department of mineral resource, Thailand )

x i M t

h

 

 (1)

*

) ( )

( iC

x CM t

Ch  

 

 (2)

The x-axis flow (main and cross flow direction) is given by the following momentum equation, as shown in Eq.3:

x

T

gh h x gh

uM t

M

 

 

 

 

 

 ( ) sin cos (3)

The equation for determining the change in the bed surface elevation, as shown in Eq.4:

 0

 

i t

z (4)

Where h isthe flowdepth (m), u is the x-axisflow velocity(m/s), M is flow flux(uh), C isthe sediment concentration by volume in the

Mt. Phanom

(2)

2 Fig.3 The arrangement of variables in 1D area.

Fig.4 The arrangement of variables at a Sabo dam .

debris flow, C

*

is the sediment concentration by volume in the movable bed layer, β is momentum correction factor(1.25 for stony debris flow), z is the bed elevation(m), t is time(s), i is the erosion or deposition velocity(m/s), g is the acceleration due to gravity(m/s

2

), Ɵ is the gradient of river bed, ρ

T

is mixture density(=ϭC+(1-C)ρ) (kg/m

3

), ϭ is density of sediment particle, ρ is the interstitial fluid density(kg/m

3

), and τ is the riverbed shearing stresses.

The erosion and deposition velocity have been given by Takahashi et al. 2001 are described as follows.

Erosion velocity, if C < C

;

d

m

M i C

  C

*

C -

 C (5)

Deposition velocity, if C ≥ C

;

d

m

i M

* '

C C - C

  (6)

where δ is erosion coefficient, δ’ is deposition coefficient, d

m

is mean diameter of sediment, C

is the debris flow sediment concentration.

3.3 Conditions of Sabo dam design

The numerical simulation model applied a staggered scheme using finite different method. Scalar and vector quantities are staggered by ∆x/2 in flow direction, as shown in Fig.3. Sabo dams are set at the calculation point of flow velocity, as shown in Fig.4. The effective flow depth, h’, at the dam point, which is used to calculate the flow flux and the flow surface gradient, Ɵ

e

, as shown below;

 

 

) (

;

) 0 (

; 0

) 0 (

; '

dam i i

dam i i

dam i i dam i i

z z h

z z h

z z h z z h

h (7)

 

 

 

2 tan

1

/

x z z h

i i dam

e

(8) Where h

i

is flow depth in scalar evaluation point next to the dam

Fig.5 Daily rainfall in Khao Phanom district, Krabi province.

Fig.6 Supplied Hydrograph

position in the upstream direction, z

i

is the riverbed height and z

dam

is the dam crest elevation.

3.4 Supplied hydrograph

For a debris flow calculation, the present study needs to set the hydrographic conditions. A debris flow is usually caused by heavy rainfall, so the nearest rainfall observation station is The Southern Meteorological Center (West Coast) at Krabi province. The peak daily rainfall, when debris flow was occurring, is 161.4 mm (29

th

march 2011). The present study assumed the most severe rainfall condition to be 161.4 mm/day and applied it to the rational formula (Aron and Kibler 1990), one of the simplest method formula to determine peak discharge from drainage basin runoff, as shown in Eq.9;

A r f Q

p

   

6 . 3

1 (9) where Q

p

is the peak discharge (m

3

/s), f is the coefficient of runoff (here, 0.7 for mountainous streams), r is the rainfall intensity (mm/h) and A is the basin area (km

2

), which was 3 km

2

for the study area.

For setting the debris flow hydrograph, the sediment volume need to be considered. The present study obtained a debris flow concentration of 30% by applied equation (Takashi et al. 2001), as shown in Eq.10;

) tan )(tan (

tan

 

C

(10) Then, the peak debris flow discharge was calculated by using the method described is the Sabo Master Plan for Debris Flow (NILIM Japan 2007) as shown in Eq.11;

p

sp

Q

C C Q C

*

*

(11)

where C

is the debris flow sediment concentration (0.3 ≤ C

≤ 0.9C

*

),

ϭ is the mass density of bed material (2650 kg/m

3

), ρ is the fluid

density (1000 kg/m

3

), Ø is the internal friction angle (35 deg.), tanƟ is

the average gradient of the river bed (1/6), C

*

is the concentration of

moveable bed (0.65) and Q

sp

is the debris flow peak discharge (m

3

/s).

(3)

3 Table.1 Scenarios for the simulation.

Scenario 1 Scenario 2 Scenario 3 Scenario 4

Num. of dam 1 2 3 4

Dam type Close, Slit Close, Slit Close Close Table.2 Other parameters for the simulation

The peak discharge of debris flow and sediment concentration were calculated to be 39m

3

/s and 30% respectively. Supplied hydrograph was presumed in triangle shaped and the duration time of debris flow was set at 1 hour. The daily rainfall in study area and supplied hydrograph are shown in Fig.5 and Fig.6, respectively.

3.5 Simulation cases and parameters

The present study simulated four scenarios by comparing number, types and locations of dam, as shown in Table.1. The red line is a downstream of river and used for river profile, because there are many peoples and cultivated area at downstream, as shown in Fig.9. The present study presumed the locations of Sabo dam, as shown in Fig.10, point A is 237.5 m from upstream, point B is 387.5m from upstream, point C is 537.5m form upstream, and point D is 687.5m from upstream.

In this debris flow case, the present study assumed diameter of material is 1 m. Manning’s coefficient, which is used for calculating riverbed shearing stresses of debris flow, was set as 0.03, the typical value for the mountainous river. The erosion and deposition coefficients were set as 0.0007 and 0.05, respectively (Takahashi 2007). For the 1D simulation area, the interval of 1D calculation points was set as 25m, the river width was set as 10m, the unstable soil layer was set as 2m (Keisuke et at. 2014) and dam height was set as 5m from the fixed layer.

Four- type of scenarios were simulated and analyzed. The results were percentage reduce of sediment volume at Obs.1. In each case, the result were compared with in case of without Sabo dam.

Scenario-0, without Sabo dam

Scenario-1, one-dam of close or slit type Sabo dam was simulated and compared in each dam location points (A, B, C and D).

Scenario-2, two-dam of close and slit type Sabo dams were simulated and compared in possible dam location points.

Scenario-3, three-dam of close type Sabo dams were simulated and compared in possible dam location points.

Scenatio-4, four-dam were set in all dam location points.

3.6 Simulation results

Calculated the river as shown in Fig.10 , with Kanako model. The simulations were performed to investigate sediment volume in

Fig.9 Phanom Mountain, Krabi province (Red line is a river profile).

Fig.10 Longitudinal profile of river

downstream (Obs.1) according to types and locations of dam. The best conditions of each scenario, as shown below;

Scenario-1, close type Sabo dam was placed on 387.5m(B) from upstream, percent reduced of sediment volume is 21.65%

Scenario-2, two-close type Sabo dam were placed on 387.5m and 687.5m (B,D) from upstream, percent reduced of sediment volume is 28.92%

Scenario-3, three-close type Sabo dam were placed on 387.5m, 537.5m and 687.5m (B,C,D) from upstream, percent reduced of sediment volume is 37.08%

Scenario-4, four-close type Sabo dam were placed on all of dam location points (A,B,C,D), percent reduced of sediment volume is 40.73%.

After simulated, the results of scenario-1, 2 revealed that close type Sabo dam is more effective than slit Sabo dam. The present study used only close type dam in scenario 3, 4. The more dam construct, the more sediment volume reduced. For example, graph of sediment discharge, Fig.11 and Fig.12 show the results of simulation of Scenario-1 and Scenario-4, respectively.

3.7 Simulation of percent sediment volume reduce due to increases intensity rainfall

Based on simulation results, as shown above. All of the best conditions, in each scenario, were used for produce the graph. The author made the prediction graph to predict the percent reduced of sediment volume by using only rainfall intensity (mm/h), as shown in Fig.13 . The graph shows the percent reduce of sediment volume when the rainfall is measured.

Parameters Value Unit

Simulation time 3600 s

Time step 0.01 s

Diameter of material 1 m

Mass density of bed material 2650 kg/m

3

Mass densit y of fluid phase 1000 kg/m

3

Concentration of movable bed 0.65

Internal friction angle 35

Acceleration of gravit y 9.8

Coefficient of erosion rate 0.0007 Coefficient of deposition rate 0.05

Manning’s coefficient 0.03

(4)

4 Table.3 B/C Analysis (m. = million)

Fig.11 Sediment discharge of one-dam placed at 387.5m from up stream

4. Benefit and cost

After the simulation, the best condition of each scenario were used to calculate the benefit and cost for the future construction plan.

cost on Constructi

project on constructi of

Benefit C

B

Benefit of construction is the difference between damage cost before and after construction. The total cost of damage at Krabi province, the information from Krabi public relation department, was 563 million baht (1,505 million yen). Unfortunately, it was no information of damage cost in study area. Therefore, area and number of victims were used for estimate the damage cost. After estimated, the cost of damage is 18 million baht ( 48 million yen ). The construction cost is source by bill of quantities. The best condition of each scenario were calculated the benefit by B/C analysis, the results as shown in Table.3

Although the more dam construct, the more sediment was reduced but, considered by B/C analysis, one-dam is the proper way to construct sabo dam in study area.

5. Conclusions

This research showed that the best condition to construct the sabo dam in Khao Phanom Mountain, Krabi province, Thailand. And evaluation graph, for damage of debris flow prediction when sabo dam was set in stream, is produced. As a result, the simulations revealed that close sabo dam is more effective than slit dam in study area. From B/C analysis, 1-dam, was placed on 387.5m from upstream, is the proper way for construction.

References

Aron G, Kibler DF ; Pond sizing for rational formula hydrographs. Water Resource Bulletin 26(2): 255-258, DOI:10.111/j.1752-1688.1990.tbo1368.x Keisuke Ono, So Kazama, Chaiwat Ekkawatpanit ; Assessment of rainfall-

induced shallow landslides in Phetchabun and Krabi provinces, Thailand.

Fig.12 Sediment discharge of four-dam placed at all locations

Fig.13 Percent reduced of sediment volume graph

Nat Hazards (2014) 74:2089–2107, DOI 10.1007/s11069-014-1292-3 Nakagawa H., Takahashi T., Satofuka Y. and Kawaike K.: Numerical

simulation of sediment disasters caused by heavy rainfall in Camuri Grande basin, Venezuela 1999, Proceeding of the 3

st

Conference on Debris-Flow Hazards Mitigation., pp.671-682, 2003.

National Institute for Land and Infrastructure Management, Ministry of Land, Infrastructure and Transport, Japan ; Manual of Technical Standard for establishing Sabo master plan for debris flow and driftwood, Technical Note of National Institute for Land and Infrastructure Management, Report.No.364 , 2007 ( in Japanese )

Satofuka Y., Mizuyama T. ; Numerical simulation of a debris flow in a mountainous river with a sabo dam, Journal of the Japan Society of Erosion Control Engineering vol.58, No.1, pp. 14-19, 2005 (in Japanese )

Soralump Suttisak ; 2011 disastrous landslides at Khao Panom,Krabi.Thailand Takahashi T, Nakagawa H, Satofuka Y. et al. ; Flood and sediment disasters

triggered by 1999 rainfall in Venezuela: A river restoration plan for an alluvial fan. Journal of Natural Disaster Sceience 23:65-82, 2001.

Takakahashi T. ; Debris flow : Mechanics, Prediction and Countermeasures.

Taylor&Francis, Leiden, CRC Press, London, UK, 2007.

Scenario 1 2 3 4

%reduce m. yen %reduce m. yen %reduce m. yen %reduce m. yen

Benefit 21.65 10.52 28.92 14.06 37.08 18.02 40.73 19.80

Construction Cost 0.64 1.28 1.92 2.56

B/C ratio 16.64 10.99 9.40 7.74

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