Keywords: Scour, 2D average velocity; RIVER 2D model, scour depth
2.1 Calculation of pier scour by the method of using 1D average velocity.
General scour.
O.V.Andreev (1955) [7] proposed a method to calculate the maximum general scour under the bridge (lower limit of scour) based on the analysis of the movement of alluvium particles in the mainstream and the river beach below the bridge. In the river beach part under the bridge, scour only starts when the velocity of water flowing under the bridge is greater than the allowed non-scour velocity (vox) of the geological soil layer forming the river beach (vbc>vox) and the scour will stop when the flow rate decreases to the allowed non-scour rate. In the mainstream, the flow rate is always greater than the allowable rate of non- scour of the riverbed’s geological layer and therefore the topsoil layer of the riverbed is always in a state of motion, but the river is not deeply eroded because there is a balance of alluvium along the river. Thus, the flow rate under the bridge is greater than the allowable rate without erosion, which is not the cause of scour in the mainstream and the deformation of the river under the bridge can only be explained by the imbalance of alluvium along the river. The overall scour under the bridge is calculated according to the principle of balance of sediment limit for the mainstream and the flow part with alluvium transport of O.V.Andreev (1955) [7]. The flow depth after scouring is determined according to equation (1) .
Where:
+ Q1=Qch, Q2=Q'ch: Water flow before and after bridge construction at the mainstream.
+ hch, h'ch : Water depth at mainstream before (natural time) and after scouring.
hch = ▼hhm – ▼htbs
▼hhm: Elevation of flow rate at natural time (taken according to design frequency)
▼htbs: average elevation of the riverbed
+ Bch, B'ch: Mainstream width before and after bridge construction.
Bch = L0 = 1657.34m.
B'ch = L = 1401.5 m.
Calculation results of general scour depth according to table 1 Table 1. Table of results for calculating the general scour depth of piers located on the main stream according to the 1D average velocity method.
Bridge Piers |
Bottom elevation (m) |
Surface elevation (m) |
Water Depth before scour hch (m) |
Water Depth after scour h'ch (m) |
Rising water (m) |
General depth scour (m) |
Bottom elevation after local scour (m) |
T3 |
-0.500 |
2.830 |
3.330 |
3.504 |
0.061 |
0.235 |
-0.735 |
T4 |
-1.250 |
2.830 |
4.080 |
4.293 |
0.061 |
0.274 |
-1.524 |
T5 |
-1.240 |
2.830 |
4.070 |
4.283 |
0.061 |
0.274 |
-1.514 |
T6 |
-1.210 |
2.830 |
4.040 |
4.251 |
0.061 |
0.272 |
-1.482 |
T7 |
-0.960 |
2.830 |
3.790 |
3.988 |
0.061 |
0.259 |
-1.219 |
T8 |
-1.420 |
2.830 |
4.250 |
4.472 |
0.061 |
0.283 |
-1.703 |
T9 |
-1.720 |
2.830 |
4.550 |
4.788 |
0.061 |
0.299 |
-2.019 |
T10 |
-1.900 |
2.830 |
4.730 |
4.977 |
0.061 |
0.308 |
-2.208 |
T11 |
-2.050 |
2.830 |
4.880 |
5.135 |
0.061 |
0.316 |
-2.366 |
T12 |
-2.540 |
2.830 |
5.370 |
5.651 |
0.061 |
0.342 |
-2.882 |
T13 |
-2.630 |
2.830 |
5.460 |
5.745 |
0.061 |
0.346 |
-2.976 |
T14 |
-3.400 |
2.830 |
6.230 |
6.556 |
0.061 |
0.387 |
-3.787 |
T15 |
-8.150 |
2.830 |
10.980 |
11.554 |
0.061 |
0.635 |
-8.785 |
T16 |
-11.600 |
2.830 |
14.430 |
15.184 |
0.061 |
0.815 |
-12.415 |
T17 |
1.260 |
2.830 |
1.570 |
1.652 |
0.061 |
0.143 |
1.117 |
T18 |
0.000 |
2.830 |
2.830 |
2.978 |
0.061 |
0.209 |
-0.209 |
T19 |
-0.050 |
2.830 |
2.880 |
3.031 |
0.061 |
0.212 |
-0.262 |
T20 |
0.040 |
2.830 |
2.790 |
2.936 |
0.061 |
0.207 |
-0.167 |
T21 |
-0.040 |
2.830 |
2.870 |
3.020 |
0.061 |
0.211 |
-0.251 |
Caculating local Scour (p = 1%)
Two authors N.X Truc and N.H. Khai (1982) [8] introduced the formula for determining the largest local scour value at the bridge pier. Based on the research results on the causes and development process of local scour on pier scour models in the hydraulic laboratory and the research results of foreign authors, a reasonable structural form of the local scour calculation formula has been selected. The formula (2) has the following simple form. When v³ vox (for mainstream piers).
hcb= 0,52.kd.b0,88.h0,12.(V/Vox)1,16 (2)
Where:
+ hcb: maximum local scour depth at bridge pier, m
+ kd: factor taking into account the influence of cylinder shape, taken as 0,1kζ
+ kζ : Iaratslaxev's shape coefficient
+ h: depth of water flow at bridge pier before local scour, m
+ V: water velocity at bridge pier before local scour, m/s
+ Vox : allowable no- scour velocity of the soil layer at the location where scour development
+ b: calculated width of the cylinder, m
The results of local scour calculation are obtained from Table 2
Table 2. Table of results of calculation of local scour depth of piers located on the main stream according to the average 1D velocity method.
Bridge Piers |
Shape factor Kd |
Width of pier b (m) |
Depth of water flow h (m) |
Velocity V (m/s) |
No-scour velocity Vox (m/s) |
Ratio V/Vox |
Maximum local scour depth hcb (m) |
T3 |
0.97 |
1.8 |
3.565 |
1.484 |
0.720 |
2.061 |
2.280 |
T4 |
0.97 |
1.8 |
4.354 |
1.484 |
0.790 |
1.878 |
2.097 |
T5 |
0.97 |
1.8 |
4.344 |
1.484 |
0.780 |
1.903 |
2.128 |
T6 |
0.97 |
1.8 |
4.312 |
1.484 |
0.770 |
1.927 |
2.158 |
T7 |
0.97 |
1.8 |
4.049 |
1.484 |
0.740 |
2.005 |
2.243 |
T8 |
0.97 |
1.8 |
4.533 |
1.484 |
0.805 |
1.843 |
2.062 |
T9 |
0.97 |
1.8 |
4.849 |
1.484 |
0.815 |
1.821 |
2.049 |
T10 |
0.97 |
1.8 |
5.038 |
1.484 |
0.820 |
1.810 |
2.044 |
T11 |
0.97 |
2 |
5.196 |
1.484 |
0.825 |
1.799 |
2.235 |
T12 |
0.97 |
4 |
5.712 |
1.484 |
0.835 |
1.777 |
4.103 |
T13 |
0.97 |
5 |
5.806 |
1.484 |
0.840 |
1.767 |
4.969 |
T14 |
0.97 |
5 |
6.617 |
1.484 |
0.860 |
1.726 |
4.911 |
T15 |
0.97 |
5 |
11.615 |
1.484 |
0.910 |
1.631 |
4.921 |
T16 |
0.97 |
5 |
15.245 |
1.484 |
0.950 |
1.562 |
4.837 |
T17 |
0.97 |
4 |
1.713 |
1.484 |
0.650 |
2.283 |
4.748 |
T18 |
0.97 |
2 |
3.039 |
1.484 |
0.705 |
2.105 |
2.515 |
T19 |
0.97 |
1.8 |
3.092 |
1.484 |
0.705 |
2.105 |
2.297 |
T20 |
0.97 |
1.8 |
2.997 |
1.484 |
0.690 |
2.151 |
2.346 |
T21 |
0.97 |
1.8 |
3.081 |
1.484 |
0.700 |
2.120 |
2.315 |
Published on 24/11/23
Accepted on 30/10/23
Submitted on 31/07/23
Volume 39, Issue 4, 2023
DOI: 10.23967/j.rimni.2023.10.009
Licence: CC BY-NC-SA license
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