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NCHRP Report 516: Pier and Contraction Scour in Cohesive Soils (2004)
National Cooperative Highway Research Program (NCHRP)

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Wang, J, Briaud, J-L, Li, Y, Chen, H-C, Nurtjahyo, P, Transportation Research Board. "5.21 Maximum Scour Depth Equation for Complex Pier Scour." NCHRP Report 516: Pier and Contraction Scour in Cohesive Soils. Washington, DC: The National Academies Press, 2004.

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Front Matter (R1-R10)
Summary (1-7)
1.4 Why Was This Problem Addressed? (8-8)
1.5 Approach Selected to Solve the Problem (9-9)
2.4 Erodibility and Correlation to Soil and Rock Properties (10-13)
3.3 EFA Test Data Reduction (14-14)
3.4 EFA Precision and Typical Results (15-16)
4.2 Small Flood Followed by Big Flood (17-17)
4.3 Big Flood Followed by Small Flood and General Case (18-18)
4.4 Hard Soil Layer Over Soft Soil Layer (19-20)
4.6 Equivalent Time (21-21)
4.7 Extended and Simple SRICOS-EFA Method (22-23)
4.8 Case Histories (24-25)
4.9 Predicted and Measured Local Scour for the Eight Bridges (26-28)
4.10 Conclusions (29-29)
5.4 Measuring Equipment (30-31)
5.5 Soils and Soil Bed Preparation (32-32)
5.6 Flume Tests: Procedure and Measurement (33-33)
5.8 Shallow Water Effect on Maximum Pier Scour Depth (34-35)
5.9 Shallow Water Effect on Initial Shear Stress (36-36)
5.11 Pier Spacing Effect on Maximum Scour Depth (37-37)
5.12 Pier Spacing Effect on Initial Scour Rate (38-38)
5.15 Pier Shape Effect on Initial Scour Rate (39-39)
5.18 Attack Angle Effect on Maximum Scour Depth (40-41)
5.20 Attack Angle Effect on Scour Hole Shape (42-42)
5.21 Maximum Scour Depth Equation for Complex Pier Scour (43-44)
6.2 Existing Knowledge on Numerical Simulations for Scour (45-45)
6.5 Shallow Water Effect: Numerical Simulation Results (46-46)
6.6 Shallow Water Effect on Maximum Shear Stress (47-47)
6.7 Pier Spacing Effect: Numerical Simulation Results (48-48)
6.9 Pier Shape Effect: Numerical Simulation Results (49-50)
6.10 Pier Shape Effect on Maximum Shear Stress (51-51)
6.11 Attack Angle Effect: Numerical Simulation Results (52-52)
6.12 Attack Angle Effect on Maximum Shear Stress (53-53)
6.13 Maximum Shear Stress Equation for Complex Pier Scour (54-55)
7.3 Flume Tests and Measurements (56-56)
7.4 Flume Tests: Flow Observations and Results (57-58)
7.5 Flume Tests: Scour Observations and Results (59-59)
7.6 Maximum and Uniform Contraction Depths for the Reference Cases (60-62)
7.7 Location of Maximum Contraction Depth for the Reference Cases (63-63)
7.8 Correction Factors for Transition Angle and Contraction Length (64-64)
7.9 SRICOS-EFA Method Using HEC-RAS Generated Velocity (65-65)
7.11 Scour Depth Equations for Contraction Scour (66-67)
8.3 Transition Angle Effect: Numerical Simulation Results (68-68)
8.4 Contracted Length Effect: Numerical Simulation Results (69-71)
8.6 Maximum Shear Stress Equation for Contraction Scour (72-75)
9.3 The Integrated SRICOS-EFA Method: Step-by-Step Procedure (76-80)
9.5 The SRICOS-EFA Program (81-83)
9.6 Output of the SRICOS-EFA Program (84-84)
10.4 Gill (1981) Database: Contraction Scour (85-87)
10.5 Remarks (88-88)
11.2 Preparation of the Future Hydrographs (89-89)
11.3 Risk Approach to Scour Predictions (90-90)
11.4 Observations on Current Risk Levels (91-92)
12.2 Example 2: Single Rectangular Pier with Attack Angle and Approaching Hydrograph (93-94)
12.3 Example 3: Group Rectangular Piers with Attack Angle and Approaching Constant Velocity (95-98)
12.4 Example 4: Contracted Channel with 90-Degree Transition Angle and Approaching Constant Velocity (99-102)
12.5 Example 5: Contracted Channel with 60-Degree Transition Angle and Approaching Hydrograph (103-104)
12.6 Example 6: Bridge with Group Piers and Contracted Channel with Hydrograph in Contracted Section (105-110)
13.1 Conclusions (111-112)
13.2 Recommendations, (113-113)
References (114-115)
Nomenclature (116-117)
Unit Conversions (118-118)
Appendix A - Photographs from the Flume Tests (119-125)
Abbreviations used without definitions in TRB publications (126-126)

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OCR for page 43
43 TABLE 5.8 Transition of the location of maximum scour depth Attack Angle (°) Location of the maximum scour depth 2.5cm 0 (1), (4) 5.5cm 0<<45 (1) (4) (4) 45 (1), (3) 6cm 7cm(1) 45<<90 (3) 90 (1), (2), (3), (4) (1) 14cm 8cm 10cm the location of the maximum scour depth will either happen at Corner 1 or Corner 3. When the attack angle increases, the (3) 6cm location of the maximum scour depth gradually moves from (3) 3cm (2) Corner 1 to Corner 3, and this transition is documented in (2) Table 5.8. It also was noted that the scour hole in the tested cohesive soil (Figure 5.27) was much smaller than the scour Figure 5.27. Shape of scour around a skewed pier in a hole in sands sketched by Raudkivi (1991). cohesive soil (left: attack angle = 15 degrees, right: attack angle = 30 degrees). 5.21 MAXIMUM SCOUR DEPTH EQUATION FOR COMPLEX PIER SCOUR In the previous sections, individual effects on the maximum pier scour depth were studied by flume testing. A series of (1) (1) 15° 15° (1) 45° (1) 45° figures and equations are given to quantify the corresponding correction factors. However, bridge piers are likely to exhibit (3) (3) (3) (3) a combination of these effects and recommendations are needed to combine these effects in the calculations. It is rec- ommended that the correction factors be multiplied in order to 0.5m 0.5m 0.5m 0.5m 0.5m 0.5m represent the combined effect: Figure 5.28. Configuration of the flume tests to verify the ( BvV ) 0.635 superposition rule. Zmax ( mm ) = 0.18 K w K sp K sh (5.7) where Zmax is the maximum depth of scour (mm); V is depth vidual effects described in previous sections were expected average velocity at the location of the pier if the pier or to happen simultaneously. The main parameters and results bridge was not there (m/s); B is the projection width of are summarized in Table 5.9, and the time history of the the pier (m); v is the kinematic viscosity of water (10E-6 scour development is plotted in Figure 5.29. The final (m2/s) at 20°C); Kw is the correction factor for shallow water maximum scour depth was obtained by using the hyper- effect (Equation 5.2), Ksp for pier spacing effect (Equation bola model. 5.3), and Ksh for pier shape effect (1.1 for rectangular piers); The maximum scour depths for the two tests were calcu- and B is the pier projection width (Equation 5.4 for rectan- lated according to Equation 5.7. The calculations are detailed gular pier). This is a common approach that implies that the in Table 5.10, and the measured results also are listed at the effects are independent and has been used in many instances bottom of that table which shows that the difference between before (HEC-18, Melville [1997]). the predictions and measurements is remarkably small (less Two complex pier flume tests were conducted with the than 5%). This tends to indicate that the chosen superposition configuration shown in Figure 5.28 where all of the indi- law works well for complex pier scour predictions. TABLE 5.9 Parameters and results for the complex pier flume tests Test H V L B C g Time Zmax No. (mm) (mm/s) (mm) (mm) (mm) (°) (h) (mm) Cp-1 375 330 244 61 500 15 115.32 175.4 Cp-2 375 330 244 61 500 45 150.67 285.7

OCR for page 44
44 200 160 Scour Depth (mm) 120 80 CP-1 CP-2 40 0 0 50 100 150 200 Time (Hr) Figure 5.29. Scour development curves for the complex pier flume tests. TABLE 5.10 Comparison of calculated and measured maximum pier scour depths PARAMETERS Cp - 1 Cp - 2 CALCULATION NOTE Primary Inputs B (mm) 61 61 Pier width L (mm) 244 244 Pier length H (mm) 375 375 Water depth (°) 15 45 Attack angle V (mm/s) 330 330 Mean approaching velocity C (mm) 500 500 Center to center pier spacing Attack Angle Effect B' (mm) 122.07 215.67 Projection width following Eq. (5.4) Basic Scour Depth Z1 (mm) 151.19 217.01 SRICOS: simple pier Eq. (5.6) Water Depth H/B' 3.07 1.74 Kw 1.00 1.00 Shallow water effect, Eq. (5.1) Contraction Effect C/B' 4.10 2.32 Ksp 1.0 1.233 Interpolated from Fig. 5.7 Pier Shape Effect Ksh 1.1 1.1 Calculated from Fig. 5.11 Composite Effect K 1.16 1.36 K= Kw·Ksp·Ksh Final Scour Depth Zcal(mm) 174.63 294.33 Zcal=K·Z1 Comparison Ztest (mm) 175.44 285.71 (Zcal-Ztest)/Ztest - 0.46 3.02 (%)