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Research paper

A multi-parameter design formula for riprap size selection at wing-wall abutments

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Pages 651-661 | Received 05 Oct 2019, Accepted 19 Aug 2020, Published online: 03 Dec 2020
 

Abstract

A numerically-based approach is used to obtain a size selection formula for the riprap stone part of the apron used to protect wing-wall abutments against erosion. Several series of simulations with a given mean riprap diameter are conducted to estimate the maximum bed shear stress over the riprap apron and then the maximum (critical) Froude number at which riprap stones will resist shear failure by the flow for cases where the abutment is placed in straight and curved channels with or without a floodplain. Simulation results show that some of the existing design formulas for wing-wall abutments placed in straight river channels are not conservative enough for relatively large floodplain widths. Using data from the numerical simulations, a modified, two parameter design formula for riprap size selection is proposed that explicitly incorporates the effects of bank curvature and floodplain width.

Acknowledgement

This research was funded by Grant # 15801350/15243500/69A3551747107 from the Mid-America Transportation Center (MATC). The authors would like to thank MATC for supporting this research.

Notation

Bf=

width of the floodplain (m)

C=

model coefficient (–)

D50=

mean riprap stone diameter (m)

d50=

mean sand diameter (m)

Fr=

Froude number (–)

Href=

length scale (m)

g=

gravitational acceleration (m s−2)

Ks=

shape factor (–)

ks=

surface roughness (m)

P=

pressure (Pa)

R=

channel radius of curvature (m)

Re=

Reynolds number (–)

R4=

width of the riprap apron (m)

Ss=

specific gravity of the riprap stone (–)

Ui=

velocity component along the i direction (m s−1)

uτc=

critical friction velocity for riprap shear failure (m s−1)

V=

velocity scale (m s−1)

W=

width of main channel (m)

xi=

space coordinate the i direction (m)

yf=

flow depth over the floodplain (m)

ym=

flow depth over the main channel (m)

α=

power law exponent (–)

δik=

Kronecker symbol (–)

τ=

bed shear stress (Pa)

ρ=

fluid density (kg m−3)

μ=

dynamic viscosity (kg m−1 s−1)

μt=

eddy viscosity (kg m−1 s−1)

Correction Statement

This article has been corrected with minor changes. These changes do not impact the academic content of the article.

Additional information

Funding

This work was supported by Mid-America Transportation Center, University of Nebraska-Lincoln [grant number: 15243500].

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