River Channel Forms in Relation to Bank Steepness: A Theoretical Investigation Using a Variational Analytical Method

Riverbanks vary considerably in anti-scourability and consequently take various profiles. By using an isosceles trapezoid as the generalized form of river channel cross-sections and then incorporating the effects of bank angle into the variational analytical approach developed by Huang and Nanson (2000), this study presents a detailed theoretical investigation of the self-adjustment of alluvial channel forms. It is demonstrated that when alluvial channel flow achieves stable equilibrium, a significant decrease in riverbank steepness leads to a slight decrease in maximum sediment (bedload) discharge, and yet results in a significant increase in optimal channel width and a considerable decrease in optimal channel depth. The hydraulic geometry relations, theoretically derived for bank steepness to vary across a wide range, show that among the multivariant controls, the roles of bed sediment size, channel roughness, flow discharge and sediment (bedload) discharge are independent of bank steepness. While the effects of bank steepness illustrated in the theoretically derived hydraulic geometry relations are highly consistent with the results of threshold theory and previous empirical studies, limitations on using bank angle to reflect the anti-scourability of natural riverbanks are also highlighted.

[1]  B. Eaton,et al.  Predicting gravel bed river response to environmental change: the strengths and limitations of a regime‐based approach , 2017 .

[2]  G. Nanson,et al.  Self‐adjustment in rivers: Evidence for least action as the primary control of alluvial‐channel form and process , 2017 .

[3]  G. Nanson,et al.  A philosophy of rivers: Equilibrium states, channel evolution, teleomatic change and least action principle , 2016 .

[4]  Heqing Huang,et al.  Reformulation of the bed load equation of Meyer‐Peter and Müller in light of the linearity theory for alluvial channel flow , 2010 .

[5]  G. Nanson,et al.  The hydraulic geometry of narrow and deep channels; evidence for flow optimisation and controlled peatland growth , 2010 .

[6]  G. Nanson,et al.  Least action principle, equilibrium states, iterative adjustment and the stability of alluvial channels , 2008 .

[7]  G. Nanson,et al.  Why some alluvial rivers develop an anabranching pattern , 2007 .

[8]  Howard H. Chang,et al.  Scale independent linear behavior of alluvial channel flow , 2006 .

[9]  R. Millar Theoretical regime equations for mobile gravel-bed rivers with stable banks , 2005 .

[10]  B. Eaton,et al.  Optimal alluvial channel width under a bank stability constraint , 2004 .

[11]  Howard H. Chang,et al.  Minimum energy as the general form of critical flow and maximum flow efficiency and for explaining variations in river channel pattern , 2004 .

[12]  G. Nanson,et al.  A stability criterion inherent in laws governing alluvial channel flow , 2002 .

[13]  Subhash C. Jain,et al.  Open-Channel Flow , 2000 .

[14]  R. Millar Influence of bank vegetation on alluvial channel patterns , 2000 .

[15]  G. Nanson,et al.  The influence of bank strength on channel geometry: an integrated analysis of some observations , 1998 .

[16]  R. Millar,et al.  Stable Width and Depth of Gravel-Bed Rivers with Cohesive Banks , 1998 .

[17]  G. Nanson,et al.  Vegetation and channel variation; a case study of four small streams in southeastern Australia , 1997 .

[18]  R. Warner,et al.  The multivariate controls of hydraulic geometry: A causal investigation in terms of boundary shear distribution , 1995 .

[19]  R. Millar,et al.  Effect of Bank Stability on Geometry of Gravel Rivers , 1993 .

[20]  G. Parker,et al.  Stable width and depth of straight gravel rivers with heterogeneous bed materials , 1988 .

[21]  C. Thorne,et al.  Stable Channels with Mobile Gravel Beds , 1986 .

[22]  Charles C. S. Song,et al.  Comment on “External Hypotheses for River Regime: An Illusion of Progress” by George A. Griffiths , 1986 .

[23]  R. Ferguson Hydraulics and hydraulic geometry , 1986 .

[24]  Howard H. Chang River Morphology and Thresholds , 1985 .

[25]  C. Yang Unit Stream Power Equation for Gravel , 1984 .

[26]  Howard H. Chang Comment on “Extremal hypotheses for river regime: An illusion of progress” by George A. Griffiths , 1984 .

[27]  E. Andrews Bed-material entrainment and hydraulic geometry of gravel-bed rivers in Colorado , 1984 .

[28]  Howard H. Chang Modeling of River Channel Changes , 1984 .

[29]  W. White,et al.  Analytical Approach to River Regime , 1982 .

[30]  Chih Ted Yang,et al.  Sediment Transport and Unit Stream Power Function , 1982 .

[31]  Charles C. S. Song,et al.  Hydraulic geometry and minimum rate of energy dissipation , 1981 .

[32]  Howard H. Chang Geometry of Gravel Streams , 1980 .

[33]  Howard H. Chang STABLE ALLUVIAL CANAL DESIGN , 1980 .

[34]  Charles C. S. Song,et al.  Theory of Minimum Rate of Energy Dissipation , 1979 .

[35]  Howard H. Chang Geometry of Rivers in Regime , 1979 .

[36]  Howard H. Chang Minimum stream power and river channel patterns , 1979 .

[37]  G. Parker Self-formed straight rivers with equilibrium banks and mobile bed. Part 1. The sand-silt river , 1978, Journal of Fluid Mechanics.

[38]  G. Parker Self-formed straight rivers with equilibrium banks and mobile bed. Part 2. The gravel river , 1978, Journal of Fluid Mechanics.

[39]  D. Rhodes The b-f-m Diagram for Downstream Hydraulic Geometry , 1978 .

[40]  Chih Ted Yang,et al.  Minimum Unit Stream Power and Fluvial Hydraulics , 1976 .

[41]  Chih Ted Yang,et al.  Unit Stream Power and Sediment Transport , 1972 .

[42]  S. Schumm,et al.  Experimental Study of Channel Patterns , 1971, Nature.

[43]  H. Einstein,et al.  The Bed-Load Function for Sediment Transportation in Open Channel Flows , 1950 .

[44]  R. Müller,et al.  Formulas for Bed-Load transport , 1948 .

[45]  J. H. Mackin CONCEPT OF THE GRADED RIVER , 1948 .

[46]  G. Nanson,et al.  Hydraulic geometry and maximum flow efficiency as products of the principle of least action , 2000 .

[47]  R. Millar An optimization model for the development and response of alluvial river channels , 1994 .

[48]  Stanley A. Schumm,et al.  Experimental fluvial geomorphology , 1987 .

[49]  Howard H. Chang Analysis of River Meanders , 1984 .

[50]  G. Griffiths Extremal Hypotheses for River Regime: An Illusion of Progress , 1984 .

[51]  Howard H. Chang Mathematical Model for Erodible Channels , 1982 .

[52]  Chih Ted Yang,et al.  Unit stream power equations for total load , 1979 .

[53]  S. Schumm The Fluvial System , 1977 .

[54]  Chih Ted Yang,et al.  Applicability of Unit Stream Power Equation , 1976 .

[55]  S. Schumm The shape of alluvial channels in relation to sediment type , 1960 .

[56]  L. B. Leopold,et al.  River channel patterns: Braided, meandering, and straight , 1957 .

[57]  E. W. Lane A study of the shape of channels formed by natural streams flowing in erodible material , 1957 .

[58]  E. W. Lane Design of Stable Channels , 1955 .

[59]  L. B. Leopold,et al.  The hydraulic geometry of stream channels and some physiographic implications , 1953 .

[60]  G Lacey,et al.  STABLE CHANNELS IN ALLUVIUM (INCLUDES APPENDICES). , 1930 .