Flow and Velocity Distribution in Meandering Compound Channels Kanhu Charan Patra 1 ; Srijib K. Kar 2 ; and Amartya K. Bhattacharya, A.M.ASCE 3 Abstract: An investigation of flow and velocity distribution in meandering compound channels with over bank flow is described. Equations concerning the three-dimensional variation of longitudinal, transverse, and vertical velocity in the main channel and floodplain of compound section in terms of channel parameters are presented. The flow and velocity distributions in meandering compound channels are strongly governed by interaction between flow in the main channel and that in the floodplain. The proposed equations take adequate care of the interaction affect. Results from the formulations, simulating the three-dimensional velocity field in the main channel and in the floodplain of meandering compound channels are compared with their respective experimental channel data obtained from a series of symmetrical and unsymmetrical test channels with smooth and rough sections. The aspect ratio of the test channels varies from two to five. The equations are found to be in good agreement with the experimental data. The formulations are verified against the natural river and other meandering compound channel data. The power laws used for simulating the three-dimensional velocity structure are found to be quite adequate. DOI: 10.1061/ASCE0733-94292004130:5398 CE Database subject headings: Meanders; Flood plains; Velocity distribution; Flow distribution; Channels, waterways. Introduction A river is the author of its own geometry. It is an established fact that meandering represents a degree of adjustment of water and sediment laden river with its size, shape, and slope such that a flatter channel can exist in a steeper valley. By nature or by de- sign, rivers have compound sections consisting of a main channel, which always carry low flows and one or more side floodplains, which carry flow above the bank full stages. Once a river stage overtops the banks, the cross sectional geometry of flow under- goes a steep change, a situation common to most of the natural or man-made channels. The flow structure in a compound channel is characterized by large shear layers generated by the difference of velocity between the main channel and the floodplain flow. There is also a wide variation in the distribution of longitudinal velocity from the inner to the outer bank of a meandering compound chan- nel section. Due to the continuous streamwise variation of radius of curvature, the flow parameters are considerably more complex in a meandering channel than in a straight channel. The flow geometry in a meandering channel is in the state of either devel- opment or decay or both. Distribution of flow and velocity in a meandering river are important topics in river hydraulics to be investigated from a practical point of view in relation to the bank protection, naviga- tion, water intakes, and sediment transport-depositional patterns. Knowledge on velocity distribution in a channel also helps to determine the energy expenditure, bed shear stress distribution, and the associated heat and mass transport problems. An attempt is made here for an analytical solution of a three-dimensional flow structure in meandering compound channel to get a complete picture of velocity distribution at any section of a meandering path. More efforts have been made to model the distribution of flow between the main channel and floodplain of a meandering compound channel. The usual practice in one-dimensional 1Danalysis of com- pound channel is to calculate separately the flow that can be con- veyed by the various discrete subareas of a compound section as if the subareas are independent. For each subarea, either a Man- ning or Darcy-Weisbach equation is used to calculate the convey- ance capacity using appropriate values for the area, wetted perim- eter, and roughness coefficients of the subareas. The individual discharges are then added to give the total discharge carried by the compound section. The roughness coefficient n or f is a some- what crude measure of the net effect of the influences of the shear and the secondary flow, wherein all the hydraulic effects are lumped into a simple bulk resistance parameter. Using ‘‘divided channel’’ method of Lotter 1933and following the work of Wormleaton, Allen, and Hadjipanos 1982, Knight and Dem- etriou 1983, and Knight and Hamed 1984for straight chan- nels, Patra and Kar 2000proposed a variable interface plane of separation of compound channel for a better estimate of discharge in meandering and straight compound river sections. The percent- ages of total flow carried by the main channel and floodplain of a compound section in terms of four dimensionless channel param- eters were suitably modeled. The effect of flow interaction be- tween the floodplain and main channel for various depths of flow over floodplain was adequately taken care of. 1 Associate Professor, Civil Engineering Dept., College of Engineering and Technology, Orissa Univ. of Agricultural and Technology, Bhubaneswar, Orissa, India—751 003. 2 Professor, Civil Engineering Dept., Indian Institute of Technology, Kharagpur, India—721302. E-mail: skkar@civiliitkgp.ernet.in 3 Lecturer, Applied Mechanics Dept., B.E. Coll. Deemed Univ., Howrah, W.B. India. Note. Discussion open until October 1, 2004. Separate discussions must be submitted for individual papers. To extend the closing date by one month, a written request must be filed with the ASCE Managing Editor. The manuscript for this paper was submitted for review and pos- sible publication on May 23, 2000; approved on February 25, 2003 . This paper is part of the Journal of Hydraulic Engineering, Vol. 130, No. 5, May 1, 2004. ©ASCE, ISSN 0733-9429/2004/5-398 – 411/$18.00. 398 / JOURNAL OF HYDRAULIC ENGINEERING © ASCE / MAY 2004