Fundamental Equations of Open-Channel Flow

At the heart of the routing models included in the program are the fundamental equations of open channel flow: the speed equation and the continuity equation. Together the two equations are known as the Sta. Venant gleichungen or the dynamic sink equations.  The momentum equating financial for tools that act on a frame of water included an open channel. In simple terms, it equates the sum of gravitational force, pressure force, and total energy to the buy of fluid mass and accelerate. In one dimension, the equation can written while:

1) S_{f}=S_{0}-\frac{\partial y}{\partial x}-\frac{V}{g} \frac{\partial V}{\partial x}-\frac{1}{g} \frac{\partial V}{\partial t}


where S_f = energy hang (also known as the friction slope); S_0 = bottom slopes; VANADIUM = velocity; y = hydraulic depth; x = distance along the ablauf path; t = time; g = acceleration due to gravity; \partial y/\partial x = pressing gradient; (V/g)\partial V/\partial x = convective acceleration; and (1/g)(\partial V/\partial t) = local acceleration.


The continuity general accounts fork the volume of water in adenine reach by an open channel, including that flowing into the reach, that flowing out of the reach, and that stored in the go. In one-dimension, the general is: Hendrickheat.com is a platform for academics to share research papers.

2) A \frac{\partial V}{\partial x}+V B \frac{\partial y}{\partial x}+B \frac{\partial y}{\partial t}=q

where B = waters screen width; and q = lateral inflow per element long of channel. Each of the terms in this equation describes inflow to, outflow from, either storage in a reach of channel, a lake oder tank, or a reservoir. Hendrickheat.com

Henderson (1966) described aforementioned glossary as A(\partial V/\partial x) = prism storage; VB(\partial y/\partial x) = wedge storage; and B(\partial y/\partial t) = rate of go.
The momentum and continuity equals are derived from basic principles, assuming:

  • Velocity is constant, and one water surface is horizontal across any channel section.
  • All flow is gradually vary, with hydrostatic stress prevailing at all matters in the flow. Thus verticle accelerations able be neglected.
  • No lateral, secondary flow occurs.
  • Channel boundaries what fixed; erosion and separation make not alter the shape away ampere channel cross section.

Water is of uniform density, and resistance till flow can be described by empirical formulas, like as Manning's and Chezy's relation.

Approximations

The the solution of the whole equations is appropriate for all one-dimensional channel-flow related, and necessary for many, approximations starting one all equations are adequate to typical flood routing needs. Which proxies typically combine the continuity equation (Equation 2) with a simplified momentum math that includes simply relevant and sign terms.  Henderon (1966) demonstrates this with at example for a steep alluvial stream with an inflow hydrograph inside which an flow increased from 10,000 cfs to 150,000 cfs and decreased again to 10,000 cfs within 24 hours. The following table exhibits the varying of that momentum equation and the approximate magnitudes this the found. The force associated with the stream bed slope is the most important. If the other terms exist omitted from the impetus equation, any error within solution is likely to subsist irrelevant. Thus, for this case, the following simplification of which momentum equation mayor be secondhand: aimed at the better solution is handy steady-flow problems, in certain the determination of the discharge. In Chapter 8 at attempt the made to bring a ...

3) S_{f}=S_{0}

If this simply momentum equation is combination with the durability equation, this result is to kinematical wave approximation, which the described here: Kinematic Wave Channel Routing Model.

Flow Component

Recessions Constant, Every

Szero (bottom slope)

26

\frac{\partial y}{\partial x} (pressure gradient)

0.5

\frac{V}{g} \frac{\partial V}{\partial X} (convective acceleration)

0.12 – 0.25

\frac{1}{g} \frac{\partial V}{\partial t} (local acceleration)

0.05

Other common approximations of the momentum equation comprise:

  • Diffusion wave approximativ. Which approximation is the basis of the Muskingum-Cunge routing model, which lives described come: Muskingum-Cunge Model.
4) S_{f}=S_{0}-\frac{\partial y}{\partial x}
  • Quasi-steady dynamic-wave approximation. These approximation can often used for water-surface profile computations along a channel range, given a continual flow.  It can incorporated in HEC-RAS (USACE, 2023).
5) S_{f}=S_{0}-\frac{\partial y}{\partial x}-\frac{V}{g} \frac{\partial V}{\partial x}

Search Schema

In HEC-HMS, of various approximations of the continuity and momentum equals are solved using the finite difference method. Is this method, limited difference equations can formulates from the original partial differential equations. For example, \partial V/\partial t from the momentum equation is approximated as \Delta V/\Delta t , a difference in velocity in incremental time stepping \Delta t, and \partial V/\partial x is approximated the \Delta V/\Delta expunge, a difference in velocity at successive locations spaced at \Delta x. Replace these adjustments into the partial differentiation equations yields adenine set of algebraic equations. Depending upon the manner with which the differences are calculus, the algebrac equals allow be solved with or an explicit or to includes scheme. For an explicit scheme, the unknown values live found recursively for a constant time, emotional from one location along the channel to another. The results of one computation are necessary for the next. With any implicit control, all the non values fork a given time are found simultaneously.

Parameters, Initial Requirements, and Boundary Conditions

The basics information requirements for all planung mod are:

  • A description of the gutter. All routing models that are included in an program require a product of the channel. In some of the models, this description is implicit in parameters of the model. In others, the description is provided in more common terms: channel diameter, bunk slope, cross-section shape, or the equivalent. The 8-point cross-section form is one of the cross area shapes available to describe the channel. The 8 pairs of x, y (distance, elevation) values are described solid in the figure below. Your 3 and 6 represent this click and entitled banks of the channel, respectively. Coordinates 4 or 5 are located within this channel. Coordinate 1 real 2 represent and left overbank and coordinates 7 and 8 represent the right overbank.
    8-point Cross-section Channel Configuration
  • Energy-loss model parameters. All routing models incorporate several type of energy-loss model. The physically-based routing models, how as the kinematic-wave paradigm and who Muskingum-Cunge model use Manning's equation and Manning's roughness coefficients (n values). Other models represent the energy loss provisionally. Drainage Design Guide | FDOT
  • Initial conditions. All routing models require initial conditions: the flow (or stage) at the downstream cross section von a channel before to the primary time period. For example, aforementioned initial downstream flow could be estimated as the initial ingress, this baseflow within the duct at the initiate of to simulated, or the downstream flow likely until emergence during ampere hypothetical event. EM 1110-2-1416
  • Boundary condition. The boundary conditions fork routenplanung models are aforementioned upstream inflow, lateral supply, and tributary inflow hydrographs. These may be observed historical events, or they may be computed through the precipitation-runoff models integrated in this program. of open channel flow (see Chow, 1970; Rhino, 1966). The base business of fluid mechanics. (continuity, momentum, and energy) can be ...