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Sediment transport and tractive force approach

Short answer

Sediment transport occurs as bed and suspended load; stability requires tractive force τ = γRS to stay below critical shear from Shields criterion. Design computes permissible depth from bed (τb = γDS) and side (τs = 0.75γDS) conditions, then finds width via Manning's equation. Suitable for coarse non-cohesive material with little sediment inflow.

Explain sediment transport and tractive force approach in canal design.

Sediment transport in canals

Sediment moves as bed load (rolling, sliding, saltating along the bed) and suspended load (carried up by turbulence). If flow is too slow, sediment settles (silting, loss of capacity); if too fast, it scours the bed and banks. A canal is stable when neither occurs. The movement starts when the tractive force (shear stress) on the bed exceeds the critical value for the particles.

Tractive force approach

Tractive force is the drag of flowing water on the wetted perimeter per unit area:

τ0=γRS\tau_0 = \gamma R S

For a wide channel R≈DR \approx D:

  • Maximum on the bed: τb=γDS\tau_b = \gamma D S (about 0.97γDS0.97\gamma DS).
  • Maximum on the sides: τs=0.75γDS\tau_s = 0.75\gamma D S.

Critical (permissible) shear for non-cohesive soil comes from Shields' criterion:

τc=θc(γs−γ)d,θc≈0.047\tau_c = \theta_c(\gamma_s - \gamma)d,\qquad \theta_c \approx 0.047

or from tables/charts (Lane) for the soil type.

Side slope stability

A particle on a slope θ\theta (angle with horizontal) with angle of repose ϕ\phi resists a smaller shear than on the bed:

K=τc,sideτc,bed=cos⁡θ1−tan⁡2θtan⁡2ϕ=1−sin⁡2θsin⁡2ϕK = \frac{\tau_{c,\text{side}}}{\tau_{c,\text{bed}}} = \cos\theta\sqrt{1 - \frac{\tan^2\theta}{\tan^2\phi}} = \sqrt{1 - \frac{\sin^2\theta}{\sin^2\phi}}

Design steps

  1. Obtain QQ, SS, soil data (dd, ϕ\phi), nn and side slope zz.
  2. Compute permissible τc\tau_c for bed and KτcK\tau_c for side.
  3. Bed condition: γDS≤τc⇒D≤τcγS\gamma D S \le \tau_c \Rightarrow D \le \dfrac{\tau_c}{\gamma S}. Side condition: 0.75γDS≤Kτc⇒D≤Kτc0.75γS0.75\gamma DS \le K\tau_c \Rightarrow D \le \dfrac{K\tau_c}{0.75\gamma S}. The smaller DD governs.
  4. Using that DD, find BB from Manning's equation so that the section carries QQ.
  5. Check the actual stresses on bed and side against the permissible values and adjust if necessary.

Merits and limits

The approach is rational for canals in coarse, non-cohesive material (stable channels) where there is little sediment inflow, whereas regime theories (Kennedy/Lacey) suit alluvial canals that carry silt. It needs reliable soil data and does not consider the sediment inflow.

✓ Answer checked by Claude Opus 5.5 (high effort)

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