Wave Driven Sediment Transport Calculator
Free Wave driven sediment transport Calculator for oceanography & coastal science. Enter variables to compute results with formulas and detailed steps.
Formula
Q = K * Pls * sin(2*alpha_b) / ((rho_s - rho_w) * g * (1-p))
Where Q is the volumetric transport rate (m3/s), K is the empirical coefficient (0.39), Pls is the wave energy flux at breaking, alpha_b is the breaking wave angle, rho_s and rho_w are sediment and water densities, g is gravity, and p is sediment porosity.
Worked Examples
Example 1: Moderate Wave Energy Beach
Problem: Breaking waves with Hb = 1.5 m arrive at 10 degrees to a sandy beach with 8-second period. Sand density is 2650 kg/m3, grain size 0.3 mm. Calculate the annual longshore transport rate.
Solution: Breaking depth = 1.5/0.78 = 1.92 m\nLongshore energy flux Pls = (1025*9.81*1.5^2*sqrt(9.81*1.5*0.78))/16 = 8,937 W/m\nPls component = 8,937 * sin(2*10deg) = 8,937 * 0.342 = 3,058 W/m\nQ = 0.39 * 3,058 / ((2650-1025)*9.81*(1-0.4))\nQ = 1,192.6 / 9,567 = 0.0001247 m3/s\nAnnual = 0.0001247 * 86400 * 365 = 3,932 m3/year
Result: Longshore Transport: ~3,932 m3/year | ~10.8 m3/day | Bar formation expected
Example 2: High Energy Exposed Coast
Problem: Storm waves break at 3 m height with a 15-degree angle on an exposed coast. Calculate the sediment transport rate during the storm event.
Solution: Breaking depth = 3.0/0.78 = 3.85 m\nPls = (1025*9.81*9.0*sqrt(9.81*3.0*0.78))/16 = 34,220 W/m\nPls component = 34,220 * sin(2*15deg) = 34,220 * 0.5 = 17,110 W/m\nQ = 0.39 * 17,110 / ((2650-1025)*9.81*0.6)\nQ = 6,672.9 / 9,567 = 0.000697 m3/s\nDaily = 0.000697 * 86400 = 60.3 m3/day
Result: Storm Transport: ~60 m3/day | ~22,000 m3/year if sustained | Highly erosive
Frequently Asked Questions
What is longshore sediment transport and what drives it?
Longshore sediment transport, also called littoral drift, is the movement of sediment parallel to the shoreline within the surf zone, driven primarily by wave-induced currents. When waves break at an oblique angle to the shoreline, they generate a longshore current that flows parallel to the beach in the direction of wave propagation. This current, combined with the orbital motion of breaking waves that suspends sediment from the bed, transports sand along the coast. The volume of sediment transported depends strongly on wave height (proportional to Hb raised to the 2.5 power) and the breaking wave angle. Longshore transport rates vary enormously from near zero on protected coasts to over one million cubic meters per year along energetic exposed coastlines. Understanding and predicting longshore transport is critical for coastal engineering.
How does breaking wave angle affect sediment transport rates?
The breaking wave angle has a critical influence on longshore sediment transport through the sin(2*alpha) term in the CERC formula. Maximum longshore transport occurs when waves break at 45 degrees to the shoreline because sin(2*45) equals 1.0. At breaking angles near zero (waves parallel to shore) or 90 degrees (waves perpendicular to shore), the longshore transport approaches zero. In practice, most waves break at relatively small angles of 5 to 15 degrees because wave refraction turns waves nearly parallel to the shore before they break. Even small changes in breaking angle at these low values cause significant changes in transport rate because the sin(2*alpha) function is steep near zero. This sensitivity means that accurate measurement or prediction of the breaking wave angle is essential for reliable sediment transport calculations.
What is the difference between gross and net longshore transport?
Gross longshore transport is the total volume of sediment moved in both directions along the beach over a specified period, while net transport is the difference between the volumes moved in each direction. On most coastlines, waves approach from different directions at different times, driving sediment transport alternately to the left and right. The net transport, which determines long-term shoreline evolution, is often much smaller than the gross transport. For example, a beach might have a gross transport of 500,000 cubic meters per year with 300,000 moving to the right and 200,000 to the left, giving a net transport of only 100,000 cubic meters per year to the right. Coastal structures like groins and jetties interrupt net transport, causing sediment accumulation on the updrift side and erosion on the downdrift side.
How do coastal structures affect sediment transport patterns?
Coastal structures dramatically alter sediment transport patterns by blocking, redirecting, or modifying wave-driven currents. Groins, constructed perpendicular to the shoreline, trap sediment on the updrift side and cause erosion on the downdrift side by interrupting the longshore transport pathway. Jetties at harbor entrances have similar effects but on a larger scale, often creating wide beaches updrift and severe erosion downdrift. Breakwaters reduce wave energy in their lee, creating a zone of reduced longshore transport that causes sediment deposition in the sheltered area. Seawalls and revetments do not directly affect longshore transport but can increase wave reflection and turbulence at their base, potentially enhancing cross-shore sediment loss. The unintended downdrift erosion caused by structures has led to costly litigation and mitigation requirements.
What role does grain size play in sediment transport?
Grain size significantly affects sediment transport rates though the basic CERC formula does not explicitly include it. Finer sediments are more easily entrained and transported because they have lower settling velocities and require less wave energy to be suspended. Coarser sediments like gravel and cobbles require much larger waves to be mobilized and are transported primarily as bedload rather than suspended load. The Kamphuis formula, an alternative to CERC, explicitly includes grain size and generally provides better predictions across different sediment types. Grain size also determines the equilibrium beach profile shape, with coarser sediments producing steeper beach faces. In practice, beaches with mixed grain sizes exhibit selective transport where finer material is preferentially moved, leading to spatial sorting of sediment and variable beach characteristics along the coast.
What is cross-shore sediment transport and how does it differ from longshore?
Cross-shore sediment transport moves sediment perpendicular to the shoreline, either onshore or offshore, and is driven by different mechanisms than longshore transport. During storms, large breaking waves generate strong offshore-directed undertow currents that carry suspended sediment seaward, creating offshore bars and eroding the beach face. During calm conditions, smaller non-breaking waves transport sediment shoreward through asymmetric orbital velocities, rebuilding the beach berm. The Dean number relates wave height, sediment fall velocity, and wave period to predict whether conditions are erosive or accretive. Cross-shore transport is typically more variable than longshore transport, with dramatic beach changes possible during a single storm event. Understanding the balance between cross-shore and longshore transport is essential for predicting overall beach behavior.