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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.

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Earth Science & Geology

Wave Driven Sediment Transport Calculator

Calculate longshore sediment transport rates using the CERC formula. Estimate wave-driven sand movement, beach erosion potential, and coastal sediment budgets for engineering analysis.

Last updated: December 2025Reviewed by NovaCalculator Mathematics Team

Calculator

Adjust values & calculate
1.5 m
10ยฐ
8 s
2650
0.3 mm
0.02
Annual Longshore Transport
2,701,080 mยณ/yr
to the right (looking seaward)
Daily Transport
7400.2 mยณ/day
Energy Flux Component
2100.58 W/m
Breaking Depth
1.92 m
Profile Type
Dissipative (flat, wide surf zone)
Dean Number: 15.67
Erosion/Accretion
Bar Formation (Erosive)
Mass Transport Rate
4,294,718 tonnes/yr
Note: The CERC formula provides order-of-magnitude estimates. Actual transport rates depend on grain size distribution, beach profile, wave spectrum, and tidal effects not captured by this simplified approach.
Your Result
Transport: 2701080 m3/yr | to the right (looking seaward) | Dissipative (flat, wide surf zone)
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Understand the Math

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.

Last reviewed: December 2025

Worked Examples

Example 1: Moderate Wave Energy Beach

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 Longshore energy flux Pls = (1025*9.81*1.5^2*sqrt(9.81*1.5*0.78))/16 = 8,937 W/m Pls component = 8,937 * sin(2*10deg) = 8,937 * 0.342 = 3,058 W/m Q = 0.39 * 3,058 / ((2650-1025)*9.81*(1-0.4)) Q = 1,192.6 / 9,567 = 0.0001247 m3/s Annual = 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

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 Pls = (1025*9.81*9.0*sqrt(9.81*3.0*0.78))/16 = 34,220 W/m Pls component = 34,220 * sin(2*15deg) = 34,220 * 0.5 = 17,110 W/m Q = 0.39 * 17,110 / ((2650-1025)*9.81*0.6) Q = 6,672.9 / 9,567 = 0.000697 m3/s Daily = 0.000697 * 86400 = 60.3 m3/day
Result: Storm Transport: ~60 m3/day | ~22,000 m3/year if sustained | Highly erosive
Expert Insights

Background & Theory

The Wave Driven Sediment Transport Calculator applies the following established principles and formulas. Earth science calculators draw on a wide range of measurement scales and physical principles that quantify natural phenomena across geological, atmospheric, and hydrological systems. Earthquake magnitude is most precisely described by the Moment Magnitude Scale (Mw), which replaced the original Richter scale for larger events. Mw is calculated as Mw = (2/3) log10(M0) โˆ’ 10.7, where M0 is the seismic moment in dyne-centimeters. The Richter scale, while still referenced colloquially, is a local magnitude (ML) measurement derived from peak seismograph amplitude at a standard 100 km distance. Wind intensity is classified using the Beaufort Scale, a 13-point empirical scale (0โ€“12) relating wind speed in knots to observable sea and land effects, with Beaufort 12 corresponding to hurricane-force winds above 64 knots. Tropical cyclone intensity is further categorized by the Saffir-Simpson Hurricane Wind Scale, which assigns Categories 1 through 5 based on sustained wind speed, correlating with expected structural damage. Mineral hardness is quantified on the Mohs scale (1โ€“10), comparing scratch resistance relative to reference minerals from talc (1) to diamond (10). Soil composition analysis measures the proportions of sand, silt, and clay by particle size, alongside organic matter content, bulk density, and porosity, which together determine engineering and agricultural suitability. Seismic wave velocity in rock varies by material: P-waves travel at approximately 5โ€“7 km/s in granite and 1.5 km/s in water, while S-waves travel at roughly 60% of P-wave speeds. Atmospheric pressure decreases with altitude according to the barometric formula: P = P0 ร— exp(โˆ’Mgh / RT), where M is molar mass of air, g is gravitational acceleration, h is altitude, R is the universal gas constant, and T is temperature in Kelvin. Standard sea-level pressure is 101,325 Pa. Tidal calculations use harmonic analysis of gravitational forcing by the Moon and Sun, with the principal lunar semidiurnal tidal constituent (M2) having a period of approximately 12.42 hours.

History

The history behind the Wave Driven Sediment Transport Calculator traces back through the following developments. The systematic study of Earth's structure and processes spans millennia, but the scientific foundations were laid in the seventeenth century. In 1669, Danish naturalist Nicolas Steno published his principles of stratigraphy, establishing the laws of superposition, original horizontality, and lateral continuity โ€” foundational rules for reading rock layers that remain in use today. Scottish geologist James Hutton introduced the concept of uniformitarianism in 1788, proposing that geological processes observable in the present have operated throughout Earth's history at broadly consistent rates. This idea of deep time challenged prevailing biblical chronologies and set the stage for modern geology. Charles Lyell systematized these ideas in his landmark three-volume work Principles of Geology, published beginning in 1830, which directly influenced Charles Darwin's thinking on biological evolution during the voyage of the Beagle. The nineteenth century saw growing curiosity about continental shapes, but a coherent theory awaited Alfred Wegener, a German meteorologist who proposed continental drift in 1912, arguing that the continents had once formed a supercontinent he called Pangaea. His evidence included matching fossil records and geological formations across the Atlantic, but his mechanism was disputed for decades. The theory gained acceptance in the 1960s when seafloor spreading was confirmed through paleomagnetic studies, and plate tectonics emerged as the unifying framework of modern geoscience. The United States Geological Survey was established by Congress in 1879 to classify public lands and examine the geological structure, mineral resources, and products of the national domain. The twentieth century brought instrumental advances, including the global seismograph network deployed after World War II, initially to monitor nuclear tests, which dramatically improved earthquake detection and characterization. Satellite Earth observation began in earnest with the Landsat program launched in 1972, enabling continuous global monitoring of land use, glacier retreat, and vegetation patterns. Today, GPS networks, LIDAR scanning, and ocean-floor mapping provide centimeter-scale precision for tracking tectonic motion, sea level rise, and volcanic deformation in near real time.

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Frequently Asked Questions

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.
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.
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.
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.
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.
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.
Educational Note: This calculator is provided for educational and informational purposes. Results are based on the formulas and inputs provided. Always verify important calculations independently. NovaCalculator processes calculator inputs client-side; optional analytics follow visitor consent settings.Reviewed by: NovaCalculator Mathematics Team โ€” Verified against standard mathematical and scientific references. Last reviewed: December 2025. ยฉ 2024โ€“2026 NovaCalculator.

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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.

References

Reviewed by Daniel Agrici, Founder & Lead Developer ยท Editorial policy