🌊 Earth Science · Wave Physics
📅 Березень 2026⏱ 11 min🟡 Середній

Tsunami Physics: From Seafloor to Shore

In the open ocean, a tsunami is barely noticeable — 1 metre high, travelling at 800 km/h, with wavelengths of 200 km. Hours later, as it enters shallow water, it slows to 50 km/h and piles up to 30 metres. The physics of this transformation is governed by a single elegant formula.

1. Generation Mechanisms

Tsunamis are generated by any sudden large-scale displacement of a water body:

2. Shallow-Water Wave Theory

A wave is "shallow-water" when its wavelength λ ≫ water depth h (specifically, h < λ/20). For tsunamis:

Shallow-water wave speed: c = √(g · h) g = 9.81 m/s² h = water depth (m) Average Pacific depth = 4,000 m: c = √(9.81 × 4,000) = √39,240 ≈ 198 m/s ≈ 713 km/h Deep ocean trench (Mariana, h = 11,000 m): c = √(9.81 × 11,000) ≈ 1,039 km/h Why tsunamis are "shallow-water" waves: Ocean depth ≈ 4 km Tsunami wavelength ≈ 200 km h/λ ≈ 4/200 = 0.02 << 1/20 ✓ (firmly in shallow-water regime) Compare to wind waves: Ocean swell depth ≈ 4 km, wavelength ≈ 100 m h/λ ≈ 40 >> 1 (deep-water regime) c = √(gλ/2π) — very different physics

3. Ocean Propagation

Because c = √(gh), tsunamis slow down in shallower water and speed up over deeper water. This creates refraction — the wavefront bends to follow depth contours, much like light bending in optics.

Key features of open-ocean propagation:

4. Shoaling & Amplification

As the tsunami approaches shore and depth decreases, it slows dramatically. Energy is conserved, so decreasing wave speed must be compensated by increasing amplitude — wave shoaling:

Green's law for shoaling amplification: H₂/H₁ = (h₁/h₂)^(1/4) H = wave height, h = water depth From ocean (h₁=4,000m, H₁=1m) to nearshore (h₂=10m): H₂ = 1 × (4000/10)^(1/4) = 1 × (400)^0.25 = 1 × 4.47 ≈ 4.5 m Beyond this, nonlinear effects and friction further modify run-up. Real amplification can be much greater due to coastal geometry: V-shaped bays concentrate wave energy 2011 Tōhoku: deep bays amplified waves to 40+ m in some locations
The "drawback" effect: Before a tsunami arrives, the sea often recedes dramatically — a leading depression wave drawing water offshore. In 2004, this visible drawback (the sea retreating hundreds of metres) occurred minutes before the wave struck, giving crucial but brief warning to those who recognised the sign. Many people walked toward the exposed seafloor in curiosity rather than running to high ground.

5. Run-Up & Inundation

Run-up height R (measured above sea level at the furthest inland reach) is what determines destruction. It is not simply the wave height — it depends strongly on coastal bathymetry, topography, and wavelength.

Maximum run-up (nonlinear shallow-water, sloped beach): R / H ≈ 2.831 × (H/λ)^(-1/2) × tan(slope)^(-1/2) Notable historical run-ups: 2004 Indian Ocean: max 30+ m (Sumatra), average 5-8 m 2011 Tōhoku: max 40.1 m (Miyako, Japan), average 10-15 m 1958 Lituya Bay: 524 m (megatsunami from rockfall) 1883 Krakatoa: 35 m (volcanic caldera collapse) Inundation modelling uses: • Non-linear shallow-water equations (NSWW/MOST model) • Depth-averaged, finite-difference solvers • Validated with tide gauge and field survey data • GEBCO bathymetry (1-arc-minute resolution globally)

6. Detection & Early Warning

The Pacific Tsunami Warning Center (PTWC) and NOAA's DART (Deep-ocean Assessment and Reporting of Tsunamis) buoy network provide the primary warning infrastructure:

7. Mitigation Engineering