PhysSandbox
Classical MechanicsWaves & SoundElectricity & MagnetismOptics & LightGravity & OrbitsLabs
🌙Astronomy & The Sky🌡️Thermodynamics🌍Biophysics, Fluids & Geoscience📐Math Visualization🔧Engineering🧪Chemistry

More from Biophysics, Fluids & Geoscience

Other simulators in this category — or see all 19.

View category →
NewUniversity / research

Ekman Spiral in the Ocean

Wind stress, Coriolis f, eddy viscosity A_z: classical Ekman spiral of horizontal velocity with depth; deflection angle.

Launch Simulator
NewUniversity / research

Hodgkin–Huxley Action Potential

Squid-axon HH ODEs: membrane voltage V(t) and gating (m, h, n); step stimulus and Na⁺/K⁺ conductance traces.

Launch Simulator
NewUniversity / research

Cable Equation on an Axon

1D passive cable ∂V/∂t = D∂²V/∂x² − (V−V_r)/τ + I; compare uniform fiber vs myelinated (higher D in internodes).

Launch Simulator
NewSchool

Coupled FitzHugh–Nagumo Neurons

Two excitable FHN units with diffusive coupling: phase plots, time traces, and synchronization vs coupling strength.

Launch Simulator
NewSchool

Nernst Potentials & Membrane

Nernst E for K⁺ and Na⁺ from inside/outside concentrations; optional Goldman–Hodgkin–Katz resting estimate.

Launch Simulator
NewUniversity / research

Kelvin–Helmholtz Shear Instability

Two parallel flows with slip U: Fourier-mode growth rate sketch and animated interface billows (linear toy model).

Launch Simulator
PhysSandbox

Interactive physics, chemistry, and engineering simulators for students, teachers, and curious minds.

Physics

  • Classical Mechanics
  • Waves & Sound
  • Electricity & Magnetism

Science

  • Optics & Light
  • Gravity & Orbits
  • Astronomy & The Sky

More

  • Thermodynamics
  • Biophysics, Fluids & Geoscience
  • Math Visualization
  • Engineering
  • Chemistry

© 2026 PhysSandbox. Free interactive science simulators.

PrivacyTermsContact
Home/Biophysics, Fluids & Geoscience/River Meandering (Toy)

River Meandering (Toy)

Natural river meanders arise from feedbacks among flow, sediment transport, and erodible banks — often summarized in reduced models (e.g. Ikeda–Parker–Sawai) where bend curvature and its streamwise gradient steer lateral migration. This page collapses that story to a pinned-end centerline y(x,t) on a fixed downstream reach: curvature κ is approximated by ∂²y/∂x² (gentle slopes), streamwise curvature gradient by ∂κ/∂x, and a toy evolution ∂y/∂t = k₁ ∂κ/∂s + λ ∂²y/∂x² with ∂κ/∂s ≈ ∂κ/∂x. Parameters are chosen for visible bend growth and numerical stability, not field calibration.

Who it's for: Introductory geomorphology or PDE-motivation labs after basic derivatives.

Key terms

  • Meander
  • Curvature
  • Centerline migration
  • Semi-empirical model
  • Numerical diffusion

Real meanders couple hydraulics, sediment, banks, and floodplain memory; this page keeps a single semi-empirical PDE-like rule so the “k₁ ∂c/∂s” bend-talk from notes becomes a visible curve.

Live graphs

Toy bend law

0.022
0.11
1.6
0.14

Centerline y(x,t) on a fixed reach with pinned ends. Curvature κ ≈ ∂²y/∂x² (small-slope); toy law ∂y/∂t = k₁ ∂κ/∂s + λ ∂²y/∂x² with ∂κ/∂s ≈ ∂κ/∂x — a schematic bend migration, not a full Ikeda–Parker bar model.

Measured values

Model time (arb.)0.00
max |y| (norm.)0.1394
max |κ| (norm.)15.474

How it works

Pinned-end centerline of a river reach: curvature κ drives lateral migration via a gradient term k₁ ∂κ/∂s plus smoothing — a classroom cartoon of why bends can sharpen and propagate along valley floors.

Key equations

κ ≈ ∂²y/∂x²; ∂y/∂t = k₁ ∂κ/∂s + λ ∂²y/∂x² (with ∂κ/∂s ≈ ∂κ/∂x here).

Frequently asked questions

Does this include bars, width variation, or floodplain stratigraphy?
No. It is a single-line cartoon with smoothing λ to mimic unresolved subgrid dissipation; there is no cross-section, no Exner bed update, and no bank-height physics.
Why pin y=0 at both ends?
It fixes the reach length and prevents rigid translation of the whole thread, making relative bend growth easier to see in a small canvas.