# Rayleigh-Taylor Instability

We consider the classic Rayleigh-Taylor instability problem which consists of a heavy fluid resting on top of a light fluid in a gravitational field supported by a counterbalancing pressure gradient.

## 2D Lagrangian Results Using Q1-Q0, Q2-Q1, Q4-Q3 and Q8-Q7 Finite Elements

Results for density and curvilinear mesh in the Rayleigh-Taylor problem using Q1-Q0 finite elements at times t = 3, 4, 4.5 and 5.

## 2D Lagrangian Late Time Results Using Q8-Q7 Finite Elements

Comparing an ALE-AMR simulation (left) to a purely Lagrangian simulation with Q8-Q7 finite elements (center) for the Rayleigh-Taylor instability problem at time t = 5.6625. A zoomed in view of the Q8-Q7 Lagrangian mesh (right) reveals the extreme mesh distortion. High-order Lagrangian methods are capable of handling extreme mesh distortion due to complex vortical flow.

Results for 2D Lagrangian, ALE and Eulerian (ALE in the Eulerian limit) simulations with Q4-Q3 finite elements for the Rayleigh-Taylor instability problem at time t = 4.5. *High-order ALE methods are robust with respect to mesh motion*.

Lagrangian

Eulerian

## Multi-Mode High Resolution 2D Eulerian Results Using Q4-Q3 Finite Elements

Results for density in the multi-mode Rayleigh-Taylor problem using Q4-Q3 finite elements on a 256 by 512 zone mesh at times t = 1.5, 3 and 5.25 (left to right). Initial velocity perturbation is based on a randomized multi-mode expansion using six modes. Problem run on 256 processors for 65,051 cycles with a wall time of ~10 hours.

## High-order Simulation on 2-Element Mesh (12th Order Elements)

High-order geometry and field representation allow modelling of the smooth version of this problem on extremely coarse meshes, in this case consisting of two 12th order elements. Note the developing element curvature and the sharp transition of the density at the material interface.