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Case Study

High-Fidelity 3D Multiphase Acoustics

Simulating Acoustic Wave Propagation Through Dense Bubble Clouds

Some of the hardest flow problems to test in the lab are the ones that mix acoustics, liquids, and thousands of tiny gas bubbles. With NumericalAI, you can run these scenarios directly in the browser and see how an incoming pressure wave travels through, scatters, and interacts with a dense bubble cloud.

The visualization below shows a 3D bubble screen inside water — every blue shape is a tracked bubble responding to the acoustic pulse. This is the kind of detail that helps teams design quieter systems, better dampers, and more efficient underwater or medical devices.

3D Lagrange Bubble Screen Simulation

Figure 1: 3D view of bubble cloud exposed to an acoustic source — void fraction distribution at t = 0.33s

The visualization shows the spatial distribution of gas volume fraction, with individual bubbles tracked using a Lagrangian approach while the surrounding liquid flow is captured with Eulerian methods.


Simulation Overview

Domain Configuration

Domain Size:

0.5m × 0.3m × 0.3m

Grid Resolution:

200 × 120 × 120 cells

Total Cells:

2.88 million

Bubble Count:

~3,500 bubbles

Physical Parameters

Fluid:

Water (ρ = 998 kg/m³)

Gas:

Air (ρ = 1.2 kg/m³)

Bubble Diameter:

2-5 mm

Acoustic Frequency:

5 kHz

Temporal Settings

Simulation Time:

0.5 seconds

Time Step:

5 × 10⁻⁶ s

Total Steps:

100,000

CFL Number:

0.3

Computational Cost

Wall-clock Time (estimated):

~16min

GPU Used:

NVIDIA A100

Memory Usage:

~37 GB

Speedup vs 1 CPU:

~36×


Technical Approach

Hybrid Eulerian-Lagrangian Framework

This simulation employs a sophisticated two-way coupled approach that captures the best of both worlds:

  • Eulerian Phase (Continuous Liquid)

    The water phase is solved on a fixed Cartesian grid using compressible Navier-Stokes equations with acoustic wave propagation. A high-order WENO scheme captures sharp pressure gradients.

  • Lagrangian Phase (Dispersed Bubbles)

    Each bubble is tracked as a discrete particle with 6-DOF dynamics. The Rayleigh-Plesset equation governs radial oscillations in response to local pressure changes, while drag, lift, and added-mass forces determine translational motion.

  • Two-Way Coupling

    Bubbles receive pressure and velocity information from the Eulerian grid, while their volume and momentum are projected back onto the grid using a particle-source-in-cell (PSI-Cell) method. This bidirectional exchange captures realistic wave scattering and attenuation.

Acoustic Source Modeling

A planar acoustic source is positioned at x = 0, emitting a sinusoidal pressure wave with amplitude of 50 kPa and frequency of 5 kHz. The source uses a soft-start ramp over 3 cycles to avoid spurious numerical oscillations. The bubble screen is positioned 0.15m downstream, creating a dense scattering region with void fractions up to 15%.

Boundary Conditions

Inlet (x = 0):

Prescribed pressure wave

Outlet (x = 0.5m):

Non-reflecting boundary

Lateral (y, z):

Periodic boundaries

Bubble Surface:

Free-slip, compressible interface


Key Results & Findings

Acoustic Attenuation Performance

The bubble screen achieved a 23 dB reduction in transmitted acoustic energy at 5 kHz, with peak attenuation occurring at the bubble resonance frequency (~4.8 kHz for 3mm diameter bubbles).

23 dB

Sound Reduction

~65%

Energy Dissipated

4.8 kHz

Peak Frequency

Bubble Dynamics Observations

  • Radial Oscillations: Bubbles near resonance exhibited volume changes up to 35%, significantly enhancing scattering efficiency

  • Collective Effects: Dense packing (void fraction 15%) created cooperative oscillations that amplified attenuation by ~30% compared to isolated bubbles

  • Bubble Drift: Acoustic radiation pressure caused net bubble displacement of ~2cm downstream over the 0.5s simulation


What NumericalAI Delivers for This Problem

  • Full 3D resolution — capture spatial wave patterns and bubble distribution effects impossible in 2D

  • Individual bubble tracking — thousands of bubbles with independent dynamics, not statistical averaging

  • Time-accurate acoustics — resolve wave propagation with microsecond precision for frequency-dependent studies

  • GPU-accelerated solve — 45× faster than CPU, turning multi-day simulations into same-day results

  • Cloud execution — no local HPC infrastructure needed, run from anywhere with a web browser

Industrial Applications

Marine & Underwater Defense

Design and optimize bubble curtain systems for acoustic signature control in submarines, surface vessels, and sonar countermeasures. Predict attenuation performance across frequency bands without expensive sea trials.

Energy & Process Engineering

Understand cavitation damage in pumps and turbines, design gas-liquid contactors with acoustic monitoring, and optimize bubble column reactors. Prevent equipment failure through predictive multiphase flow modeling.

Medical Ultrasound & Therapy

Model ultrasound contrast agents, focused ultrasound surgery (FUS) with microbubbles, and cavitation-enhanced drug delivery. Virtual testing accelerates device development and treatment planning.

Research & Development

Explore fundamental physics of bubble-acoustic interactions, validate reduced-order models, and develop new attenuation concepts. High-fidelity data generation for AI/ML training datasets.

Business Value

NumericalAI turns what used to be a specialist, HPC-only workflow into a repeatable SaaS experience: upload the setup, run, visualize, and share — all without installing a solver or maintaining a cluster.

ROI Impact: Reduce physical prototyping by 60%, accelerate design cycles from months to weeks, and eliminate capital expenses on local HPC infrastructure. One simulation replaces dozens of expensive lab tests.

Ready to Solve Your Multiphase Acoustics Problems?

Start your own high-fidelity simulation on NumericalAI's cloud platform. No installation, no infrastructure management — just results.

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