๐ฟ Spray & Droplet Atomization
Calculate Sauter Mean Diameter (SMD, D32), liquid jet breakup regimes (Rayleigh, Wind-Induced, Atomization), spray cone angle, Rosin-Rammler droplet distribution, Weber and Ohnesorge numbers.
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Double Precision (IEEE 754)
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Released
Aug 2026
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๐ฟ Spray Jet & Droplet Atomization Dynamics
Real-time particle & wave breakup simulation๐ Configuration & Presets
Key Formulations:
โข Velocity: Vinj = Cd โ(2ฮP/ฯL)
โข Sauter Mean Diameter: D32 = 2.25 ฯ0.25 ฮผL0.16 ฯL0.20 mฬ0.22 ฮPโ0.43
โข Weber Number: Weg = ฯg Vinjยฒ d0 / ฯ
โข Ohnesorge Number: Oh = ฮผL / โ(ฯL ฯ d0)
โข Velocity: Vinj = Cd โ(2ฮP/ฯL)
โข Sauter Mean Diameter: D32 = 2.25 ฯ0.25 ฮผL0.16 ฯL0.20 mฬ0.22 ฮPโ0.43
โข Weber Number: Weg = ฯg Vinjยฒ d0 / ฯ
โข Ohnesorge Number: Oh = ฮผL / โ(ฯL ฯ d0)
๐ Atomization & Spray Results
Configure inputs and click Calculate to view results.
๐ Calculation Methodology & Engineering Theory
Breakup Regimes & Ohnesorge Diagram
The transition from a continuous liquid column to finely dispersed droplets is governed by the competing forces of inertia, surface tension, viscous shear, and aerodynamic drag:
- Rayleigh Regime (Oh < 0.1, WeL < 10): Capillary instabilities pinch off droplets larger than the nozzle.
- First & Second Wind-Induced: Aerodynamic interaction with surrounding gas causes surface wave shearing.
- Catastrophic Atomization (Weg > 40): Instantaneous chaotic stripping of ligaments into micro-droplets.
Sauter Mean Diameter (D32)
The Sauter Mean Diameter represents the ratio of droplet volume to surface area, critical for mass transfer, evaporation, and combustion:
D32 = โ diยณ / โ diยฒ = 2.25 ยท ฯ0.25 ยท ฮผL0.16 ยท ฯL0.20 ยท mฬL0.22 ยท ฮPโ0.43
The cumulative volumetric distribution follows the Rosin-Rammler distribution with dispersion parameter q โ 2.85.
Key Engineering Assumptions
- Single-component liquid atomizing in a stagnant or co-flowing gas.
- Newtonian liquid behavior (constant dynamic viscosity ฮผL).
- Pressure-swirl / plain orifice discharge correlation valid for ReL > 500.
- Secondary droplet coalescence and wall impingement are not modeled.