💻 Microchannel Two-Phase Flow Boiling

Model high-heat-flux two-phase flow boiling in microchannels: two-phase HTC (htp), confinement number (Co), boiling number (Bo), chip wall temperature, and pressure drop.

⚡ Fortran 90 Engine Double Precision (IEEE 754) ✓ ISO / ASME Validated
📊 Solver Telemetry ● ACTIVE
👁️ Consultations 36
⚡ Calculs faits 29
💾 Téléchargements 271 📦 Code Fortran 10.8 KB
📅 Mise en service Jun 2026
⏱️ Latence < 1 ms
⚡ Outils & Rapports :
💾 Télécharger Fortran 90

💻 Silicon Microchannel Cold Plate & Confined Vapor Slugs

Real-time visual simulation: High-heat-flux microchannel array with Taylor vapor slugs sweeping through micro-fins

📝 Configuration & Presets

🖥️ AI GPU Chip (R1233zd) ⚡ EV SiC Inverter (Water) 📡 Radar GaN RF Power ❄️ Micro-Evaporator Loop
📐 Microchannel Array Dimensions
⚡ Operating Hydraulics & Heat Flux
1 W/cm² = 10 kW/m²
🧪 Fluid Thermophysical Properties
Kandlikar Microchannel Formulation:
• Confinement Number: Co = (1/Dh) √(σ / (g (ρL − ρV))) > 0.5
• Boiling Number: Bo = q″ / (G · hfg)
• Two-Phase HTC: htp = max( hNBD, hCBD ) [W/(m²·K)]
• Wall Temperature: Twall = Tsat + (q″ / htp) [°C]

📊 Microchannel Boiling Results

Configure inputs and click Compute to view results.

📘 Calculation Methodology & Microchannel Boiling Standards

Kandlikar Microchannel Correlation

Incorporates confinement effects ($Co$) and boiling number ($Bo$) to capture transition between nucleate bubble nucleation and thin-film evaporation:

htp = max( hNBD, hCBD )

Confinement Number Criterion

When $Co = \frac{1}{D_h}\sqrt{\frac{\sigma}{g(\rho_L - \rho_V)}} > 0.5$, bubble growth is constrained by channel walls, forming elongated Taylor slugs.

Key Engineering Assumptions

  • Parallel rectangular microchannel heat sinks with uniform flow distribution.
  • Saturated two-phase flow boiling regimes ($0.05 \le x \le 0.85$).
  • Applicable to semiconductor electronics, high-power lasers, and compact heat exchangers.