🔥 Compressible Rayleigh Flow (Heat Addition)

Evaluate 1D compressible flow with heat addition or combustion, computing exit Mach (M2), thermal choking limit (q_max), stagnation pressure loss, and entropy generation.

⚡ Fortran 90 Engine Double Precision (IEEE 754) ✓ ISO / ASME Validated
📊 Solver Telemetry ● ACTIVE
👁️ Consultations 44
⚡ Calculs faits 35
💾 Téléchargements 238 📦 Code Fortran 4.4 KB
📅 Mise en service Jun 2026
⏱️ Latence < 1 ms
⚡ Outils & Rapports :
💾 Télécharger Fortran 90

🔥 Combustor Duct Thermal Expansion & Thermal Choking (M = 1.0)

Real-time visual simulation of flame heat zone, thermal acceleration & Rayleigh entropy increase

📝 Configuration & Presets

⚡ Gas Turbine Combustor 🚀 Ramjet Afterburner ✈️ Scramjet (M = 2.4) 🏭 Furnace Burner Duct
🔥 Thermal Heat Addition & Gas
Air: 1.005, Combustion Gas: 1.15–1.25
🚀 Inlet Flow & Stagnation State
Rayleigh Flow Formulations:
• Stagnation Temp Ratio: T₀/T₀* = 2(γ+1)M² (1 + ½(γ−1)M²) / (1 + γM²)²
• Max Heat Addition: qmax = cp (T₀* − T₀₁) [kJ/kg]
• Heat addition accelerates subsonic flow toward M=1 and decelerates supersonic flow.
• Total Pressure Loss: ΔP₀ is unavoidable during heat addition at high speed.

📊 Rayleigh Flow Results

Configure inputs and click Compute to view results.

📘 Calculation Methodology & Rayleigh Flow Standards

Thermal Choking Limit

Adding heat to a subsonic compressible flow increases Mach number and entropy up to the sonic point $M=1$. Exceeding $q_{max}$ causes thermal choking:

qmax = cp (T₀* − T₀₁)

Combustion Total Pressure Loss

Fundamental momentum conservation dictates that adding thermal energy to a high-speed gas creates an unavoidable fundamental total pressure drop $\Delta P_0$.

Key Engineering Assumptions

  • 1D steady frictionless flow in constant cross-sectional area duct.
  • Uniform thermal energy addition across the stream.
  • Ideal gas with constant average $c_p$ and $\gamma$.