๐ฟ Impinging Jet Array Heat Transfer (Martin)
Compute impinging round nozzle array Nusselt number (Nu_avg), convective heat transfer coefficient (h), stagnation peak flux, and orifice pressure drop using Martin (1977) correlation.
โก Fortran 90 Engine
Double Precision (IEEE 754)
โ ISO / ASME Validated
๐ Solver Telemetry
โ ACTIVE
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39
โก Solves
30
๐พ Downloads
399
๐ฆ Fortran Code
10.8 KB
๐
Released
Jun 2026
โฑ๏ธ Latency
< 1 ms
๐ฟ Array of Impinging Nozzle Jets & Stagnation Cooling Layer
Real-time visual simulation of vertical high-speed fluid jets, target impingement spots & radial wall-jet spread๐ Configuration & Presets
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Martin (1977) Array Formulation:
โข Area Fraction: f = (ฯ/4) / (S/d)ยฒ
โข Average Nusselt: Nu = 2โf ยท [ (1 โ 2.2โf) / (1 + 0.2(H/d โ 6)โf) ] ยท 2 Re0.5 (1 + 0.005 Re0.55)0.5 Pr0.42
โข Heat Flux: qโณ = havg ยท (Ts โ Tj) [kW/mยฒ]
โข Orifice Drop: ฮP โ 0.75 ยท ฯ Ujยฒ [kPa]
โข Area Fraction: f = (ฯ/4) / (S/d)ยฒ
โข Average Nusselt: Nu = 2โf ยท [ (1 โ 2.2โf) / (1 + 0.2(H/d โ 6)โf) ] ยท 2 Re0.5 (1 + 0.005 Re0.55)0.5 Pr0.42
โข Heat Flux: qโณ = havg ยท (Ts โ Tj) [kW/mยฒ]
โข Orifice Drop: ฮP โ 0.75 ยท ฯ Ujยฒ [kPa]
๐ Jet Impingement Results
Configure inputs and click Compute to view results.
๐ Calculation Methodology & Martin Impingement Standards
Martin (1977) Correlation
The standard correlation accounts for the interaction between neighboring jet fountains and cross-flow spent fluid resistance in periodic nozzle arrays:
Nu = 2โf ยท [ (1 โ 2.2โf) / (1 + 0.2(H/d โ 6)โf) ] ยท F(Re) ยท Pr0.42
Stagnation vs Wall-Jet Zone
Peak heat transfer occurs directly beneath the nozzle center ($Nu_0$). In arrays, spent cross-flow deflects outer jets and moderates area-averaged performance.
Key Engineering Assumptions
- Square or hexagonal array of sharp-edged circular orifice nozzles.
- Validity range: $2000 \le Re_d \le 100,000$, $0.004 \le f \le 0.04$, $2 \le H/d \le 12$.
- Constant fluid thermophysical properties at film temperature.