NASA ARA M100 Wingbody (Large)

Validation: ARA-M100 Version 1.0


  • Transonic Aerodynamics
  • External Aircraft Component Design

Models active in this Validation Case

  • Compressible flow
  • Energy models
  • Ideal gases
  • Mixed Precision


To profile the accuracy and performance of Envenio’s EXN/AERO manycore CFD solver on a challenging transonic aerospace test case. We undertook this demonstration to show that DES and LES are realistic options today for solvers that are properly optimized for low-cost heterogeneous computing architectures. Engineers working in aerospace have been seeking this capability for some time now in order to explore corners of the operating envelope, to understand complex interactions of wing components (e.g. flaps) and to identify ways to reduce noise.

Reference Case Description

The ARA M100 wing body geometry is based on a scale wind tunnel model and is referenced by NASA as a validation case for CFD codes with compressible / transonic flow capability. The configuration of the model is similar to what is seen in civil and military transport aviation and features a finite wing, a realistic wing root and a fuselage. Dimensions are shown in Figure 1.  

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Figure 1: ARA M100 general dimensions in mm. Image source refefenced in bibliography.

Surface Mesh: The surface mesh used to create the CFD grid is available on the site (link in bibliography). General dimensions are shown in Figure 1.

Coordinates & Domain Size

X direction: Roll axis, positive streamwise

Y direction: Pitch axis, positive to starboard

Z direction: Yaw axis, positive to top of aircraft


X dimension ~41 m

Y dimension ~21.75 m

Z-dimension ~41 m


Position of model:

Upwind face relative to inlet: ~20.5 m

Y position: Centred

Z position: Attached to symmetry plane


Mesh Resolution in the vicinity of the fuselage;

This 3D wing/body test case is at Ma.=0.803 and chord Reynolds number Rec = 13.1 × 106 (max chord = 0.378 m). The mesh has a y+ distribution as follows:

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The mesh generator was instructed to use a wall function over the fuselage and direct solve-to-wall was employed on the wing. Freestream turbulence levels used as mesh generator inputs are Tu = 0.5% and µt/µ = 25.

Total Mesh Size: ~100.3 Million

Simulation Completion Criteria

The simulation is run until the coefficients of lift and drag achieve a time-averaged variation less than 1e-4 for CL and 1e-5 for CD.  In this analysis the averaging window size, (4750 timesteps, 0.0095 seconds), is equal to the fuselage length (1.7m) divided by 0.7*Vfreestream,(0.7*257.4m/s = 180m/s) which is taken to be the convection time for the near-body fluid past the body.  Successive averaging windows are computed 100 timesteps apart.  The results of this analysis are presented in Figure 2.  From this figure we see that CL converged in approximately 7200 timesteps and CD converged in approximately 8400 timesteps.  

Simulation Setup

Solver Control

Time Step: 2e-6 seconds

EXN GPU Allocation: 6 Nvidia K80 GPUs (3x K80 cards, 2x GPU per card)

EXN CPU Allocation: 10 Intel Xeon 2.6GHz


X-axis orientation: Positive downstream

Y-axis orientation: Positive to the left of the body, looking downstream

Z-axis orientation: Positive upward, normal to ground plane


Boundary Conditions

Turbulence Kinetic Energy: 0.0001 m2/s2

Turbulence K Dissipation: 0.0003 m2/s3

Wall model: Smooth wall

Outlet: Constant Specified Pressure


Initial Velocity: [257.1,  0,  12.9] m/s

Angle of Attack: 2.870 deg

Mach Number: 0.803

Temperature:  255 Kelvin

Pressure: 315.98 kPa


Fluid Settings

Initial Velocity: [257.1,  0,  12.9] m/s

Initial Turbulence Kinetic Energy: 0.0001 m2/s2

Initial Turbulence K Dissipation: 0.0003 m2/s3


Turbulence Model: DES SST k-omega

Flow type Compressible, Ideal Gas (R = 286.9 J/kg K)

Constant Viscosity: 1.715 x 10-5 kg/m s


Precision Mixed precission 93.3M Single precission, 7.0M Double precission


Other notes

Body convection time:  0.0095 seconds (4750 time steps)

Total simulated time:  0.01842 seconds (9210 time steps, 1.94 washthroughs)

Mesh Topology Structured multiblock, one-to-one connections at block interfaces, data written as structured arrays in CGNS format


Simulation Outcomes, Timing, and External Factors

The pressure coefficient profiles at different spanwise locations along the wing, namely at span-normalized cross section y/B = 0.123, y/B = 0.231, y/b = 0.325, y/B = 0.455, y/B = 0.633 and y/B = 0.817 are presented in Figures 2 thru 7. The pressure distribution across upper wing surface and fuselage is shown graphically in Figure 8. Table 1 shows simulation performance outcomes and Table 2 shows approximate simulation cost information.


Table 1: Simulation performance outcomes

Reporting Item EXN/Aero
Simulation starting conditions Simulation initial conditions were interpolated from a previous

coarse mesh, 25M control volume, simulation.

Time to 1st wash-through Simulated time of 0.0095 sec requires 4750 time steps.

This is equivalent to real-time ~70 hours (2.9 days).

Time to completion

(CL & CD criteria)

Simulated time of 0.01842 sec requires 9210 time steps

This is equivalent to real time ~136 hours (5.6 days).

Real time per time step 53sec
CPU type Intel Xeon @ 2.6GHz
CPU cores 10
GPU type NVIDIA Tesla K80
GPU cores 6 x 2496 CUDA core per GPU
Available Memory 128GB system, 24GB each K80 card (12GB each GPU)


Table 2: Simulation cost information, assuming an owned system and a single license of EXN/Aero, operating year-round; figures in US dollars.

Commercial Open Source EXN/Aero
Req’d CPU Processors 192 192 10 192 192 10
Req’d GPU Processors 6
Req’d System Hours 720 720 135
Cost per system-hour $17.28 $17.28 $7.50
Total Compute Cost $12,441.60 $12,441.60 $1,012.50
Pro-rated license (req’d hrs / 8750 hrs) *annual license $23,918 0 $462.86
Cost of Simulation $36,359 $12,441 $1,475
Cost Reduction 95.94% 88.14%  

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Figure 2: Convergence of lift and drag coefficient during the the EXN/Aero simulation.

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Figure 3: Comparison of EXN/Aero simulation and experimental results at y/B=0.123

Screen Shot 2017-01-12 at 11.44.43Figure 4: Comparison of EXN/Aero simulation and experimental results at y/B=0.231

Screen Shot 2017-01-12 at 11.45.23Figure 5: Comparison of EXN/Aero simulation and experimental results at y/B=0.325

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Figure 6: Comparison of EXN/Aero simulation and experimental results at y/B=0.455

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Figure 7: Comparison of EXN/Aero simulation and experimental results at y/B=0.633

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Figure 8: Comparison of EXN/Aero simulation and experimental results at y/B=0.817

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Figure 9: Pressure coefficient contours at the cross section

The comparison of pressure coefficient profiles with the experimental profiles reveals that our model matches closely with the experiments in subsonic regions of the wing. For the two outboard wing sections (y/B 0.633) the Cp distribution is accurately represented by simulation data. For inboard sections (y/B < 0.633) the drop in Cp is delayed and smoother than the experimental data. Inset images from a Cobalt simulation using the Spalart-Almaras RANS model show an early drop in Cp on inboard sections. It is expected that mesh refinement in the vicinity of the shocks will bring EXN/Aero results more in line with experimental data sets; this work is planned as part of Enveino’s QA process and will be updated regularly on Envenio’s wiki site (accessible on


We completed the 100 million node transonic DES simulations for the ARA-M100 wing body in 5.9 days. It had a Reynolds number of 13.2M. It ran on one of our desktop compute nodes and the computing burden was shared by 3 Nvidia K80 cards and 6 CPUs.

Recall that this is run on 3 Nvidia K80 GPU cards and 6 Intel CPU on a desktop-scale computer, which was the minimum hardware arrangement. Even in the minimum arrangement, this result is fast by DES standards. A properly resourced simulation (e.g. a desktop equipped with 6 or more K80 GPU) has the potential to be much faster.

If you would like to run one of your meshes on our solver, we have it hosted on a cloud server so you can access it via your browser. Just click the link below for more details.

Try EXN/Aero


  • External Flow
  • DES SST k-omega
  • Compressibility
  • Energy Models
  • Double Precision
  • Integrated Boundary Values
  • External Flow
  • Lift & Drag
  • Vehicle Maneuvering
  • Transonic Flow


  1. Wing geometry available from:
  2. Figures 3-8 insets from:
  3. ARAA-M100 Diagrams (Figure 1)