Tilt-Wing eVTOL Transition Corridor, Stall and Pitch Trim

Map airspeed against wing tilt using coupled force and pitch equilibrium, propeller slipstream, wing stall, thrust and power limits. Inspect a chosen transition path.

#eVTOL #pitch trim #tilt-wing #transition corridor #wing stall

Caution

Do not use this corridor to fly or program an aircraft. Establish operating limits with validated vehicle data and approved flight-test procedures.

A tilt-wing aircraft changes from thrust-supported hover to wing-supported flight by rotating its wings and propellers. The difficult part is the interval between those endpoints: the wing may meet the local airflow at too large an angle, the motors may run out of thrust or power, or the available pitch controls may be unable to balance the aircraft. This tilt wing transition corridor calculator puts those constraints on one airspeed–tilt map.

The tool is intended for engineers comparing early designs, students studying powered lift, and readers investigating why an apparently reasonable conversion schedule can fail. It models a tandem arrangement with forward and aft wings sharing a common tilt angle. Each wing has its own propeller group, aerodynamic forces and moment arm. It is a design estimate, not a flight envelope or a flight-planning aid.

Start with mass, total wing area, the forward-area fraction and the distances from the center of gravity to both wings. Enter total propeller disk area and the total thrust and electrical power limits. Each group receives half the disk area and half the installed thrust capacity. Replace the illustrative aerodynamic coefficients and control effectiveness values with data appropriate to your aircraft. The default mass, wing area and maximum lift coefficient match the scale of NASA's GL-10 stall-speed example; the tandem geometry, propulsion and control settings are illustrative and do not reproduce GL-10.

The conversion corridor chart shows the calculated limits and your chosen operating path. Set a knee airspeed and wing tilt between the hover endpoint and the final zero-tilt endpoint. Move or play Path position to inspect equilibrium along that schedule. The animation is a sequence of trim points, not a time simulation. A utilization of one marks a limit. The speed-band table lists every consecutive group of feasible grid samples at each tilt; multiple rows at one angle preserve separated bands. Blank speed cells mean no feasible sample was found. Neither the table nor the colored cells establishes an exact boundary between samples.

For each point, the solver balances horizontal and vertical forces and pitching moment. Momentum theory supplies induced velocity, which changes both wing angle of attack and dynamic pressure in the propeller slipstream. The model checks wing stall, individual group thrust, total electrical power, pitch-control command and body attitude. A path can cross a wing-stall gap despite having feasible hover and cruise endpoints.

This eVTOL transition calculator excludes dynamic stability, gust response, actuator rates and torque, rotor blade limits, wing–wing wake interaction, structural loads and failures. Those omissions matter in a real conversion corridor. Use validated aerodynamic and propulsion data and a vehicle-specific dynamic model before interpreting any point as an operating limit.

How it is calculated

The implemented model is a longitudinal tandem tilt-wing equilibrium with a prescribed common wing tilt β\beta, flight-path angle γ\gamma and along-path acceleration aa. Positive body pitch θ\theta is nose-up; tilt is relative to the body, with 90° in hover configuration. The solver finds total thrust TT, body pitch and normalized pitch-control command uu together.

Each wing has a blown and an unblown zone. For each propeller group, the positive propulsive branch of uniform oblique momentum theory is solved:

Tj=2ρAjvi,j(U∥+vi,j)2+U⊥2.T_j=2\rho A_jv_{i,j}\sqrt{(U_\parallel+v_{i,j})^2+U_\perp^2}.

Here U∥=Vcos⁡(θ+β−γ)U_\parallel=V\cos(\theta+\beta-\gamma) and U⊥=Vsin⁡(θ+β−γ)U_\perp=V\sin(\theta+\beta-\gamma). Eight scalar Newton updates are applied in parallel across points. The axial limit agrees with May, Milz and Looye (2023), Eq. 37, attached PDF p. 12. Negative axial inflow is excluded.

In a blown zone, the effective velocity is the freestream vector plus ksvik_s v_i along the thrust axis. In an unblown zone it is the freestream alone. Its direction gives local flow angle ψ\psi, so α=θ+β−ψ\alpha=\theta+\beta-\psi and q=ρ∣U∣2/2q=\rho|\mathbf U|^2/2. This follows the local-flow/strip-force construction in May et al., Eqs. 26–34, attached pp. 10–11, using two uniform zones per wing. The finite-wing polar is CL=aL(α−α0+τfδ)C_L=a_L(\alpha-\alpha_0+\tau_f\delta), CD=CD0+kCL2C_D=C_{D0}+k C_L^2 and Cm=Cm0+CmδδC_m=C_{m0}+C_{m\delta}\delta, with angles in radians. Lift and drag are rotated from each local flow direction into earth axes.

Pitch control follows a declared allocation: d=dmaxusin⁡2βd=d_{max}u\sin^2\beta, Tf=T(1+d)/2T_f=T(1+d)/2, Ta=T(1−d)/2T_a=T(1-d)/2, and δf=−δa=δmaxucos⁡2β\delta_f=-\delta_a=\delta_{max}u\cos^2\beta. Thus differential thrust dominates hover and differential elevons dominate cruise. Forces, thrust moments and local qScCmqScC_m are summed about the CG; the moment arm calculation uses body coordinates, including wing height. Fuselage drag acts at the CG. Group electrical power is Tj(U∥+κivi)/ηT_j(U_\parallel+\kappa_i v_i)/\eta.

A bounded, finite-difference Newton solve enforces ΣFx=macos⁡γ\Sigma F_x=ma\cos\gamma, ΣFz=mg+masin⁡γ\Sigma F_z=mg+ma\sin\gamma, and ΣM=0\Sigma M=0. Accepted residuals are below 10−510^{-5} after normalization by weight and weight times total wing-arm distance. Feasible samples also satisfy ∣CL∣≤CLmax|C_L|\leq C_{Lmax} in every nonzero-area, moving-air zone, Tj≤Tlim/2T_j\leq T_{lim}/2, P≤PlimP\leq P_{lim}, ∣u∣≤1|u|\leq1, and ∣θ∣≤θlim|\theta|\leq\theta_{lim}. Outside stall, the unbounded attached-flow polar is used only to locate a failed constraint; those force and power values are extrapolations, not post-stall predictions.

Assumptions

  • Rigid tandem wings with equal mean chord, common tilt, fixed CG, and independently loaded forward/aft propeller groups. Each group has half the total disk area and half the installed thrust capacity. Wing aerodynamic centers and thrust application points coincide at the specified arms and height.
  • Wing slope, drag, maximum lift and control derivatives are design inputs, assumed constant with Reynolds number, tilt and thrust. Maximum positive and negative lift magnitudes are assumed equal; elevon deflection shifts the lift curve. Calibrated finite-wing coefficients are required.
  • Uniform induced flow over the specified blown fraction; the same wake multiplier and area fraction apply to both wings. The remaining area is explicitly evaluated in free flow. A stalled uncovered strip excludes a point even when its load is small; at exactly zero local speed it carries no force and imposes no stall test.
  • Constant density, straight flight path, zero pitch rate and zero angular acceleration. A nonzero acceleration is a local force-balance prescription, not an integrated trajectory.
  • Default mass 25.9 kg, area 0.737 m² and CLmax 1.43 come from NASA/TM-2017-219794, attached p. 28. That report's area unit “m3” is a typographical error; area is m². Geometry, disk area, coefficients, limits and the chosen schedule are illustrative engineering assumptions. This is not a GL-10, VZ-2 or XC-142 performance reproduction.

Where it applies

This is a design estimate for the stated tandem configuration and control allocation, not a flight envelope. A feasible cell establishes only the modeled longitudinal force and pitch balance; it establishes neither static nor dynamic stability, handling qualities, reserve control authority or an executable transition.

The corridor uses 13 airspeeds by 19 tilt angles (5° tilt spacing; default speed spacing 2.92 m/s). The operating path uses 41 independently solved samples. This keeps browser work small while retaining the coupled physics, at the cost of missing narrow bands and exact boundary locations. Cells extend halfway toward neighboring samples only for display. The table reports sample endpoints, preserves disjoint bands, and never certifies the interval between samples. Path position is solved independently on each animation frame.

The equilibrium solver uses at most 16 bounded Newton iterations and the inflow solver eight updates. A gray “Unresolved” cell means no admissible converged solution was obtained or axial inflow was negative; it is not proof that every possible trim branch is impossible. Blank selected-point results have that same meaning. Multiple trim branches and alternative control allocations can exist.

Stall and lift/drag parameters need measured or validated vehicle data. The two-zone approximation omits spanwise gradients, wake contraction and skew, swirl, propeller–propeller and wing–wing interference, flow separation detail and dynamic stall. The wake multiplier is an input, not a computed wake geometry. The electrical power expression uses a lumped efficiency allowance and induced-loss factor; it does not replace motor/propeller maps or include a separate fixed profile-power term.

No descent, windmill-brake operation, gusts, ground effect, lateral/directional trim, actuator rates or wing-tilt torque, structural limits, battery sag/thermal limits, rotor tip Mach/blade stall or failure cases are checked. In particular NASA/TM-2017-219643, attached p. 17, identifies tilt-actuator torque as an additional GL-10 corridor boundary. The present model must not be interpreted as including it. Reference cases verify the stall-speed and actuator-disk submodels; no independent aircraft-level transition or pitch-trim validation is claimed. The corridor drawing uses fixed SI axes; inputs, scalar results and numeric table columns retain their declared units for the viewer's metric/US conversion.

References

  • May, M. S., Milz, D. and Looye, G. (2023). Semi-Empirical Aerodynamic Modeling Approach for Tandem Tilt-Wing eVTOL Control Design Applications. AIAA 2023-1529. DOI: 10.2514/6.2023-1529. Open author manuscript: https://elib.dlr.de/199983/1/PaperWithCopyrightNotice.pdf
  • NASA/TM-2017-219794 (2017), GL-10 flight-testing report, attached p. 28 (printed p. 25), measured CLmax and stall-speed example: https://ntrs.nasa.gov/citations/20180000765
  • NASA/TM-2017-219643 (2017), GL-10 design, development and flight testing, attached pp. 17–18 (printed pp. 14–15), corridor constraints and pitch-control schedules: https://ntrs.nasa.gov/citations/20170007194
  • Pegg, R. J. (1962). Summary of Flight-Test Results of the VZ-2 Tilt-Wing Aircraft. NASA TN D-989, attached pp. 3 and 8: https://ntrs.nasa.gov/citations/19980227196
  • O'Brien, D. M. (2006). Analysis of Computational Modeling Techniques for Complete Rotorcraft Configurations. PhD thesis, Georgia Institute of Technology, §4.2, theoretical rotor: 6.26 lbf/ft² disk loading and 36.3 ft/s hover inflow. https://hdl.handle.net/1853/10535

Inputs

InputSymbolUnitDefault
Massmasskg25.9
Air densityrhokg/m^31.225
Total wing areaS_wm^20.737
Mean wing chordc_wm0.3
Forward wing area fraction
The remaining area belongs to the aft wing.
sf0.5
Forward wing armlfm0.8
Aft wing armlam0.8
Wing height above CG
Positive above the center of gravity.
zwm0.05
Total propeller disk areaA_diskm^21
Total thrust limitT_limN500
Electrical power limitP_limW5000
Power efficiency factor
Lumped motor, drive and propeller profile-loss allowance.
eta0.8
Induced power factork_ind1.15
Wing slipstream multiplier
One at the disk; two in an ideal fully developed wake.
wake1.6
Blown wing area fraction
Set from the wing area actually immersed in propeller wakes.
blown1
Wing lift slope
Lift coefficient change per radian, including finite-wing effects.
a_lift4.5
Zero-lift anglealpha0deg-2
Maximum lift coefficientCL_lim1.43
Wing profile drag coefficientCD00.025
Induced drag factork_drag0.06
Fuselage drag areaCdAm^20.05
Wing pitching moment coefficientCm0-0.025
Elevon lift effectiveness
Effective angle-of-attack change per radian of elevon deflection.
flap_tau0.45
Elevon moment derivative
Pitching moment coefficient change per radian of local elevon deflection.
Cm_delta-0.2
Elevon deflection limitdelta_limdeg20
Differential thrust fraction
At full command: forward thrust T(1+d)/2 and aft thrust T(1−d)/2.
diff_lim0.35
Body pitch limittheta_limdeg25
Flight path angle
Positive for a climb; descent and windmill-brake states are excluded.
gamma_fdeg0
Along-path acceleration
Zero gives steady flight; positive values prescribe forward acceleration.
a_pathm/s^20
Cruise path airspeedV_endm/s30
Path knee airspeedV_kneem/s12
Path knee tiltbeta_kneedeg40
Chart maximum airspeedV_maxm/s35
Path position
Play moves along the chosen speed–tilt schedule; it does not integrate a flight.
path_s0.68

Results

With the default inputs above, the calc gives:

ResultValue
Selected pointModel limits met
Chosen pathPath crosses model limits
Selected path airspeed20.4 m/s
Selected wing tilt21.3 deg
Required total thrust39.5 N
Required electrical power1.022 kW
Required body pitch-7.74 deg
Forward elevon deflection0.09 deg
Required pitch control command0.005
Wing stall utilization0.817
Group thrust utilization0.079
Electrical power utilization0.204
Pitch-control utilization0.31
Forward blown-wing angle of attack12.83 deg
Aft blown-wing angle of attack12.83 deg
Unpowered wing-borne stall speed19.84 m/s

Checked against sources

Each case below was calculated by this calc and agrees with the value from its source (within the tolerance where one is shown).

NASA GL-10 wing-borne stall speed

Source: NASA/TM-2017-219794 (2017), printed p. 25 / attached p. 28: independent wind-tunnel CLmax 1.43 and published stall speed 19.6 m/s for mass 25.9 kg, density 1.255 kg/m³ and area 0.737 m². The report uses g=9.8 m/s²; standard gravity here changes speed by 0.034%. Its area unit m³ is a typographical error. Tolerance 0.05 m/s reflects the reported one-decimal-place speed.

Inputs: Air density = 1.255 kg/m³; the others as above.

ResultSourceThis calc
Unpowered wing-borne stall speed19.6 ± 0.05 m/s19.598 m/s

Published actuator-disk hover inflow

Source: D. M. O'Brien, Analysis of Computational Modeling Techniques for Complete Rotorcraft Configurations, Georgia Tech PhD thesis (2006), §4.2, Eq. 60: disk loading 6.26 lbf/ft² yields 36.3 ft/s at the disk in hover. Normalize total disk area to 1 m² and mass to 30.564 kg; use sea-level density 1.225 kg/m³. Published rounded inflow is 11.06424 m/s. The university repository source is open access but its full text was not retrievable by the attachment service; the indexed §4.2 passage supplies the reference. https://repository.gatech.edu/server/api/core/bitstreams/ab597fb9-5000-4b42-b8fe-a03502e04be8/content Tolerance 0.016 m/s reflects rounding of 36.3 ft/s to 0.1 ft/s.

Inputs: Mass = 30.564 kg; the others as above.

ResultSourceThis calc
Ideal weight-supporting hover inflow11.064 ± 0.016 m/s11.061 m/s

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