Abstract
Helicopters like the EC 135 with its bearingless main rotor design feature large equivalent hinge offsets of about 10 %, significantly higher than conventional rotor designs and leading to improved maneuverability and agility. For such a helicopter, the fuselage and rotor responses become fully coupled and the quasi-steady assumption using a 6-DoF rigid-body model state space description and approximating the neglected rotor degrees of freedom by equivalent time delays is not suitable. Depending on the intended use of the model, the accurate mathematical description of the vertical motion for these configurations requires an extended model structure that includes inflow and coning dynamics. The paper first presents different modeling approaches and their relationship. Next, identification results for the DLR EC 135 are presented for a model that only describes the vertical motion excluding coupling to the other axes. Here, the differences between the modeling approaches and the respective deficits are explained. Next, the modeling approach most widely used in the rotorcraft identification literature is extended to account for hinge offset. In addition, some model parameters are estimated instead of fixing them at their theoretical predictions which leads to a very good match with EC 135 flight test data. Results for a complete model of the EC 135 including flapping, coning/inflow, and regressive lead–lag are shown as a final result.
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Abbreviations
- \(a_z\) :
-
Vertical acceleration (m/s2)
- \(B_i\) :
-
Coning derivatives (\(i=\nu\), \(\beta _0\), \(\dot{\beta _0}\), \(\delta _{\rm col}\))
- \(c\) :
-
Rotor blade chord (m)
- \(C_{L_\alpha }\) :
-
Blade lift curve slope (1/rad)
- \(C_T\) :
-
Thrust coefficient (\(C_T = T/[\rho \pi R^2 (\Omega R)^2]\))
- \(C_0\) :
-
Inflow constant
- \(e\) :
-
Hinge offset (m)
- \(g\) :
-
Acceleration due to gravity (m/s2)
- \(I_{\beta }\) :
-
Blade flapping moment of inertia (kg m2)
- \(K_{\beta }\) :
-
Flapping stiffness (Nm/Rad)
- \(K_{\theta _0}\) :
-
Control gain (rad/%)
- \(m\) :
-
Aircraft mass (kg)
- \(p\), \(q\), \(r\) :
-
Roll, pitch and yaw rates (rad/s)
- \(R\) :
-
Rotor radius (m)
- \(s\) :
-
Laplace variable (1/s)
- \(T\) :
-
Rotor thrust (N)
- \(T_i\) :
-
Thrust derivatives (\(i=\nu\), \(\dot{\nu }\), \(\dot{\beta _0}\))
- \(u\), \(v\), \(w\) :
-
Body-fixed velocity components (m/s)
- \(V_i\) :
-
Inflow derivatives (\(i=\nu\), \(\dot{\nu }\), \(\dot{\beta _0}\))
- \(Z_i\) :
-
Vertical force derivatives (\(i=u\), \(v\), \(w\), \(p\), \(q\), \(r\), \(\nu\), \(\dot{\beta _0}\), \(C_T\), \(\delta _{\rm lon}\), \(\delta _{\rm lat}\), \(\delta _{\rm ped}\), \(\delta _{\rm col}\))
- \(\beta _0\) :
-
Coning angle (rad)
- \(\delta _{\rm lon}\), \(\delta _{\rm lat}\) :
-
Longitudinal and lateral cyclic inputs (%)
- \(\delta _{\rm ped}\), \(\delta _{\rm col}\) :
-
Pedal and collective inputs (%)
- \(\epsilon\) :
-
Hinge offset ratio (\(\epsilon = e/R\))
- \(\Phi , \Theta\) :
-
Roll and pitch angles (rad)
- \(\gamma\) :
-
Lock number (\(\gamma = \rho C_{L_\alpha } c R^4 /I_\beta\))
- \(\nu\) :
-
Inflow (m/s)
- \(\bar{\nu }_0\) :
-
Trim inflow ratio
- \(\rho\) :
-
Air density (kg/m3)
- \(\sigma\) :
-
Solidity
- \(\tau\) :
-
Time delay (s)
- \(\Omega\) :
-
Rotor rotation speed (rad/s )
- \(m\) :
-
Measured value
- \(0\) :
-
Trim value
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This paper is based on a presentation at the European Rotorcraft Forum, September 2–5, 2014, Southampton, UK.
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Seher-Weiss, S. Comparing different approaches for modeling the vertical motion of the EC 135. CEAS Aeronaut J 6, 395–406 (2015). https://doi.org/10.1007/s13272-015-0150-7
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DOI: https://doi.org/10.1007/s13272-015-0150-7