This relates to the field of vibration and noise control for any system with an unwanted vibratory disturbance.
Multiple helicopter original equipment manufacturers (OEMs) are interested in hub-based active vibration control (AVC). Placing force generators on the helicopter hub provides the capability of canceling hub loads near the source, thus enabling global vibration control.
One type of hub-based force generator comprises two co-rotating motorized imbalanced rotors. These rotors may rotate in the same direction as the hub such that the masses are rotating at the blade pass frequency. These rotors create a controllable rotating force vector that can be controlled to cancel hub loads. Another type of hub-based force generator comprises two pairs of co-rotating motorized imbalanced rotors—one pair rotating in the same direction as the hub, and the other pair rotating in the opposite direction.
One challenge with hub-based AVC, however, pertains to the need to address certain failure modes such as loss of operation or loss of power in which the imbalanced rotors will discontinue rotating relative to the hub. They may come to a stop in a statically balanced condition, in a statically worst case imbalance condition, or in some condition in between. The static imbalance that results after loss of operation will create 1P hub loads that will cause vibration on the hub, the gearbox and the engines. The static imbalance condition that results after such a failure mode may dictate the severity of the failure mode (e.g., minor, major, hazardous, or catastrophic). For example, if after loss of operation, the rotors come to rest in a statically mass balanced condition, this may be classified as a Minor failure mode. On other hand, if after loss of operation, the rotors come to rest in a severely imbalanced condition, the resulting 1P loads and vibration may be severe enough that this may be classified as a Hazardous or catastrophic failure mode. If the latter is true, a hub-based AVC system design is required that will sufficiently mitigate this failure mode. Accordingly, there is a need for improvements to design and system architecture to address potentially hazardous and catastrophic failure modes.
A hub based AVC design has been conceived that includes at least one pair of co-rotating motorized imbalanced rotors that create a controllable rotating force vector that can be controlled to cancel hub loads on a rotating hub. This control is achievable using a configuration in which each rotor has an axis of rotation that is offset from the hub axis of rotation. In this way, in a loss of operation failure mode, the system is designed such that centrifugal forces will cause the masses to spin to an orientation of low static imbalance.
In one aspect the hub-based AVC system comprises a hub associated with a rotary wing aircraft, at least one controller, at least one sensor, and at least one pair of imbalanced rotors. The hub configured for rotation about a hub axis of rotation at a hub frequency. The at least one sensor in electronic communication with the at least one controller, the at least one sensor configured to measure at least one vibration associated with the rotary wing aircraft. The at least one pair of imbalanced rotors coupled with the rotating hub, the at least one pair of imbalanced rotors comprising: a first imbalanced rotor having a first axis of rotation that is offset in a first direction from the hub axis of rotation; and a second imbalanced rotor having a second axis of rotation that is offset from the hub axis of rotation in a second direction that is different from the first direction. Wherein the at least one controller is configured to provide control to at least one of the imbalanced rotors. Wherein the at least one pair of imbalanced rotors is configured for co-rotation at a controllable rotor speed. Wherein a phase associated with each imbalanced rotor is adjustable to create a controllable rotating force vector
In another aspect, a method for active vibration control at a rotating hub of a rotary wing aircraft is provided. The hub configured for rotation about a hub axis of rotation at a hub frequency. The method comprises: providing at least one controller and at least one sensor capable of measuring a vibration in the rotary wing aircraft, wherein the at least one sensor is in electronic communication with the at least one controller; providing at least one pair of imbalanced rotors coupled with the hub, the at least one controller controlling the at least one of imbalanced rotors; during normal operation, co-rotating at least one pair of imbalanced rotors that are coupled with the hub at a controllable rotor speed, wherein a phase associated with each imbalanced rotor is adjustable to create a controllable rotating force vector; and during a loss of operation or loss of power failure mode, rotating the at least one pair of imbalanced rotors to an orientation of low static imbalance with respect to one another.
Although some of the aspects of the subject matter disclosed herein have been stated hereinabove, and which are achieved in whole or in part by the presently disclosed subject matter, other aspects will become evident as the description proceeds when taken in connection with the accompanying drawings as best described hereinbelow.
Referring to
The control electronics include at least one controller (not shown) and at least one sensor (not shown). The at least one sensor is in electronic communication with the at least one controller, the at least one sensor configured to measure at least one vibration associated with the rotary wing aircraft. In one embodiment, the at least one controller is configured to provide control to at least one of the imbalanced rotors. In one embodiment, each imbalanced rotor has at least one controller providing control thereto. In another embodiment, each pair of imbalances rotors has at least one controller providing control thereto. In another embodiment, the at least one controller is configured to provide control to at least one pair of the imbalanced rotors. In one embodiment, the at least one controller is configured to adjust a magnitude of the controllable rotating force vector.
As illustrated in
The system 100 includes at least one pair of imbalanced rotors coupled with the rotating hub 101. Referring to the configuration shown in
Regardless of the particular configuration, the at least one pair of imbalanced rotors is configured for co-rotation at a rotor speed that is controllable to be a multiple of the hub frequency, and a phase associated with each imbalanced rotor is adjustable to create a controllable rotating force vector. In particular, in some embodiments, normal operation of the system 100 can involve the hub 101 spinning at frequency Ω, and the at least one pair of imbalanced rotors being driven to co-rotate at a rotor speed NΩ (with respect to the stationary frame), where N is a multiple of the hub frequency.
In some embodiments, the system 100 is further configured such that, during a loss of operation or loss of power failure mode, the at least one pair of imbalanced rotors is configured to rotate to an orientation of low static imbalance with respect to one another.
To model this force,
{umlaut over (θ)}+2ζωn{dot over (θ)}+ωn2 sin θ=α sin(Ωt+θ)
where
where J is the rotor inertia. The natural frequency of the pendulum mass in the centrifugal field is ωn. The radius r, in a general sense, is an effective radius defining the location of the center of mass of the imbalanced rotor. In this case, rotor inertia is J=mr2 and the motion of the system can be characterized by the following parameters:
Whereas α is only a factor when gravity is present, the non-dimensional ratio ωn/Ω affects many design considerations. In particular this affects (a) the speed at which the imbalanced rotors will achieve a balanced condition upon loss of motor operation, (b) the amplitude of 1 P rotor wobble due to gravity after loss of operation, (c) the additional motor power resulting from rotor offset, and (d) the parasitic moment during normal operation resulting from rotor offset.
The dimensionless ratio ωn/Ω will dictate the speed at which the offset imbalanced masses become statically balanced upon loss of operation. The number of hub rotations M it will take for the system to settle out to the static balance condition is proportional to the following:
where ζ is the torsional damping ratio of the system.
When gravity is present, the right hand side term involving α imposes an oscillatory torque on the imbalanced rotor. The rotor responds with an oscillation at frequency Ω and steady state magnitude Θ:
Because the dynamics of the system are inherently non-linear when the gravitational disturbance is applied, the analytical expression for the steady-state magnitude of the disturbance oscillation is only an approximation.
In view of these considerations, in some embodiments, it can be advantageous for the offset distances R for each imbalanced rotor to be sized such that a ratio of the offset distance R to the radius r has a value that is within a range that provides desired performance. For example, the ratio of R/r can be less than a upper limit at which an expected centripetal field (e.g., about 4 g) would yield uncontrollable imbalances and/or very steep power increases. Additionally, the ratio of R/r can be selected to be greater than a lower limit below which the settling time Ωτsettle is undesirably large (e.g., number of hub rotations M is greater than about 4). For example, in some embodiments, the system 100 may provide desirable functionality with values of R/r between 0.02 and 0.2.
During typical operation of the system (e.g., while motors are running), there is additional power required due to the offset radius of the rotors. Per rotor, there is an additional sinusoidal power required PR due to the offset R which occurs at frequency (N−1)Ω at an amplitude:
where N−1 is the multiple of Ω at which the imbalanced rotor is spinning in the rotating frame.
A parasitic torque during normal operation will result from the rotor offset. The maximum parasitic torque τmax occurs when the imbalanced rotors are spinning at NΩ and are neutralized.
The requirement of this additional sinusoidal power PR and the presence of this parasitic torque is tolerated, however, because the offsets of the imbalance rotors allow the system 100 to better address potentially hazardous and catastrophic failure modes as discussed above.
In other embodiments, additional imbalanced rotor pairs are added. In the non-limiting embodiment shown in
Other embodiments of the present invention will be apparent to one skilled in the art. As such, the foregoing description merely enables and describes the general uses and methods of the present invention. Accordingly, the follow claims define the true scope of the present invention.
The present application claims the benefit of U.S. Provisional Patent Application Ser. No. 61/927,741, filed Jan. 15, 2014, the disclosure of which is incorporated herein by reference in its entirety.
Filing Document | Filing Date | Country | Kind |
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PCT/US2015/011594 | 1/15/2015 | WO | 00 |
Number | Date | Country | |
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61927741 | Jan 2014 | US |