Helicopter impulsive noise: Theoretical and experimental status
Summary (1 min read)
A very good approximation t o these geometrical
- As expected, the advancing-blade/ vortex interactions radiated most of their energy forward and were measured on the right wing-tip and nose-boom microphones.
- Blade/vortex interactions radiated to aft directions and were measured on the left wing tip and elevator microphones, were recorded on the right-wing-tip and nose-boom microphones, even though figure 74 shows that the advancing-blade interaction pressure variations are less than those measured on the retreating side.
- The conclusion to be drawn is that advancing-side BVIs are apparently "acoustically" more efficient than the retreating side B V I s , The retreating-.
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Cites background from "Helicopter impulsive noise: Theoret..."
...By the 1980’s, the emphasis on theoretical development combined with several model scale and flight tests had led to a fairly complete understanding and classification of the physical sources of helicopter rotor noise [21]....
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...George [20] and Schmitz and Yu [21] reviewed the status of helicopter noise in the late 1970’s and the early 1980’s, respectively....
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315 citations
165 citations
Cites background from "Helicopter impulsive noise: Theoret..."
...7r3fl (c) 4 92160 fl-h (41 + fl(79C0 + llC1 +C2 + 316'3 + 42C4))Ch, (1-22)...
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...2M2u)Mc_u (A-7) ACp = e(2- [2 - M2u]Cpu) (1-8) The above relations governing the corrections to Re, q_, M_, and Cp are assumed to apply to both 2D...
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...0181 Note that equations (A-22) and (A-23) reduce to equations (A-20) and (A-21) when (1) the flow is incompressible (/3 = 1); (2) 2/c << 1; (3) c/h << 1; and (4) the airfoil is approximated by a single vortex at the quarter chord....
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...Based on the measured pressure coefficient at a particular location near the leading edge, the velocity is determined from v = - Cp (incompressible) (1) The angle of attack that yields the above v/Voo at this particular _/c is found from...
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...4M_u ) CdOu (1-17) where Ap is the planform area of the wing (Ap = cs for a rectangular wing), CdOu is the uncorrected drag coefficient at zero lift, and the test-section shape parameter A is given by (ref....
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References
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