Subject: NAS2-99090 August monthly report
Date: September 5, 2000
The following items were completed or worked on during
August.
- Completed new spinner plug and fabricate new spinner
mold.
- Added camera on tail boom.
- Modified software and data display per pilots'
suggestions.
- Checked out electrical systems.
- Shortened push/pull cables for rudders and horizontal
stabilator and installed rudders and stabilator
- Calibrated all data collection sensors
- Tested propeller and controller
| Prop |
| Summary
of test results |
| Engine
RPM |
Prop
RPM |
HP* |
Thrust |
K** |
| 4000 |
1455 |
206 |
1005 |
7.03 |
| 4500 |
1636 |
233 |
1180 |
7.60 |
| 5000 |
1818 |
258 |
1331 |
8.00 |
| 5500 |
2000 |
272 |
1408 |
8.17 |
| 6000 |
2182 |
268 |
1398 |
8.20 |
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*HP at full throttle - engine air inlet temp
was 130o F from engine compartment - very little air through
engine compartment during static tests. Cooling was provided by spraying
water over the radaitor.
**Based on formula
Thrust = K x (HP x diameter)0.67
K of 7.63 is considered a good value for propellers
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The rest of the time was spent testing the rotor and
modifying the rotor in an attempt to obtain a smooth stable rotor throughout
its operating range (75 - 425 RPM). All 4 of the tests pilots were here
at different times to become more familiar with the operation of the aircraft,
make suggestions to improve safety, and help with the testing of the rotor.
Some of the modifications made to the rotor include:
- Adding an additional 10 lbs. of nose weight to
each blade in an attempt to move the blade dynamic center of mass ahead
of the blade aerodynamic center. Rotor could be forced into a blade
weave with a rapid cyclic stick jab above 275 RPM. We were not able
to excite the blade weave on the test stand, because the cyclic was
locked out and very stiff.
- After adding the weight to the blades, the rotor
developed an instability above 150 RPM. We attempted several things
such as preloading the cyclic control system to remove its deadband
and adding an inertia bar to provide some gyroscopic stability to the
spindle - none of which made much of an improvement. Several helicopter
rotor experts reviewed the test data and while they identified some
1,2,3, 4 and some fractional per rev oscillations at the point of instability.
They could not provide any conclusive information as to what was causing
the problem.
- Perhaps the rotor C.G. was still behind the rotor
AC - hard to believe because the same analysis approach had been accurate
on the 33-1/2 ft. diameter rotor. Nevertheless, on two different occasions
a trailing edge extension was added to the blades. The last extension
was 4 inches long and ran from station 114 to the blade tip at station
260. Neither extension made any improvement.
We noted the mast lateral frequency was at the same
RPM as the rotor instability, but since it was heavily damped, we felt
something else must be exciting the rotor. We measured the natural frequency
of some of the other systems. 1) The natural frequency of the rotor/cyclic
control system was measured at various rotor coning angles (various blade
CG locations relative to the spindle tilt axis) and found that at zero
coning, a no lift prerotating mode, a 1/3 multiple of its frequency occurred
near the rotor instability RPM. Note as the coning angle increased (i.e.
the rotor CG approached the spindle tilt axis) the frequency increased
significantly. We tried running the rotor with increasing collective angles
(rotor CG closer to the spindle tilt axis) without much of an improvement.
2) The blade torsional frequency was checked and found it started at 750
CPM (cycles per minute) and peaked at 920 CPM. ¼ of this 750 CPM (188
RPM) was near the rotor instability RPM. We also noticed that when the
rotor started to go unstable, we saw a 4 per rev load developing in the
cyclic control linkage. We are now adding +/-45 degree carbon cloth to
the outside of the blades in select areas to increase the blade's natural
frequency.
There is no way we can avoid going through some component's
natural frequency as the rotor RPM varies, but to have 3 systems (mast
side to side, rotor/cyclic linkage, and blade torsional) with nearly the
same frequency is a disaster. Adding weight to the blade to move its CG
forward lowered its torsional natural frequency and apparently caused
its new natural frequency to coincide with the other frequencies.
The aircraft is ready to fly once we are able to assure
ourselves we do not have any known rotor diverging oscillations/instabilities.
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