Item 0682
OTHER:
Flight Dynamics - General - Pitch-Lag Coupling, (δ2) ? (δ4)![]()
See also:
OTHER: Flight Dynamics - General - Lead-Flap Coupling, for Intermeshing Rotors (kpβ) & Pitch-Lag Coupling![]()
Notes:
Consider the "lean" of the hinge X-axis and/or y-axis.
Increase in a Rotor's RRPM Due to Coning:
The following is from
OTHER: Flight Dynamics - General - Lead-Flap Coupling, for Intermeshing Rotors (kpβ) & Pitch-Lag CouplingThe following may be revised for Pitch-Lag. For Electrotor-SloMo - coaxial
To calculate the increase in a blade's rotational velocity when it teeters (flaps) up or down from the plane where the blade's mass is normal to the (virtual) teetering hinge on the mast's axis. I.e. maintaining the
kinetic energy when the radius of the blade's mass is reducedThe
kinetic energy in a helicopter's rotor is not changed by a change in the coning angle.Kinetic energy;
(EKR) [ft-lbs] = (1/2) * JMO * ω 2Polar moment of inertia;
(JMO) [slug-ft2] = m * r2ω
= angular velocity [radians/second]m
= mass [slugs]r
= radius to center of blade's mass [ft]Subscript
(S ) is for the Start values (no cone or smaller cone).Subscript
(E ) is for the End values (greater cone).If the tip path plane is down at the front then
(S ) will be for 90º and 270º azimuths, and (E ) will be for 0º and 180º azimuths.Since the kinetic energy does not change;
EKR = (1/2) * JMO S * ωS 2 = (1/2) * JMO E * ωE 2Divide both sides by 1/2;
JMO S * ωS 2 = JMO E * ωE 2Polar moment of inertia equals mass time radius squared;
JMO = m * r2Therefore;
m S * rS 2 * ωS 2 = m E * rE 2 * ωE 2And since the mass does not change;
rS 2 * ωS 2 = rE 2 * ωE 2Rearranged;
ω E 2 = (rS 2 / rE 2)* ω S 2Symbol for the flap angle
β (in degrees).Since the change in the radius is cosine of the Start angle
βS minus the cosine of the End angle βE(rS 2 / r E 2) = (cosβ S 2 / cosβ E 2)
Therefore;
ω E 2 = (cosβ S 2 / cosβ E 2)* ω S 2and, if the initial flapping angle is zero (ie. the tip path plane and the mast plane are parallel, then,
ω
E 2 = (1 / cosβ E 2)* ω S 2and, assigning the initial rotational speed a value of 1, then,
ω
E 2 = (1 / cosβ E 2)* 1ω
E 2 = 1 / cosβ E 2Therefore,
ω E is the multiplier of ω S to obtain the rotational speed of the blade at the increased cone [in radians/second]___________________
Example, if the cone angle, in the vertical plane of the blade azimuth,
(β S) is 0º, (β E) is 10º, is 45ºthen
cosβ E is 0.9848, is 0.7071then
cosβ E 2 is 0.9698, is 0.5000then
ω E 2 is 1 / 0.9698 = 1.0311, is 1 / 0.5000 = 2.0000and
ω E is √1.0311 = 1.0154 * ω S, √2.0000 = 1.4142 * ω S,This means that the rotor's rpm is 01.54% faster when the coning angle has been changed from 0º to 10º.
This means that the rotor's rpm would be 41.42% faster if the conning angle was changed from 0º to 45º.In one revolution, 360º, the rotor will be
1.54% * 360 = 5.544º further advanced than it will be if the conning angle is 0º.Considering only 90º of rotation, the rotor will have advanced
5.544º / 4 = 1.386ºThis means that the maximum relative force (torque (
Q)) is sin(10º), which is 0.1737. This torque will vary from 0.0, to +0.1737, to 0.0 to -0.1737 during a single cycle.The following table will probably be more accurate if the rows went from 0 to 10 and then the values of 5 and 10 are used
|
|
Pitch in deg. |
Relative Torque(1) |
Relative Acceleration ??? (2) |
|
|
0.5 |
0.0087 |
0.0087 |
|
|
1.5 |
0.0262 |
0.0349 |
|
|
2.5 |
0.0436 |
0.0785 |
|
|
3.5 |
0.0610 |
0.1395 |
|
|
4.5 |
0.0785 |
0.2180 |
|
|
5.5 |
0.0958 |
0.3138 |
|
|
6.5 |
0.1132 |
0.4270 |
|
|
7.5 |
0.1305 |
0.5575 |
|
|
8.5 |
0.1478 |
0.7053 |
|
|
9.5 |
0.1650 |
0.8703 |
|
|
Sum |
0.8703 |
|
|
|
Average |
0.0870 |
|
(1) This is just the sine of the angle
(2) This is just a running sum of the relative Torques.
The mean lead advancement in 90º of rotation is (0.2180 /0.8703) * 1.386º = 0.3472º
![]()
Rotary Motion w/ Constant Acceleration:
(from Machinery Handbook p.151)Angle of rotation (
Initial angular velocity (
ωO) () 360º * 0.01745 = 6.282 [radians per second]Final angular velocity (
ωF) () 6.282 * 1.0154 = 6.3825 [radians per second]Angular acceleration (
α) () [radians, per second, per second] α = (ωF - ωO2) / 2θ|
|
α = (ωF - ωO2) / 2θ |
|
|
α = (6.3825 - 6.282 2) / ( 2 * 1.5705) |
|
|
α =250.6925 / 3.141 |
|
|
α = 79.8130 |
Time (
t) [in seconds] t = 2θ / (ωF + ωO)|
|
t = 2 θ / (ωF + ωO) |
|
|
t = ( 2 * 1.5705) / (6.3825 + 6.282) |
|
|
t = 3.141 / 12.6645 |
|
|
t = |
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From the above graph, it looks like the delta3 angle should be 21.8885º
If the calculations are incorrect, consider having delta3 by flap hinge geometry at 40º and delta3 by control system geometry at - 25º for at 40º flap - lead/lag and a 15º flap - pitch
~ or ~
Perhaps excessive lead will cause other problems with the rotor, particularly because it is the blade tip that is leading, not the whole blade or the whole rotor. ~ or ~ Perhaps Kaman could not have a hub with combined delta3s because his pitch mechanism was inside the hub and it operates a flap not a pitch horn. Note that the Kaman's lead/lag hinges, like others, causes the top to lead.
![]()
15° Offset Teetering Hinge: (ref. Pitch-Teeter Coupling - delta3)
Using flap hinge geometry (type A).
______________________________________
I believe that operational activity is as follows;
______________________________________
Calculation Method 1 and Calculation Method 2 give 2 different values. 1 is twice 2. One or both have a problem or misunderstanding. See:
OTHER: Flight Dynamics - General - delta3 (pitch-flap coupling) for the same concern.Calculation Method 1:

It looks like a change of 15 to 16 degrees in the teetering hinge will cause the blades to advance the correct amount to handle lead-lag. This action also causes a decrease in the input pitch angle.
In the following, a 10° of flap and a 15° teetering angle will advance the blade 0.8015" but cause a 2.68° decrease in pitch angle.
See the lower portion of the drawing for elaboration;
It may be more accurate to base the above calculations on inertia
OTHER: Flight Dynamics - General - Rotor Inertia instead of radius, because speed is to a power_____________________________________
See the upper portion of the drawing.
The elevation etc., in respect to the teetering axis, of the connection between the horizontal pitch horn and the vertical pitch link may offer the opportunity to vary the resultant actions.
![]()
zeta = X - Y
In the above, a 10° of teeter (flap)
beta and a 15° delta3 will advance the blade 0.221 degrees_____________________________________
There's a discrepancy between the above methods 1 & 2.
Also, I do not know if the delta3 angle should be 15.5 degrees, 45 degrees or some other value.
Note that the Kaman appears to be about 15ºFor more information on delta3 see: [
OTHER: Flight Dynamics - General - Pitch-Flap Coupling (delta3)]For variation of RRPM caused by cyclical Coriolis / Knuckle joint effect see:
DESIGN: Rotor - Disk - Semi-rigid TeeteringTo run calculations see:
FORM: Rotor - Disk - delta3 ![]()
Other Web Page at this Site on Auto-Collective ~ Torque Pitch
Note: The total weight, which varies according to the weight of the pilot, will probable effect the RRPM-Pitch-Torque balance. Can it be pre-flight adjustable to suit each flight?
OTHER: Miscellaneous - Thoughtless Ideas - Torque/Pitch Collective Rotor Hub
OTHER: Miscellaneous - Thoughtless Idea - Constant Speed Rotor
OTHER: Flight Dynamics - General - Cross-Coupling # Torque-Pitch
OTHER: Flight Dynamics - General - Lead-Flap Coupling, for Intermeshing Rotors & Pitch-Lag Coupling
OTHER: Flight Dynamics - General - Pitch-Lag Coupling
DESIGN: Single-Bladed All Electric Rotor- Rotor Hub - Pitch-Torque Coupling
DESIGN: Electrotor-Simplex ~ Rotor - Hub - Overview of Gimbaled w/ Torque Collective B
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Last Revised: December 13, 2009