jgtjr
New member
- Jul 11, 2011
- 2
I am interested in estimating the effect of flow acceleration on the pitching moment of a conventional aft tail monoplane. Often, discussions of this type concern themselves with Mach effects, "Mach tuck" is often used to describe the transonic effects on the horizontal stabilizer generating a nose down Cm about the vehicles CG. However, this seems a quasi steady phenomina.
I am interested in a RATO launch where the vehicle is being linearly accelerated (RATO thrust aligned with the fuselage axis). There is a distinct nose down moment and it doesn't seem likely to be a Mach effect. The vehicle is accelerated from 0.0 to approximately 500 feet per second in 2.5 seconds. The duration of the moment variation lasts for approximately 90% of the flight to 500 fps. I.e. the moment increment asymptotes to zero as the vehicle's speed increases.
In your collective opinions, is it possible that there is an apparent mass effect operating here?
Does anyone have experience with the moments imposed on a fairly rapidly accelerating flight vehicle of conventional layout?
(the horizontal control surface has an 8%, and the wing a 12% thickness to chord ratio)
I am interested in a RATO launch where the vehicle is being linearly accelerated (RATO thrust aligned with the fuselage axis). There is a distinct nose down moment and it doesn't seem likely to be a Mach effect. The vehicle is accelerated from 0.0 to approximately 500 feet per second in 2.5 seconds. The duration of the moment variation lasts for approximately 90% of the flight to 500 fps. I.e. the moment increment asymptotes to zero as the vehicle's speed increases.
In your collective opinions, is it possible that there is an apparent mass effect operating here?
Does anyone have experience with the moments imposed on a fairly rapidly accelerating flight vehicle of conventional layout?
(the horizontal control surface has an 8%, and the wing a 12% thickness to chord ratio)