Aero

John Cipolla offers a great computer program called FinSim that allows one t' do structural, me bucko, aerodynamic and aeroelastic analysis o' rocket fins. Avast! Equally impressive is his discussion located on t' FinSim Website and t' link t' a paper describin' t' details o' t' fin flutter and divergence method. Begad! Arrr! Mr. Ahoy! Cipolla wisely suggests that when usin' FinSim t' estimate flutter velocity, me bucko, one should bound t' flutter prediction by usin' t' theoretical 2-dimensional lift coefficient (2 pi ) t' establish a lower bound and t' 3-dimensional lift coefficient t' establish an upper bound. Avast! Aye aye! Most likely t' flutter velocity will fall betwixt these two extremes.

T' purpose o' this review is t' put an emphasis on Mr. Aye aye! Cipolla's advice and t' suggest that t' lower bound be taken more seriously as a means t' design fins that will nay flutter.

There are two technical reasons that support this position, namely model (equation) applicability and t' neglect o' t' natural frequency in plunging. Well, blow me down! Both result in t' reduction o' a rather complex problem into a simple relation t' predict flutter velocity. These simplifications result in an incremental over-prediction o' flutter speed. Well, blow me down! T' more conservative approach o' usin' t' 2-dimensional lift-coefficient disguises t' effects o' these approximations. Ahoy! If I have peaked your interest, then please read on for further explanation.

T' approach used in FinSim is known as a quasi-steady approximation t' predictin' flutter speed. Arrr! This approximation assumes that t' frequency o' vibration (oscillation) is small relative t' t' linear flight speed o' t' rocket. Ya scallywag! Ahoy! This relationship is often described as a reduced frequency given by t' simple equation:

Reduced (normalized) frequency o' vibration

Where,

Frequency o' Vibration, shiver me timbers, Hz

Average Chord o' Fin, me bucko, unit-of-length

Linear Rocket Velocity, unit-of-length per second

T' quasi-steady approximation is considered valid when t' reduced frequency is small, me bucko, me bucko, that is when k.<= 0.1 This is rarely t' case for subsonic flow (Mach number less than ~0.8). T' quasi-steady approximation is best suited for t' prediction o' flutter speed in supersonic flow, me hearties, or for use in design studies where trends are o' interest rather than an accurate prediction o' flutter speed.

T' quasi-steady equation for flutter speed in FinSim relates t' flutter speed as directly proportional t' t' natural frequency in torsion (twist) and neglects any effect due t' t' natural frequency in plungin' (bending). Well, blow me down! Again, this assumption results in an incremental over-prediction o' flutter speed. Arrr! T' error can be minor or quite significant, arrr, dependin' on t' magnitude o' t' square o' t' natural frequency in plungin' relative t' t' magnitude t' t' square o' t' natural frequency in torsion. Avast! T' error tends t' increase as fin aspect ratio and taper ratio decrease. Ahoy! Begad! If t' natural frequency in plungin' were accounted for in t' quasi-steady approximation, me hearties, then t' flutter speed would be proportional t' t' square root o' t' difference in t' square o' t' natural frequencies, that is:

T' %-error due t' this approximation alone is calculated as follows:

In conclusion, arrr, t' additive error o' these two approximations could result in a significant over-prediction o' t' actual flutter speed, particularly if one were t' base their calculation on a lift-coefficient corrected for 3-dimensional effects.