April 22, 1978 Dear Rufus, The present letter is unrelated to the one I sent you two days ago, and is motivated by "A model for Couette flow data: which you published in the "Berkeley Turbulence Seminar." There is a possible objection to your interpretation of the data which goes as follows. Due to the rotational symmetry of the system, a generic possibility is that the time periodicity corresponding to the frequency; is one purely to the rotation of a configuration of the fluid which is steady in a suitable rotating frame. This is intuitive once you think of it, it can also be proved [Cf. my paper in Arch. Rat. Mech. Anal. 51, 136-152 (1973)]. If another frequency w1 or w2 corresponds to "intrinsic" motion of the fluid, like pulsation, which cannot be ruled out even by going to a rotating reference frame, there is no reason to expect that w2 or w3 will "lock in" with w1. This is because w1 can be changed in an arbitrary manner by going to a suitable rotating reference frame, and that is not true of w1 or w2 To summarize: Depending on the geometry of the system, one expects that locking-in of frequencies will take place or not. I understand that Fenstermacher, Golub, and Swinney are making a new experiment with two laser beams which should throw some light on the geometry of the system. Best regards, David. Copy: H. Swinney J. Golub Let me know if you need further assistance or clarification with this letter. |
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