Table of Contents
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V. CONCLUSIONS
We have experimentally demonstrated the differential
rotation of a pulsed jet that radially expands in a rotating frame.
We chose less shear in the Ωdifferential case than will be
used in the liquid sodium experiment to measure the pulsed jet
rotation because of the stated difficulties in obtaining accurate flow
visualization images. We believe that we have shown that there is
more rapid jet rotation in the Ωdifferential case than in
the Ω = const case. The partial entrainment of the jets with
the background flow leads to a drag on differential rotation in the
case of Ω = const flow and to an acceleration of differential
rotation of the pulsed jet in an Ωdifferential rotating
frame. We presume that this is due to turbulent entrainment in the
sheared flow field and so we should expect a still more enhanced
effect in the sodium experiment where the shear is still greater. The
final determination of the effective α-effect will have to be
done magnetically or with 3-D numerical modeling with Re > 104 and
Remag > 200. We believe that an understanding of Eq. (5) is
substantiated.
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