The contour s 1,2 contribute to the asymptotics at plus and minus infinities, respectively.
The condition at infinity can be determined as if the harbour were absent.
If the rotation axis is passive, the coefficient of elasticity for axial rotation is almost zero and is close to infinity.
First, one may simply run ever more trials, and approach the infinity limit ever more closely.
When s or c take values close to unity, the fluid at infinity is rotating with nearly the same angular velocity as the disk.
According to this understanding of infinity, the in-finite is limitless.
The equations for incompressible fluids can then be immediately obtained by letting the sound velocity approach infinity.
I will now show that there is generally an infinity of efficient taking-it-in-turns equilibria if there are any at all.
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