I'm sure there's a Dr. Dave page illustrating the details of this.
I didn't, but now I have a video. Check it out:
Thank you again for letting me use your excellent illustration.
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I'm sure there's a Dr. Dave page illustrating the details of this.
A major point in the video is that the situation where the effect comes into play is very rare because usually you can use cut to help the throw and the throw you can get from the double spin transfer is slight -- much smaller than CIT. You have to work really hard to isolate the effect.I didn't, but now I have a video. Check it out: ...
i was waiting for an example of using cut and spin to manipulate the direction. Otherwise, great videoI didn't, but now I have a video. Check it out:
Thank you again for letting me use your excellent illustration.
A major point in the video is that the situation where the effect comes into play is very rare because usually you can use cut to help the throw and the throw you can get from the double spin transfer is slight -- much smaller than CIT. You have to work really hard to isolate the effect.
A situation that is similar is when you have three balls in line. Can the third ball be thrown? If so, which way?
i was waiting for an example of using cut and spin to manipulate the direction.
Thanks.Otherwise, great video
You did a great job! Broke it down to its components, structured it as a quiz, revealed the answer, and shown it all in practical on-the-table circumstances.I didn't, but now I have a video. Check it out:
Thank you again for letting me use your excellent illustration.
You did a great job! Broke it down to its components, structured it as a quiz, revealed the answer, and shown it all in practical on-the-table circumstances.
I believe OB2 always heads in the same direction as CB spin. Here is the reasoning. With a head-on collision of the CB onto OB1 with sidespin, OB1 receives some friction impulse, say its horizontal (Using MattPoland’s diagram ) component is J. Then using the linear momentum equation, OB1 has horizontal velocity J/m, while (angular momentum equation) it has angular velocity 5/2J/(mr). OB2’s direction is entirely determined by the relative sliding between OB1 and OB2. Now the point on OB1, touching OB2, has translational velocity J/m, and some velocity provided by the rotation, which is 5/2 J/(mr) * r. Since OB1’s induced spin and throw has opposite direction (when viewed from the point of view of the contact point on the surface), the combined velocity is (5/2-1)J/m = 3/2 J/m, always in the sidespin (induced from CB spin) direction of CB. I feel like this is the correct analysis. So OB2 always throws in the same direction as CB spin, it’s just a matter of how much CB2 throws in the direction of CB spin.