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Selected Topics in Classical Mechanics. Topic I: Rotation of a Hanging Chain. The first topic I will describe is equilibrium configurations of a heavy, inextensible chain (or rope) which is suspended from one end and free to rotate about the vertical axis through the point of suspension. The chain has no stiffness and no torsional degrees of freedom. The point of suspension is the upper end, and the other end of the chain is the lower end. Case 1: the classical helicoseir. I will also consider the case t...

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Helicoseir | mathphys.net Reviews
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Selected Topics in Classical Mechanics. Topic I: Rotation of a Hanging Chain. The first topic I will describe is equilibrium configurations of a heavy, inextensible chain (or rope) which is suspended from one end and free to rotate about the vertical axis through the point of suspension. The chain has no stiffness and no torsional degrees of freedom. The point of suspension is the upper end, and the other end of the chain is the lower end. Case 1: the classical helicoseir. I will also consider the case t...
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Helicoseir | mathphys.net Reviews

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Selected Topics in Classical Mechanics. Topic I: Rotation of a Hanging Chain. The first topic I will describe is equilibrium configurations of a heavy, inextensible chain (or rope) which is suspended from one end and free to rotate about the vertical axis through the point of suspension. The chain has no stiffness and no torsional degrees of freedom. The point of suspension is the upper end, and the other end of the chain is the lower end. Case 1: the classical helicoseir. I will also consider the case t...

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The solutions of the quadratic equation. Are usually given as. But an equally valid formula is. For each root, one formula suffers a cancellation error, and the other formula does not.

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Selected Topics in Classical Mechanics. Topic I: Rotation of a Hanging Chain. The first topic I will describe is equilibrium configurations of a heavy, inextensible chain (or rope) which is suspended from one end and free to rotate about the vertical axis through the point of suspension. The chain has no stiffness and no torsional degrees of freedom. The point of suspension is the upper end, and the other end of the chain is the lower end. Case 1: the classical helicoseir. I will also consider the case t...

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