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Linear Algebra, 2020a

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486 Chapter Five. Similarity<br />

That equation is quadratic in ω 2 . Apply the formula to solve quadratic equations,<br />

(−b ± √ b 2 − 4ac)/(2a).<br />

√<br />

ω 2 = 2ω2 0 ± 4ω 4 0 − 4(ω4 0 − ɛ2 /4mI)<br />

= ω 2 0 ± ɛ<br />

2<br />

2 √ mI<br />

The value ɛ/ √ mI = ɛ/ √ κk is often written ω B so that ω 2 = ω 2 0 ± ω B/2. This<br />

is the beat frequency, the difference between the two normal mode frequencies.<br />

Although the argument is beyond our scope, the general formula for the<br />

motion of the pendulum is a linear combination of the motions during the normal<br />

modes. Thus, the pendulum’s motion is entirely determined by the eigenvalues<br />

of the above matrix. See [Berg & Marshall].<br />

Exercises<br />

1 Use the formula for the cosine of a sum to give an even more general formula for<br />

simple harmonic motion.<br />

2 Find the eigenvectors associated with the eigenvalues.<br />

3 Find the values of ω in the case where x(t) =A 1 cos(ωt+φ) and θ(t) =A 2 cos(ωt+<br />

(φ + π)).<br />

4 Build a Wilberforce pendulum out of a Slinky Jr and a soup can. You can drill<br />

holes in the can for bolts, either two or four of them, that you can use to adjust<br />

the moment of inertia of the can so the periods of vertical and rotational motion<br />

coincide.

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