On a compact disc (CD), music is coded in a pattern of tiny pits arranged in a track that spirals outward toward the rim of the disc. As the disc spins inside a CD player, the track is scanned at a constant $linear$ speed of $v =$ 1.25m/s. Because the radius of the track varies as it spirals outward, the angular speed of the disc must change as the CD is played. (See Exercise 9.20.) Let's see what angular acceleration is required to keep $v$ constant. The equation of a spiral is $r(\theta) = r_0 + \beta\theta$, where $r_0$ is the radius of the spiral at $\theta =$ 0 and $\beta$ is a constant. On a CD, $r_0$ is the inner radius of the spiral track. If we take the rotation direction of the CD to be positive, $\beta$ must be positive so that $r$ increases as the disc turns and $\theta$ increases. (a) When the disc rotates through a small angle $d\theta$, the distance scanned along the track is $ds = rd\theta$. Using the above expression for $r(\theta)$, integrate $ds$ to find the total distance $s$ scanned along the track as a function of the total angle $\theta$ through which the disc has rotated. (b) Since the track is scanned at a constant linear speed $v$, the distance s found in part (a) is equal to $vt$. Use this to find $\theta$ as a function of time. There will be two solutions for $\theta$ ; choose the positive one, and explain why this is the solution to choose. (c) Use your expression for $\theta(t)$ to find the angular velocity $\omega_z$ and the angular acceleration $\alpha_z$ as functions of time. Is $\alpha_z$ constant? (d) On a CD, the inner radius of the track is 25.0 mm, the track radius increases by 1.55 mm per revolution, and the playing time is 74.0 min. Find $r_0, \beta,$ and the total number of revolutions made during the playing time. (e) Using your results from parts (c) and (d), make graphs of $\omega_z$ (in rad/s) versus $t$ and $\alpha_z$ (in rad/s$^2$) versus $t$ between $t =$ 0 and $t =$ 74.0 min. $\textbf{The Spinning eel.}$ American eels ($Anguilla$ $rostrata$) are freshwater fish with long, slender bodies that we can treat as uniform cylinders 1.0 m long and 10 cm in diameter. An eel compensates for its small jaw and teeth by holding onto prey with its mouth and then rapidly spinning its body around its long axis to tear off a piece of flesh. Eels have been recorded to spin at up to 14 revolutions per second when feeding in this way. Although this feeding method is costly in terms of energy, it allows the eel to feed on larger prey than it otherwise could.