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A computer disk drive is turned on starting from rest and has constant angular acceleration. If it took 0.0865 s for the drive to make its \(second\) complete revolution, (a) how long did it take to make the first complete revolution, and (b) what is its angular acceleration, in rad/s\(^2\)?

Short Answer

Expert verified
(a) 0.0611 s; (b) 3386.52 rad/sĀ².

Step by step solution

01

Understanding the Problem

We are given that a disk drive starts from rest with constant angular acceleration and takes 0.0865 s to complete its second revolution. We need to calculate the time taken for the first revolution and the angular acceleration.
02

Using the Angular Kinematics Formula

The equation for angular displacement under constant angular acceleration is \( \theta = \omega_i t + \frac{1}{2} \alpha t^2 \). Since it starts from rest \( \omega_i = 0 \) and the angle for one revolution is \( 2\pi \) radians.
03

Writing Equations for First and Second Revolutions

For the first revolution, \( 2\pi = \frac{1}{2} \alpha t_1^2 \). For the first and second revolutions combined, \( 4\pi = \frac{1}{2} \alpha t_2^2 \). We know \( t_2 = t_1 + 0.0865 \) s.
04

Solving for Angular Acceleration

We can solve the equations simultaneously to find \( \alpha \), the angular acceleration. Substituting \( t_2 = t_1 + 0.0865 \) into the second equation: \( 4\pi = \frac{1}{2} \alpha (t_1 + 0.0865)^2 \).
05

Simplifying and Solving for \( t_1 \)

From the first equation: \( \alpha = \frac{4\pi}{t_1^2} \). Substitute into the combined equation gives: \( 4\pi = 2\pi (\frac{t_2^2}{t_1^2}) \), solve for \( t_1 \) gives \( t_1 \approx 0.0611 \) s.
06

Calculating Angular Acceleration

Using \( t_1 \approx 0.0611 \) s in the first formula for \( \alpha \), \( \alpha = \frac{4\pi}{(0.0611)^2} = 3386.52 \text{ rad/s}^2 \).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Constant Angular Acceleration
Understanding constant angular acceleration is crucial to solving this problem. This term describes how an object's rotational speed changes at a constant rate over time. In layman's terms, it means that with each passing second, the disk drive spins faster and faster by the same amount.
For example, if the angular acceleration of the disk is 3386.52 rad/s two, as calculated in the solutions, it means that the rotational speed increases by this amount every second.
  • Constant angular acceleration implies predictable rotational motion.
  • It allows us to use simple equations to solve complex problems.
This concept is akin to linear acceleration in everyday experiences, like a car speeding up at a constant rate.
Angular Kinematics
Angular kinematics involves the equations used to describe rotational motion, similar to linear motion equations used for objects moving in a straight line. Here, however, we're dealing with angles, angular speed, and angular acceleration instead of distances, speeds, and linear accelerations.
The main formula used in this problem is:\[\theta = \omega_i t + \frac{1}{2} \alpha t^2\]where:
  • \(\theta\): Angular displacement (in radians)
  • \(\omega_i\): Initial angular velocity (\(0\) in this problem as it starts from rest)
  • \(\alpha\): Angular acceleration
  • \(t\): Time
This formula is essential to understanding how the drive completes its revolutions, beginning with zero speed and gradually speeding up.
Revolution Timing
Revolution timing refers to the time taken for the disk drive to complete one full spin or revolution. In this scenario, weā€™re examining the timing of both the first and second revolutions.
To find out how long it takes to reach one complete rotation, we need to consider its angular kinematics. The first complete revolution timing calculation uses \(2\pi = \frac{1}{2} \alpha t_1^2\) to find that it took about 0.0611 seconds.
  • The second revolution takes 0.0865 seconds, as given.
  • The difference between the two provides insights into how acceleration impacts timing.
By comparing these times, we can learn about the diskā€™s increasing speed during startup.
Angular Displacement
Angular displacement is the change in position of a point moving along a circular path. It's similar to how linear displacement measures change in position along a straight line, but in a circle, this change is expressed in radians.
For circular revolutions:
  • One complete revolution equals \(2\pi\) radians.
  • Two complete revolutions equal \(4\pi\) radians.
As seen in the exercise, these values are integral to determining the time required and calculating angular acceleration. Angular displacement, observed as \(2\pi\) or \(4\pi\) radians, helps quantify how much the disk has rotated over time. It's the foundation for exploring motion in circular paths.

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Most popular questions from this chapter

A thin uniform rod of mass \(M\) and length \(L\) is bent at its center so that the two segments are now perpendicular to each other. Find its moment of inertia about an axis perpendicular to its plane and passing through (a) the point where the two segments meet and (b) the midpoint of the line connecting its two ends.

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.

You are designing a rotating metal flywheel that will be used to store energy. The flywheel is to be a uniform disk with radius 25.0 cm. Starting from rest at \(t =\) 0, the flywheel rotates with constant angular acceleration 3.00 rad/s\(^2\) about an axis perpendicular to the flywheel at its center. If the flywheel has a density (mass per unit volume) of 8600 kg/m\(^3\), what thickness must it have to store 800 J of kinetic energy at \(t =\) 8.00 s?

Two metal disks, one with radius \(R_1 =\) 2.50 cm and mass \(M_1 =\) 0.80 kg and the other with radius \(R_2 =\) 5.00 cm and mass \(M_2 =\) 1.60 kg, are welded together and mounted on a frictionless axis through their common center (\(\textbf{Fig. P9.77}\)). (a) What is the total moment of inertia of the two disks? (b) A light string is wrapped around the edge of the smaller disk, and a 1.50-kg block is suspended from the free end of the string. If the block is released from rest at a distance of 2.00 m above the floor, what is its speed just before it strikes the floor? (c) Repeat part (b), this time with the string wrapped around the edge of the larger disk. In which case is the final speed of the block greater? Explain.

A meter stick with a mass of 0.180 kg is pivoted about one end so it can rotate without friction about a horizontal axis. The meter stick is held in a horizontal position and released. As it swings through the vertical, calculate (a) the change in gravitational potential energy that has occurred; (b) the angular speed of the stick; (c) the linear speed of the end of the stick opposite the axis. (d) Compare the answer in part (c) to the speed of a particle that has fallen 1.00 m, starting from rest.

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