/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 17 A flywheel having constant angul... [FREE SOLUTION] | 91Ó°ÊÓ

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A flywheel having constant angular acceleration requires \(4.00 \mathrm{~s}\) to rotate through 162 rad. Its angular velocity at the end of this time is \(108 \mathrm{rad} / \mathrm{s}\). Find (a) the angular velocity at the beginning of the 4.00 s interval; (b) the angular acceleration of the flywheel.

Short Answer

Expert verified
a) \( \omega_0 = -27 \text{ rad/s} \); b) \( \alpha = 33.75 \text{ rad/s}^2 \).

Step by step solution

01

Understanding the Problem

We are given that the flywheel rotates through 162 radians in 4 seconds with a final angular velocity of 108 rad/s. We need to find the initial angular velocity and the angular acceleration. We will use equations of motion for uniformly accelerated rotation.
02

Use the Angular Displacement Equation

The equation for angular displacement \( \theta \) when the angular acceleration \( \alpha \) is constant is given by:\[\theta = \omega_0 t + \frac{1}{2} \alpha t^2\]where \( \theta = 162 \text{ rad} \), \( t = 4 \text{ s} \), \( \omega_0 \) is the initial angular velocity, and \( \alpha \) is the angular acceleration.
03

Use the Angular Velocity Equation

The final angular velocity \( \omega \) is given by:\[\omega = \omega_0 + \alpha t\]where \( \omega = 108 \text{ rad/s} \). We now have two equations with two unknowns: \( \omega_0 \) and \( \alpha \).
04

Solve for Angular Acceleration (\( \alpha \))

From the second equation, solve for \( \alpha \):\[108 = \omega_0 + 4\alpha\]\[\alpha = \frac{108 - \omega_0}{4}\]
05

Substitute and Solve for Initial Angular Velocity (\( \omega_0 \))

Substitute \( \alpha \) from Step 4 into the first equation:\[162 = \omega_0(4) + \frac{1}{2}\left(\frac{108-\omega_0}{4}\right)(16)\]Simplify and solve for \( \omega_0 \):\[162 = 4\omega_0 + 2(108 - \omega_0)\]\[162 = 4\omega_0 + 216 - 2\omega_0\]\[162 = 2\omega_0 + 216\]\[2\omega_0 = 162 - 216 = -54\]\[\omega_0 = \frac{-54}{2} = -27 \text{ rad/s}\]
06

Confirm and Solve for Angular Acceleration (\( \alpha \))

Use the value of \( \omega_0 \) to find \( \alpha \):\[\alpha = \frac{108 - (-27)}{4}\]\[\alpha = \frac{135}{4} = 33.75 \text{ rad/s}^2\]
07

Verify the Solution

Verify both results by substituting back into the original equations to ensure consistency. Check if: \( 162 = -27(4) + \frac{1}{2}(33.75)(4^2) \) holds true.

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Key Concepts

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

Angular Acceleration
Angular acceleration is all about how quickly the angular velocity of an object changes with time. It’s much like the way linear acceleration works, but instead of speed changing, it’s the rotational speed that changes.
Angular acceleration is denoted by the symbol \( \alpha \) and is measured in radians per second squared (\( \text{rad/s}^2 \)). When an object spins faster or slower, it is accelerating, leading to either positive or negative angular acceleration.
Generally, angular acceleration occurs in scenarios such as spinning wheels, rotating planets, or anything else that turns around a point. If an object's angular velocity increases, it's experiencing positive angular acceleration. Conversely, if it slows down, the angular acceleration is negative.
Angular Velocity
Angular velocity is a measure of how fast an object rotates or spins around in circles. Picture a wheel intersected by lines. As the wheel spins, the lines sweep out angles, and angular velocity tells us how fast those angles are changing.
In physics, angular velocity is often denoted by \( \omega \) and measured in radians per second (\( \text{rad/s} \)). It's similar to linear velocity, which tells us how fast something moves in a straight line. But instead, it tells us about rotation.
With constant angular velocity, the object spins at a consistent speed without speeding up or slowing down. However, in our flywheel problem, the angular velocity changes over time, indicating that it is experiencing angular acceleration.
Equations of Motion
Equations of motion are a set of formulas used in physics to predict the future state of a moving object under constant acceleration. They are crucial tools for solving rotational motion problems.
For angular motion, the main equations include:
  • Angular Displacement: \( \theta = \omega_0 t + \frac{1}{2} \alpha t^2 \)
  • Angular Velocity: \( \omega = \omega_0 + \alpha t \)
In our context of the flywheel, these equations help determine the initial angular velocity \( \omega_0 \) and angular acceleration \( \alpha \).
By understanding these, you can break down even the most complex problems into simpler arithmetic calculations, making problem-solving more manageable.
Physics Problem Solving
Physics problem solving is like piecing together a puzzle—each piece of information adds to the complete picture. The challenge is in identifying which pieces of information to use and in what order.
In any physics problem, like the flywheel example, start by understanding the problem and identifying the known and unknown variables. Next, choose the appropriate equations that relate these variables, like those provided in the equations of motion.
Solving these equations usually involves algebraic manipulations. To prevent errors:
  • Substitute the known values accurately.
  • Consistently check units and calculations.
  • Verify the solution by reconsidering the physics of the problem.
In essence, approach each problem methodically and verify your results by back-substitution to ensure consistency, just like with our flywheel exercise.

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Most popular questions from this chapter

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