/*! 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 67 An electric fan is running on HI... [FREE SOLUTION] | 91Ó°ÊÓ

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An electric fan is running on HIGH. After the LOW button is pressed, the angular speed of the fan decreases to \(83.8 \mathrm{rad} / \mathrm{s}\) in \(1.75 \mathrm{s}\). The deceleration is \(42.0 \mathrm{rad} / \mathrm{s}^{2} .\) Determine the initial angular speed of the fan.

Short Answer

Expert verified
The initial angular speed of the fan is 157.3 rad/s.

Step by step solution

01

Identify Known and Unknown Variables

We are given the final angular speed \( \omega_f = 83.8 \, \text{rad/s} \), the time taken for the deceleration \( t = 1.75 \, \text{s} \), and the angular deceleration \( \alpha = 42.0 \, \text{rad/s}^2 \). The initial angular speed \( \omega_i \) is unknown and needs to be found.
02

Use the Angular Motion Formula

We can use the formula for angular motion: \( \omega_f = \omega_i + \alpha \cdot t \). This formula relates the initial angular speed, the final angular speed, the angular deceleration, and the time over which the deceleration occurs.
03

Rearrange the Formula to Solve for Initial Angular Speed

Rearrange the formula to solve for \( \omega_i \): \( \omega_i = \omega_f - \alpha \cdot t \). This will allow us to find the initial angular speed using the given values.
04

Substitute the Known Values

Substitute the given values into the formula: \( \omega_i = 83.8 \, \text{rad/s} - 42.0 \, \text{rad/s}^2 \cdot 1.75 \, \text{s} \).
05

Calculate the Initial Angular Speed

Calculate the initial angular speed using the substituted values: \( \omega_i = 83.8 \, \text{rad/s} - 73.5 \, \text{rad/s} \). Thus, \( \omega_i = 157.3 \, \text{rad/s} \).

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Key Concepts

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

Understanding Angular Speed
Angular speed is an essential concept when studying rotational motion. It describes how quickly an object rotates or spins around a specific point or axis. Essentially, it tells us how fast an angle is changing in a given period of time.
  • Angular speed is often represented by the letter \( \omega \) (omega).
  • It is measured in radians per second (rad/s), which is the standard unit used in physics.
The concept of angular speed is very similar to linear speed; however, instead of measuring the distance traveled over time, it measures the angle turned over time. Imagine an electric fan – the angular speed would indicate how quickly the fan blades spin around its axis.
Understanding angular speed can help us determine how fast something revolves and predict how long it takes to complete one full rotation.
What is Angular Deceleration?
Angular deceleration is the rate at which an object's angular speed decreases. It's essentially angular acceleration in the opposite direction of motion, causing the object to slow down.
  • Angular deceleration is also represented by the symbol \( \alpha \).
  • It uses the same units as angular acceleration, radians per second squared (rad/s²).
In the context of the electric fan, angular deceleration would be the process of the fan blades gradually slowing down when you press the low button.
Angular deceleration is a crucial concept in rotational dynamics because it helps in understanding how and why an object slows down over time. This principle comes into play in various practical applications, such as vehicles braking or machinery gradually coming to a stop.
Finding the Initial Angular Speed
To determine how fast an object was rotating at the start, we calculate its initial angular speed. In our electric fan example, this means finding out how quickly the fan blades were spinning before you pushed the button to slow it down.
The formula to find the initial angular speed is crucial and quite straightforward:
  • Use the equation \( \omega_i = \omega_f - \alpha \cdot t \)
  • Here, \( \omega_i \) is the initial angular speed, \( \omega_f \) is the final angular speed, \( \alpha \) is the angular deceleration, and \( t \) is the time over which the deceleration occurs.
By substituting the known values into the formula, we can solve for \( \omega_i \), the initial angular speed. In our problem, by implementing the formula, we found that the fan's initial angular speed was \( 157.3 \text{ rad/s} \).
Understanding how to determine the initial angular speed is vital for analyzing any motion that involves somebody or something rotating or spinning. It allows us to look back at the system's initial conditions and gauge how they affected its later states.

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Most popular questions from this chapter

A racing car, starting from rest, travels around a circular turn of radius \(23.5 \mathrm{m}\). At a certain instant, the car is still accelerating, and its angular speed is \(0.571 \mathrm{rad} / \mathrm{s}\). At this time, the total acceleration (centripetal plus tangential) makes an angle of \(35.0^{\circ}\) with respect to the radius. (The situation is similar to that in Interactive Figure \(8.12 b .\) ) What is the magnitude of the total acceleration?

Conceptual Example 2 provides some relevant background for this problem. A jet is circling an airport control tower at a distance of \(18.0 \mathrm{km}\) An observer in the tower watches the jet cross in front of the moon. As seen from the tower, the moon subtends an angle of \(9.04 \times 10^{-3}\) radians. Find the distance traveled (in meters) by the jet as the observer watches the nose of the jet cross from one side of the moon to the other.

The earth spins on its axis once a day and orbits the sun once a year \(\left(365 \frac{1}{4}\right.\) days \()\) Determine the average angular velocity (in rad/s) of the earth as it (a) spins on its axis and (b) orbits the sun. In each case, take the positive direction for the angular displacement to be the direction of the earth’s motion.

The angular speed of the rotor in a centrifuge increases from 420 to \(1420 \mathrm{rad} / \mathrm{s}\) in a time of \(5.00 \mathrm{s}\). (a) Obtain the angle through which the rotor turns. (b) What is the magnitude of the angular acceleration?

A propeller is rotating about an axis perpendicular to its center, as the drawing shows. The axis is parallel to the ground. An arrow is fired at the propeller, travels parallel to the axis, and passes through one of the open spaces between the propeller blades. The angular open spaces between the three propeller blades are each \(\pi / 3\) rad \(\left(60.0^{\circ}\right) .\) The vertical drop of the arrow may be ignored. There is a maximum value \(\omega\) for the angular speed of the propeller, beyond which the arrow cannot pass through an open space without being struck by one of the blades. Find this maximum value when the arrow has the lengths \(L\) and speeds \(v\) shown in the following table. $$ \begin{array}{lll} & L & v \\ (\mathrm{a}) & 0.71 \mathrm{m} & 75.0 \mathrm{m} / \mathrm{s} \\ \hline(\mathbf{b}) & 0.71 \mathrm{m} & 91.0 \mathrm{m} / \mathrm{s} \\ \hline(\mathbf{c}) & 0.81 \mathrm{m} & 91.0 \mathrm{m} / \mathrm{s} \\ \hline \end{array} $$

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