/*! 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 79 Suppose you are driving a car in... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

Suppose you are driving a car in a counterclockwise direction on a circular road whose radius is \(r=390 \mathrm{m}\) (see the figure). You look at the speedometer and it reads a steady \(32 \mathrm{m} / \mathrm{s}\) (about \(72 \mathrm{mi} / \mathrm{h}\) ). Concepts: (i) Does an object traveling at a constant tangential speed (for example, \(\left.v_{\mathrm{T}}=32 \mathrm{m} / \mathrm{s}\right)\) along a circular path have an acceleration? (ii) Is there a tangential acceleration \(\overrightarrow{\mathbf{a}}_{\mathrm{T}}\) when the angular speed of an object changes (e.g., when the car's angular speed decreases to \(4.9 \times 10^{-2} \mathrm{rad} / \mathrm{s}\) )? Calculations: (a) What is the angular speed of the car? (b) Determine the acceleration (magnitude and direction) of the car. (c) To avoid a rear-end collision with the vehicle ahead, you apply the brakes and reduce your angular speed to \(4.9 \times 10^{-2} \mathrm{rad} / \mathrm{s}\) in a time of 4.0 s. What is the tangential acceleration (magnitude and direction) of the car?

Short Answer

Expert verified
Yes, the car has centripetal acceleration. No tangential acceleration initially, but it decelerates at \(-0.00828 \text{ rad/s}^2\) during braking.

Step by step solution

01

Analyzing Constant Tangential Speed

Yes, an object traveling at a constant tangential speed along a circular path has an acceleration even though the speed doesn't change. This is because the direction of the velocity changes continuously, which means there is centripetal acceleration directed toward the center of the circle.
02

Evaluating Tangential Acceleration

When the angular speed of an object changes, there will be a tangential acceleration. This occurs because there is a change in the magnitude of the tangential velocity, which induces a tangential component of acceleration.
03

Calculating Angular Speed

The angular speed \( \omega \) can be calculated using the relation \( v_T = r \cdot \omega \). Given, the tangential speed \( v_T = 32 \text{ m/s} \) and radius \( r = 390 \text{ m} \), we find:\[ \omega = \frac{v_T}{r} = \frac{32}{390} \approx 0.0821 \text{ rad/s} \]
04

Finding Centripetal Acceleration

Centripetal acceleration \( a_c \) is given by \( a_c = \frac{v_T^2}{r} \). Plugging in the values:\[ a_c = \frac{32^2}{390} \approx 2.63 \text{ m/s}^2 \]The direction is toward the center of the circle.
05

Computing Tangential Acceleration

The tangential acceleration \( a_T \) can be calculated when the angular speed changes using \( a_T = \frac{\Delta \omega}{\Delta t} \). Suppose the initial \( \omega_i = 0.0821 \text{ rad/s} \) and final \( \omega_f = 0.049 \text{ rad/s} \), the time \( \Delta t = 4.0 \text{ s} \):\[ a_T = \frac{0.049 - 0.0821}{4.0} = \frac{-0.0331}{4.0} \approx -0.00828 \text{ rad/s}^2 \]This means the tangential acceleration is negative, indicating deceleration along the tangent.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

Key Concepts

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

Centripetal Acceleration
When an object travels along a circular path at a constant speed, it still experiences an acceleration. This might seem counterintuitive since speed is not changing. However, speed isn't the only factor in motion; direction is crucial too.
So, what happens? As the car moves along the circular road, the direction of its velocity continuously changes. This change in direction requires a change in velocity, which is what we call centripetal acceleration.
Imagine it like this: centripetal acceleration acts as an invisible force pulling the car towards the center of the circle. Even though the speedometer reads a steady speed, the velocity vector is always shifting direction to keep the car on the circular path.
If you want to calculate centripetal acceleration, use this formula:
  • \( a_c = \frac{v_T^2}{r} \)
where:
  • \( v_T \) is the constant tangential speed
  • \( r \) is the radius of the circle
Tangential Acceleration
Tangential acceleration is involved when the speed of an object changes as it travels along its path. Imagine pressing the gas pedal or applying the brakes; you are changing the car's velocity along the tangent of its path.
When you alter the angular speed of your car, such as when slowing down to steer away from a collision, you introduce a tangential component to the car's acceleration. This component doesn't affect the direction but alters the speed component directly.
You can compute tangential acceleration when there's a change in angular speed using the formula:
  • \( a_T = \frac{\Delta \omega}{\Delta t} \)
where:
  • \( \Delta \omega \) is the change in angular speed
  • \( \Delta t \) represents the time interval over which the change occurs
A negative value in the calculation indicates a deceleration—like hitting the brakes. Hence, understanding tangential acceleration helps comprehend how speed variations affect motion along a circular route.
Angular Speed
Angular speed is a measure of how fast an object rotates around a point or axis. It's like the rotational counterpart to linear speed, which is simply how fast something moves in a straight line.
In the context of driving around a circular path, angular speed explains how quickly your car sweeps around the circle. You can calculate angular speed using the relationship between linear (tangential) speed and the radius of the circle:
  • \( v_T = r \times \omega \)
Solving for angular speed gives us:
  • \( \omega = \frac{v_T}{r} \)
where:
  • \( \omega \) is the angular speed
  • \( v_T \) is the tangential speed, or speedometer reading
  • \( r \) is the circle’s radius
Thus, angular speed helps describe motion more comprehensively, especially when an object orbits around a center point, as with a car navigating a curved road.

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

A pitcher throws a curveball that reaches the catcher in 0.60 s. The ball curves because it is spinning at an average angular velocity of 330 rev/min (assumed constant) on its way to the catcher’s mitt. What is the angular displacement of the baseball (in radians) as it travels from the pitcher to the catcher?

The earth has a radius of \(6.38 \times 10^{6} \mathrm{m}\) and turns on its axis once every \(23.9 \mathrm{h}\). (a) What is the tangential speed (in \(\mathrm{m} / \mathrm{s}\) ) of a person living in Ecuador, a country that lies on the equator? (b) At what latitude (i.e., the angle \(\theta\) in the drawing) is the tangential speed one-third that of a person living in Ecuador?

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. $$ \begin{array}{lll} & L & v \\ (\mathrm{a}) & 0.71 \mathrm{m} & 75.0 \mathrm{m} / \mathrm{s} \\ \hline(\mathbf{b}) & 0.71 \mathrm{m} & 91.0 \mathrm{m} / \mathrm{s} \\ \hline(\mathbf{c}) & 0.81 \mathrm{m} & 91.0 \mathrm{m} / \mathrm{s} \\ \hline \end{array} $$

A car is traveling along a road, and its engine is turning over with an angular velocity of \(+220 \mathrm{rad} / \mathrm{s} .\) The driver steps on the accelerator, and in a time of \(10.0 \mathrm{s}\) the angular velocity increases to \(+280 \mathrm{rad} / \mathrm{s}\). (a) What would have been the angular displacement of the engine if its angular velocity had remained constant at the initial value of \(+220 \mathrm{rad} / \mathrm{s}\) during the entire \(10.0-\mathrm{s}\) interval? (b) What would have been the angular displacement if the angular velocity had been equal to its final value of \(+280 \mathrm{rad} / \mathrm{s}\) during the entire \(10.0-\mathrm{s}\) interval? (c) Determine the actual value of the angular displacement during the \(10.0-\) s interval.

The table that follows lists four pairs of initial and fi nal angular velocities for a rotating fan blade. The elapsed time for each of the four pairs of angular velocities is 4.0 s. For each of the four pairs, fi nd the average angular acceleration (magnitude and direction as given by the algebraic sign of your answer). $$ \begin{array}{lcc} & \text { Initial angular } & \text { Final angular } \\ & \text { velocity } \omega_{0} & \text { velocity } \omega \\ \text { (a) } & +2.0 \mathrm{rad} / \mathrm{s} & +5.0 \mathrm{rad} / \mathrm{s} \\ \hline \text { (b) } & +5.0 \mathrm{rad} / \mathrm{s} & +2.0 \mathrm{rad} / \mathrm{s} \\ \hline \text { (c) } & -7.0 \mathrm{rad} / \mathrm{s} & -3.0 \mathrm{rad} / \mathrm{s} \\ \hline \text { (d) } & +4.0 \mathrm{rad} / \mathrm{s} & -4.0 \mathrm{rad} / \mathrm{s} \\ \hline \end{array} $$

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.