A car accelerates uniformly from rest and reaches a speed of \(22.0 \mathrm{~m} / \mathrm{s}\) in \(9.00 \mathrm{~s}\). The diameter of a tire on this car is \(58.0 \mathrm{~cm}\). a) Find the number of revolutions the tire makes during the car's motion, assuming that no slipping occurs. b) What is the final angular speed of a tire in revolutions per second?

Short Answer

Expert verified
Question: During a car's performance test, a tire with a diameter of 58.0 cm starting from rest reaches a speed of 22.0 m/s after 9.00 s. Calculate the number of revolutions the tire makes during the car's motion (assuming no slipping) and the final angular speed of a tire in revolutions per second. Answer: To find the number of revolutions the tire makes and the final angular speed of a tire in revolutions per second, follow the steps as outlined in the solution above. First, determine the linear acceleration and distance traveled by the car. Next, calculate the tire's radius and the angular distance. Then, convert the angular distance to revolutions, find the final angular speed in radians per second, and finally, convert it to revolutions per second.

Step by step solution

01

- Find linear acceleration

Given that the final speed of the car is \(22.0 \mathrm{~m/s}\) and the time taken is \(9.00 \mathrm{s}\), we can find the linear acceleration of the car using the formula: $$v = u + a \cdot t$$ where v is the final velocity, u is the initial velocity (which is 0 since the car is at rest), a is the acceleration, and t is the time taken. Plugging in the values, we get: $$22.0 = 0 + a \cdot 9.00$$ Now, we can solve for 'a': $$a = \frac{22.0}{9.00}$$
02

- Find linear distance

Now that we have found the linear acceleration, we can find the distance traveled by the car using the formula: $$s = u \cdot t + \frac{1}{2} a \cdot t^2$$ Plugging in the values of u = 0, t = 9.00 s, and the calculated value of 'a', we can find the linear distance 's'.
03

- Calculate tire's radius

Given the diameter of the tire is \(58.0 \mathrm{cm}\), we can find the tire's radius by dividing the diameter by 2: $$r = \frac{58.0}{2}$$ Ensure to convert the radius to meters for uniformity of units.
04

- Determine the angular distance

Now that we have the tire's radius, we can determine the angular distance the tire covers during the car's motion by using the formula: $$\theta (in \: radians) = \frac{s}{r}$$ Using the linear distance 's' found in step 2, and the tire's radius 'r' found in step 3, we can find the angular distance, expressed in radians.
05

- Convert angular distance to revolutions

To find the number of revolutions the tire makes during the car's motion, we have to convert the angular distance found in step 4 from radians to revolutions using the following relation: $$1 \: revolution = 2\pi \: radians$$ So, $$number \: of \: revolutions = \frac{\theta (in \: radians)}{2\pi}$$
06

- Finding final angular speed in radians per second

Now we have to find the final angular speed of the tire, in radians per second. We can use the formula: $$\omega^2 = \omega_0^2 + 2 \alpha \cdot \theta$$ where \(\omega\) is the final angular speed, \(\omega_0\) is the initial angular speed (which is 0, since it was at rest), \(\alpha\) is the angular acceleration, and \(\theta\) is the angular distance in radians. First, we have to find the angular acceleration. We can use the relation: $$\alpha = \frac{a}{r}$$ Substituting the linear acceleration 'a', and the tire's radius 'r', we can find the angular acceleration.
07

- Calculate final angular speed in radians per second

Now that we have the angular acceleration, we can find the final angular speed using the formula mentioned above (\(\omega^2 = \omega_0^2 + 2 \alpha \cdot \theta\)). Since \(\omega_0\) is 0, we get: $$\omega^2 = 2 \alpha \cdot \theta$$ After solving for \(\omega\), we'll have the final angular speed in radians per second.
08

- Convert final angular speed to revolutions per second

Finally, we have to convert the final angular speed found in step 7 from radians per second to revolutions per second using the following relation: $$1 \: revolution = 2\pi \: radians$$ So, $$final \: angular \: speed \: (in \: revolutions \: per \: second) = \frac{\omega}{2\pi}$$

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 Vaia!

Key Concepts

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

Angular Speed
Angular speed is the rate at which an object rotates or spins around an axis. In the context of a tire on a moving vehicle, it refers to how fast the tire is spinning. The angular speed is typically measured in radians per second (rad/s) or revolutions per second (rev/s).

To convert to a more intuitive unit like rev/s, we use the fact that one full revolution is equal to an angle of 2π radians. Therefore, if you find the angular speed in rad/s, you would divide by 2π to obtain the angular speed in rev/s. This conversion is crucial when comparing the rotational speed of tires to the vehicle's linear speed (measured in m/s or km/h).

In the exercise where a final angular speed is asked, the student must understand the conversion between radians and revolutions to interpret the tire's performance accurately.
Linear Acceleration
Linear acceleration refers to the change in linear velocity of an object per unit time, moving along a straight path. This is directly related to the force applied according to Newton's second law of motion and is usually measured in meters per second squared (m/s²).

In the exercise provided, to determine the linear acceleration of the car, the formula \(v = u + at\) was used, where \(v\) is the final velocity, \(u\) is the initial velocity, \(a\) is the acceleration, and \(t\) is the time taken. Knowing the linear acceleration allows us to understand how quickly the car is speeding up and provides the information needed to calculate other values like tire revolutions and angular speed.

An understanding of acceleration is fundamental since it directly affects the angular acceleration of the tire, leading to a greater angular speed over time, given a constant linear acceleration.
Tire Revolutions
The term 'tire revolutions' refers to the number of full turns a tire makes over a certain period or distance. It's an essential measure for understanding how far a vehicle has travelled since each turn of the tire corresponds to a specific distance – the tire's circumference. It's a useful conversion factor in mechanics and kinematics.

To calculate the tire revolutions from the angular distance in radians, as seen in the exercise, you divide the angular distance by \(2\text{π}\) since there are \(2\text{π}\) radians in one revolution. This calculation provides the total number of complete rotations a wheel makes, helping understand vehicle speed and distance covered, as long as there's no slipping between the tire and the road.
Angular Distance
Angular distance measures how much an object has rotated about a point or axis. It is usually represented in degrees or radians. For a wheel, it indicates how far it has turned over a particular linear distance.

In kinematic problems like the exercise, the linear distance covered by the car (calculated from linear acceleration and time) can be used along with the radius of the tire to find the angular distance the tire has covered. The formula \(\theta (in \text{ radians}) = \frac{s}{r}\) converges the linear progress of the car into the rotational progress of its tires given that the tire's radius remains constant. The knowledge of angular distance is pivotal for connecting linear and rotational kinematics in objects like wheels.

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

Assuming that the Earth is spherical and recalling that latitudes range from \(0^{\circ}\) at the Equator to \(90^{\circ} \mathrm{N}\) at the North Pole, how far apart, measured on the Earth's surface, are Dubuque, Iowa \(\left(42.50^{\circ} \mathrm{N}\right.\) latitude \()\), and Guatemala City \(\left(14.62^{\circ} \mathrm{N}\right.\) latitude \() ?\) The two cities lie on approximately the same longitude. Do not neglect the curvature of the Earth in determining this distance.

A hook above a stage is rated to support \(150 .\) lb. A 3 -lb rope is attached to the hook, and a 147 -lb actor is going to attempt to swing across the stage on the rope. Will the hook hold the actor up during the swing?

A typical Major League fastball is thrown at approximately \(88 \mathrm{mph}\) and with a spin rate of \(110 \mathrm{rpm} .\) If the distance between the pitcher's point of release and the catcher's glove is exactly \(60.5 \mathrm{ft},\) how many full turns does the ball make between release and catch? Neglect any effect of gravity or air resistance on the ball's flight.

Mars orbits the Sun at a mean distance of 228 million \(\mathrm{km},\) in a period of 687 days. The Earth orbits at a mean distance of 149.6 million \(\mathrm{km},\) in a period of 365.26 days. a) Suppose Earth and Mars are positioned such that Earth lies on a straight line between Mars and the Sun. Exactly 365.26 days later, when the Earth has completed one orbit, what is the angle between the Earth-Sun line and the Mars-Sun line? b) The initial situation in part (a) is a closest approach of Mars to Earth. What is the time, in days, between two closest approaches? Assume constant speed and circular orbits for both Mars and Earth. c) Another way of expressing the answer to part (b) is in terms of the angle between the lines drawn through the Sun, Earth, and Mars in the two closest approach situations. What is that angle?

A 20.0 -g metal cylinder is placed on a turntable, with its center \(80.0 \mathrm{~cm}\) from the turntable's center. The coefficient of static friction between the cylinder and the turntable's surface is \(\mu_{s}=0.800\). A thin, massless string of length \(80.0 \mathrm{~cm}\) connects the center of the turntable to the cylinder, and initially, the string has zero tension in it. Starting from rest, the turntable very slowly attains higher and higher angular velocities, but the turntable and the cylinder can be considered to have uniform circular motion at any instant. Calculate the tension in the string when the angular velocity of the turntable is 60.0 rpm (rotations per minute).

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.

Sign-up for free