/*! 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 19 A car is traveling around an unb... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

A car is traveling around an unbanked curve at a maximum speed. Which force(s) is(are) responsible for keeping it on the road?

Short Answer

Expert verified
Answer: The friction force between the tires and the road surface is responsible for keeping the car on the road while traveling around an unbanked curve at maximum speed.

Step by step solution

01

Understand the forces acting on the car

When a car is traveling around a curve, there are generally two forces acting on it - the gravitational force (i.e. the weight of the car) pulling it downwards and the contact force exerted by the road on the car (essentially, the friction between the tires and the road surface) preventing it from slipping.
02

Identify the relevant force responsible for keeping the car on the road

In this particular case, since the car is traveling around an unbanked curve, we can assume it is moving horizontally. This means that the gravitational force is not relevant in this situation, because it acts perpendicular to the direction of motion. On the other hand, the force that is responsible for keeping the car on the road as it moves around the curve is the friction force. This force acts horizontally and inwards, towards the center of the curve, preventing the car from slipping off the road.
03

Understand the role of the car's speed

As the car is traveling at its maximum speed, this implies that it is moving at the highest speed it can maintain without losing its grip on the road. This is important because, at this speed, the friction force acting on the car has reached its maximum possible value. If the car's speed were to increase further, the friction force would no longer be enough to offset the car's tendency to slide off the road, causing it to lose control.
04

Conclusion

In conclusion, the force that is responsible for keeping a car on the road while it's traveling around an unbanked curve at maximum speed is the friction force between the tires and the road surface. This force acts horizontally and inwards, towards the center of the curve, preventing the car from slipping off the road.

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!

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 centrifuge in a medical laboratory rotates at an angular speed of 3600 rpm (revolutions per minute). When switched off, it rotates 60.0 times before coming to rest. Find the constant angular acceleration of the centrifuge.

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 \(80.0-\mathrm{kg}\) pilot in an aircraft moving at a constant speed of \(500 . \mathrm{m} / \mathrm{s}\) pulls out of a vertical dive along an arc of a circle of radius \(4000 . \mathrm{m}\).

A small block of mass \(m\) is in contact with the inner wall of a large hollow cylinder. Assume the coefficient of static friction between the object and the wall of the cylinder is \(\mu\). Initially, the cylinder is at rest, and the block is held in place by a peg supporting its weight. The cylinder starts rotating about its center axis, as shown in the figure, with an angular acceleration of \(\alpha\). Determine the minimum time interval after the cylinder begins to rotate before the peg can be removed without the block sliding against the wall.

A discus thrower (with arm length of \(1.2 \mathrm{~m}\) ) starts from rest and begins to rotate counterclockwise with an angular acceleration of \(2.5 \mathrm{rad} / \mathrm{s}^{2}\) a) How long does it take the discus thrower's speed to get to \(4.7 \mathrm{rad} / \mathrm{s} ?\) b) How many revolutions does the thrower make to reach the speed of \(4.7 \mathrm{rad} / \mathrm{s} ?\) c) What is the linear speed of the discus at \(4.7 \mathrm{rad} / \mathrm{s} ?\) d) What is the linear acceleration of the discus thrower at this point? e) What is the magnitude of the centripetal acceleration of the discus thrown? f) What is the magnitude of the discus's total acceleration?

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.