/*! 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 14 A person places a cup of coffee ... [FREE SOLUTION] | 91Ó°ÊÓ

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A person places a cup of coffee on the roof of her car while she dashes back into the house for a forgotten When she returns to the car, she hops in and takes off with the coffee cup still on the roof. (a) If the coefficient of static friction between the coffee cup and the roof of the car is \(0.24,\) what is the maximum acceleration the car can have without causing the cup to slide? lgnore the effects of air resistance. (b) What is the smallest amount of time in which the person can accelerate the car from rest to \(15 \mathrm{m} / \mathrm{s}\) and still keep the coffee cup on the roof?

Short Answer

Expert verified
(a) Maximum acceleration is \(2.3544 \, \mathrm{m/s^2}\). (b) Shortest time is \(6.37 \, \mathrm{s}\).

Step by step solution

01

Understanding Static Friction

The force of static friction that keeps the cup from sliding is calculated as \( F_{s} = \mu_{s} \cdot N \), where \( \mu_{s} \) is the coefficient of static friction, and \( N \) is the normal force. The normal force in this scenario is equal to the weight of the cup, which is \( mg \). Hence, the maximum static friction force is \( F_{s} = \mu_{s} \cdot mg \).
02

Relating Friction to Maximum Acceleration

According to Newton's second law, \( F = ma \). To find the maximum acceleration \( a_{max} \) that the cup can withstand without sliding, set the force of friction equal to the product of mass and acceleration: \( \mu_{s} \cdot mg = ma_{max} \). By canceling mass \( m \) from both sides, we get \( a_{max} = \mu_{s} \cdot g \).
03

Calculating Maximum Acceleration

Substitute \( \mu_{s} = 0.24 \) and the acceleration due to gravity \( g = 9.81 \mathrm{m/s^2} \). Thus, \( a_{max} = 0.24 \times 9.81 = 2.3544 \, \mathrm{m/s^2} \).
04

Calculating Smallest Time to Reach 15 m/s

The smallest time \( t \) required to accelerate the car from rest to a velocity \( v = 15 \, \mathrm{m/s} \) without the cup sliding is given by the formula \( v = a \cdot t \). Solving for time, \( t = \frac{v}{a} \).
05

Solving for Time

Substitute \( v = 15 \, \mathrm{m/s} \) and \( a = 2.3544 \, \mathrm{m/s^2} \): \( t = \frac{15}{2.3544} \). Calculating this gives \( t \approx 6.37 \, \mathrm{s} \).

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Key Concepts

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

Newton's Second Law
Newton's Second Law of Motion is a fundamental principle in physics, stating that the force acting on an object is equal to the mass of that object multiplied by its acceleration. This principle can be succinctly expressed using the formula:
  • \( F = ma \)
Where:
  • \( F \) is the total force applied on the object (measured in newtons)
  • \( m \) is the mass of the object (measured in kilograms)
  • \( a \) is the acceleration (measured in meters per second squared)
In the coffee cup scenario, the force that prevents the cup from sliding is the static friction force. According to Newton's Second Law, this static friction force is equal to the mass of the cup times its maximum acceleration (\( a_{max} \)). Solving this relationship allows us to determine how fast the car can accelerate without the cup sliding off the roof.
Coefficient of Static Friction
The coefficient of static friction, denoted as \( \mu_{s} \), is a dimensionless value representing the frictional force between two static objects. It indicates how easily one object will start to move over the other under force application.
  • This value varies between different pairs of surfaces.
  • It depends on both the materials and the surface textures in contact.
In our problem, the coefficient of static friction is given as \( 0.24 \). This means that the frictional force resisting motion (in this case preventing the coffee cup from sliding) is 24% of the normal force pressing the cup against the car roof. The higher the coefficient, the more resistance the surfaces will have against starting motion. By knowing this coefficient and applying it along with Newton's Second Law, we can determine the maximum possible acceleration the car can achieve without causing the cup to slip off.
Acceleration
Acceleration represents how quickly an object changes its velocity over time. It is a vector quantity, having both magnitude and direction. When a car accelerates, it increases its speed.
  • Units are typically meters per second squared (\( \, \mathrm{m/s^2} \)).
  • Acceleration can also mean slowing down, often referred to as negative acceleration or deceleration.
In the exercise, we calculated the maximum acceleration (\( a_{max}\)) determining how swiftly the car can speed up without the cup sliding. The calculated \( a_{max} \) of approximately \( 2.3544 \, \mathrm{m/s^2} \) represents the threshold. The car maintains grip on the cup up to this point. Any higher acceleration will overcome the static friction, causing the cup to move.
Normal Force
Normal force is the perpendicular force exerted by a surface to support the weight of an object resting on it. It is a crucial factor in friction calculations, as frictional force depends directly on it.
  • It is equal in magnitude and opposite in direction to the gravitational force acting on the object, when the object is on a horizontal surface.
  • Represented as \( N \), the normal force carries units of newtons (\( \, \text{N} \)).
For the coffee cup resting on a car roof, the normal force equals the weight of the cup, which is the product of its mass and the acceleration due to gravity \( g \), i.e., \( N = mg \). The interaction between \( N \) and the coefficient of static friction allows the calculation of static frictional force (\( F_{s} = \mu_{s} \cdot N \)). This frictional force ensures the cup remains stationary relative to the accelerating car, resisting motion until the frictional limit is surpassed.

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Most popular questions from this chapter

As your plane circles an airport, it moves in a horizontal circle of radius \(2300 \mathrm{m}\) with a speed of \(390 \mathrm{km} / \mathrm{h}\). If the lift of the airplane's wings is perpendicular to the wings, at what angle should the plane be banked so that it doesn't tend to slip sideways?

A child goes down a playground slide with an acceleration of \(1.26 \mathrm{m} / \mathrm{s}^{2} .\) Find the coefficient of kinetic friction between the child and the slide if the slide is inclined at an angle of \(33.0^{\circ}\) below the horizontal.

A tie of uniform width is laid out on a table, with a fraction of its length hanging over the edge. Initially, the tie is at rest. (a) If the fraction hanging from the table is increased, the tie eventually slides to the ground. Explain. (b) What is the coefficient of static friction between the tie and the table if the tie begins to slide when one-fourth of its length hangs over the edge?

A wood block of mass \(m\) rests on a larger wood block of mass \(M\) that rests on a wooden table. The coefficients of static and kinetic friction between all surfaces are \(\mu_{\mathrm{s}}\) and \(\mu_{\mathrm{k}}\), respectively. What is the minimum horizontal force, \(F\), applied to the lower block that will cause it to slide out from under the upper block?

Two buckets of sand hang from opposite ends of a rope that passes over an ideal pulley. One bucket is full and weighs \(120 \mathrm{N}\); the other bucket is only partly filled and weighs \(63 \mathrm{N}\). (a) Initially, you hold onto the lighter bucket to keep it from moving. What is the tension in the rope? (b) You release the lighter bucket and the heavier one descends. What is the tension in the rope now? (c) Eventually the heavier bucket lands and the two buckets come to rest. What is the tension in the rope now?

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