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A stockroom worker pushes a box with mass 11.2 \(\mathrm{kg}\) on a horizontal surface with a constant speed of 3.50 \(\mathrm{m} / \mathrm{s}\) . The coefficient of kinetic friction between the box and the surface is 0.20 . (a) What horizontal force must the worker apply to maintain the motion? (b) If the force calculated in part (a) is removed, how far does the box slide before coming to rest?

Short Answer

Expert verified
(a) Horizontal force needed is 21.952 N. (b) The box slides 3.12 meters before coming to rest.

Step by step solution

01

Understand the Problem

We have a box with mass of 11.2 kg moving on a horizontal surface. The worker applies a force to maintain a constant speed due to kinetic friction (coefficient = 0.20). First, we'll calculate the force needed to keep the box moving at a constant speed, and then determine the distance it will slide if the force is removed.
02

Calculate the Normal Force

Since the box is on a horizontal surface, the normal force is equal to the gravitational force. The normal force \( N \) can be calculated using:\[ N = mg \]where \( m = 11.2 \, \text{kg} \) and \( g = 9.8 \, \text{m/s}^2 \). Substitute to get \( N = 11.2 \times 9.8 = 109.76 \, \text{N} \).
03

Calculate the Frictional Force

The force of kinetic friction \( f_k \) can be calculated using the formula:\[ f_k = \mu_k N \]where \( \mu_k = 0.20 \). Substitute the values:\[ f_k = 0.20 \times 109.76 = 21.952 \, \text{N} \].
04

Find Horizontal Force for Constant Speed

To maintain a constant speed, the applied force \( F \) by the worker must equal the frictional force. Thus, \( F = f_k = 21.952 \, \text{N} \).
05

Calculate the Deceleration After Force is Removed

Once the worker stops applying the force, the box decelerates due to kinetic friction. The deceleration \( a \) can be calculated by Newton's second law:\[ f_k = ma \]\[ 21.952 = 11.2a \]\[ a = \frac{21.952}{11.2} \approx 1.96 \, \text{m/s}^2 \].
06

Calculate the Distance the Box Slides

To find the distance \( d \) the box slides before stopping, use the kinematic equation:\[ v^2 = u^2 + 2ad \]where \( v = 0 \, \text{m/s} \), \( u = 3.50 \, \text{m/s} \), and \( a = -1.96 \, \text{m/s}^2 \). Rearrange to solve for \( d \):\[ 0 = (3.50)^2 + 2(-1.96)d \]\[ 0 = 12.25 - 3.92d \]\[ d = \frac{12.25}{3.92} \approx 3.12 \, \text{m} \].

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Key Concepts

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

Newton's Laws of Motion
Newton's Laws of Motion are fundamental to understanding how objects move in our world. In this exercise, we primarily draw on Newton's First and Second Laws. These laws help explain why the box moves at a constant speed when a specific force is applied and what happens when that force is removed.

Newton's First Law of Motion, often termed the law of inertia, states that an object at rest stays at rest and an object in motion stays in motion at the same speed and in the same direction unless acted upon by an unbalanced external force. In our scenario, the box continues moving at a constant speed because the worker's applied force balances out the frictional force.
  • The box moves at constant speed due to the equal and opposite forces of friction and applied force.
  • When the worker stops applying the force, friction becomes the unbalanced force that slows down the box.
Newton's Second Law of Motion gives us the relationship between force, mass, and acceleration, formulated as \( F = ma \). This equation allows us to calculate the force required to maintain constant speed and also the acceleration (or deceleration) once the force is removed.

By applying these laws, we can predict and calculate how the box's motion will change under different conditions.
Kinetic Friction
Kinetic friction is a force that occurs between moving surfaces. It always acts in the direction opposite to the motion. We primarily use the concept of kinetic friction to understand the resisting force that the worker must overcome to keep the box moving.

Kinetic friction can be calculated using the formula \( f_k = \mu_k N \). Here, \( \mu_k \) is the coefficient of kinetic friction, and \( N \) is the normal force. The normal force is usually equal to the weight of the object when on a horizontal plane, so \( N = mg \).
  • For our box, \( \mu_k = 0.20 \) and the normal force \( N = 109.76 \, \text{N} \).
  • This gives a kinetic friction force \( f_k = 21.952 \, \text{N} \).
To keep the box moving at a consistent speed, the worker must exert a force equal to this frictional force, precisely balancing it to prevent acceleration.

Once the force is removed, kinetic friction works to bring the box to a stop by providing a constant deceleration until the motion ceases.
Kinematic Equations
Kinematic equations describe the motion of objects without considering the forces causing the motion. They help us find variables like distance, velocity, and acceleration when other values are known.

In the exercise, we use the kinematic equation \( v^2 = u^2 + 2ad \) to determine how far the box travels after the force stops being applied. This formula relates the final velocity \( v \), initial velocity \( u \), acceleration \( a \), and the distance \( d \).
  • Initial velocity \( u \) is 3.50 m/s, and the final velocity \( v \) is 0 m/s because the box comes to a stop.
  • The acceleration \( a \) is negative due to deceleration caused by friction, calculated as approximately \(-1.96 \, \text{m/s}^2 \).
By rearranging the equation to solve for \( d \), we find that the box slides approximately 3.12 meters before stopping. This example highlights how kinematic equations serve as powerful tools in predicting motion outcomes in real-world scenarios.

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Most popular questions from this chapter

A \(30.0-\mathrm{kg}\) packing case is initially at rest on the floor of a \(1500-\mathrm{kg}\) pickup truck. The coefficient of static friction between the case and the truck floor is \(0.30,\) and the coefficient of kinetic friction is \(0.20 .\) Before each acceleration given below, the truck is traveling due north at constant speed. Find the magnitude and direction of the friction force acting on the case (a) when the truck accelerates at 2.20 \(\mathrm{m} / \mathrm{s}^{2}\) northward and (b) when it accelerates at 3.40 \(\mathrm{m} / \mathrm{s}^{2}\) southward.

A box of weight w is accelerated up a ramp by a rope that exerts a tension \(T .\) The ramp makes an angle \(\alpha\) with the horizontal, and the rope makes an angle \(\theta\) above the ramp. The coefficient of kinetic friction between the box and the ramp is \(\mu_{k}\) . Show that no matter what the value of \(\alpha\) , the acceleration is maximum if \(\theta=\arctan \mu_{k}\) (as long as the box remains in contact with the ramp).

A flat (unbanked) curve on a highway has a radius of 220.0 \(\mathrm{m}\) . A car rounds the curve at a speed of 25.0 \(\mathrm{m} / \mathrm{s}\) , (a) What is the minimum coefficient of friction the coefficient of friction (b) Suppose the highway is icy and the coefficient of friction between the tires and pavement is only one-third what you found in part (a). What should be the maximum speed of the car so it can round the curve safely?

A light rope is attached to a block with mass 4.00 \(\mathrm{kg}\) that rests on a frictionless, horizontal surface. The horizontal rope passes over a frictionless, massless pulley, and a block with mass \(m\) is suspended from the other end. When the blocks are released, the tension in the rope is 10.0 \(\mathrm{N}\) . (a) Draw two free-body diagrams, one for the \(4.00-\mathrm{kg}\) block and one for the block with mass \(m\) . (b) What is the acceleration of either block? (c) Find the mass \(m\) of the hanging block. (d) How does the tension compare to the weight of the hanging block?

A 750.0-kg boulder is raised from a quarry 125 \(\mathrm{m}\) deep by a long uniform chain having a mass of 575 \(\mathrm{kg}\) . This chain is of uniform strength, but at any point it can support a maximum tension no greater than 2.50 times its weight without breaking. (a) What is the maximum acceleration the boulder can have and still get out of the quarry, and (b) how long does it take to be lifted out at maximum acceleration if it started from rest?

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