/*! 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 1 The floor of a railroad flatcar ... [FREE SOLUTION] | 91Ó°ÊÓ

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The floor of a railroad flatcar is loaded with loose crates having a coefficient of static friction of \(0.25\) with the floor. If the train is initially moving at a speed of \(48 \mathrm{~km} / \mathrm{h}\), in how short a distance can the train be stopped at constant acceleration without causing the crates to slide over the floor?

Short Answer

Expert verified
The train can stop in approximately 36.25 meters without the crates sliding.

Step by step solution

01

Convert Units

First, we need to convert the train's speed from kilometers per hour to meters per second, because the SI unit for speed is m/s. Use the conversion factor: \[ 1 \text{ km/h} = \frac{1}{3.6} \text{ m/s} \]So, \(48 \text{ km/h} = 48 \times \frac{1}{3.6} \text{ m/s} = 13.33 \text{ m/s}\).
02

Identify Forces Involved

The force causing the crates to slide is the force of static friction. The frictional force \(F_f\) is given by:\[ F_f = \mu_s \cdot m \cdot g \]where \(\mu_s = 0.25\) is the coefficient of static friction, \(m\) is the mass of the crate, and \(g = 9.8\, \text{m/s}^2\) is the acceleration due to gravity.
03

Relate Friction to Acceleration

The crates will just begin to slide if the negative acceleration of the train equals the acceleration due to the frictional force. Using Newton's second law \(F = m \cdot a\), we find:\[ m \cdot a = \mu_s \cdot m \cdot g \]which simplifies to:\[ a = \mu_s \cdot g \].Plugging in the values, we get:\[ a = 0.25 \times 9.8 = 2.45\, \text{m/s}^2\].
04

Use Kinematics to Find Stopping Distance

Using the kinematic equation that relates initial velocity \(v_i\), final velocity \(v_f\), acceleration \(a\), and distance \(d\):\[ v_f^2 = v_i^2 + 2\cdot a \cdot d \]Here, \(v_f = 0\) m/s (train stops), \(v_i = 13.33\) m/s, and \(a = -2.45\) m/s² (since it's deceleration). Solve for \(d\):\[ 0 = (13.33)^2 + 2 \times (-2.45) \times d \]\[ d = \frac{(13.33)^2}{2 \times 2.45} \approx 36.25 \text{ meters}\].

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Key Concepts

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

Static Friction
Static friction is a force that keeps objects at rest when they are placed on a surface. It acts between the contact surfaces and prevents them from sliding against each other.

In the context of the original exercise, the coefficient of static friction (denoted as \(\mu_s\)) is a dimensionless value that describes how strongly the surfaces grip together. This coefficient depends on the materials of the surfaces.
  • A higher coefficient means the surfaces stick more firmly, requiring more force to move one over the other.
  • A lower coefficient implies less grip, making it easier for sliding to start.
The frictional force can be calculated using the formula:\[ F_f = \mu_s \cdot m \cdot g \] - where:
  • \( F_f \) is the force of friction
  • \( m \) is the mass of the object
  • \( g \) is the acceleration due to gravity, typically \(9.8 \, \text{m/s}^2\)
In scenarios like the train problem, the static frictional force prevents the crates from sliding as long as the acceleration does not exceed this force. Understanding static friction is crucial to determining the maximum permissible deceleration or force before motion begins.
Kinematics
Kinematics is the branch of mechanics that describes the motion of objects without considering the forces that cause them. It involves quantities like velocity, acceleration, and displacement.

In the problem exercise, we used kinematic equations to determine how far the train must travel before stopping. The main kinematic equation used is:\[ v_f^2 = v_i^2 + 2 \cdot a \cdot d \] where:
  • \( v_f \) is the final velocity
  • \( v_i \) is the initial velocity
  • \( a \) is the acceleration (negative in the case of deceleration)
  • \( d \) is the distance
This equation helps us calculate the stopping distance by rearranging it to solve for \(d\). Starting with an initial speed, when the velocity reaches zero, we can see how long the object travels under constant acceleration.

Kinematics provides a framework to analyze motion without delving into why things happen, focusing instead on the paths objects take.
Newton's Second Law
Newton's Second Law of Motion describes the relationship between an object's mass, its acceleration, and the force applied. This principle is expressed as: \[ F = m \cdot a \]This fundamental law implies:
  • Force is directly proportional to both mass and acceleration.
  • The greater the mass of an object, the more force is needed to accelerate it.
Applying Newton's Law in the context of the train, we use it to relate the static friction force preventing the crates from moving, and the retardation of the train. When force due to braking equals the maximum static frictional force, the crates start to slide.

By substituting the force of friction expression from static friction into Newton's second law, we find:\[ m \cdot a = \mu_s \cdot m \cdot g \] which simplifies to: \[ a = \mu_s \cdot g \] This shows how static friction determines the maximum deceleration without motion. Newton's Second Law is essential for understanding how forces affect motion.

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Most popular questions from this chapter

What is the smallest radius of an unbanked (flat) track around which a bicyclist can travel if her speed is \(29 \mathrm{~km} / \mathrm{h}\) and the \(\mu_{s}\) between tires and track is \(0.32 ?\)

Two blocks, of weights \(3.6 \mathrm{~N}\) and \(7.2 \mathrm{~N}\), are connected by a massless string and slide down a \(30^{\circ}\) inclined plane. The coefficient of kinetic friction between the lighter block and the plane is \(0.10\), and the coefficient between the heavier block and the plane is 0.20. Assuming that the lighter block leads, find (a) the magnitude of the acceleration of the blocks and (b) the tension in the taut string.

An \(11 \mathrm{~kg}\) block of steel is at rest on a horizontal table. The coefficient of static friction between block and table is \(0.52 .\) (a) What is the magnitude of the horizontal force that will put the block on the verge of moving? (b) What is the magnitude of a force acting upward \(60^{\circ}\) from the horizontal that will put the block on the verge of moving? (c) If the force acts downward at \(60^{\circ}\) from the horizontal, how large can its magnitude be without causing the block to move?

\( \Rightarrow \sqrt{2}\) A sling-thrower puts a stone \((0.250 \mathrm{~kg})\) in the sling's pouch \((0.010 \mathrm{~kg})\) and then begins to make the stone and pouch move in a vertical circle of radius \(0.650 \mathrm{~m}\). The cord between the pouch and the person's hand has negligible mass and will break when the tension in the cord is \(33.0 \mathrm{~N}\) or more. Suppose the slingthrower could gradually increase the speed of the stone. (a) Will the breaking occur at the lowest point of the circle or at the highest point? (b) At what speed of the stone will that breaking occur?

A person pushes horizontally with a force of \(220 \mathrm{~N}\) on a \(55 \mathrm{~kg}\) crate to move it across a level floor. The coefficient of kinetic friction between the crate and the floor is \(0.35 .\) What is the magnitude of (a) the frictional force and (b) the acceleration of the crate?

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