/*! 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 5 A rope is tied to a box and used... [FREE SOLUTION] | 91Ó°ÊÓ

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A rope is tied to a box and used to pull the box \(1.5 \mathrm{~m}\) along a h zontal floor. The rope makes an angle of \(30^{\circ}\) with the horizontal has a tension of \(5 \mathrm{~N}\). The opposing friction force between the box the floor is \(1 \mathrm{~N}\). How much work does each of the following forces do on the box: (a) gravity, (b) the tension in the rope, (c) friction, and (d) the normal force? What is the total work done on the box?

Short Answer

Expert verified
(a) 0 J, (b) 6.495 J, (c) -1.5 J, (d) 0 J, Total: 4.995 J.

Step by step solution

01

Understanding Work Done by Gravity

Gravity acts vertically downward, perpendicular to the horizontal displacement of the box. Therefore, the work done by gravity, which is calculated as \( W = F \cdot s \cdot \cos(\theta) \), is zero because the angle \( \theta \) between the gravitational force and displacement is \(90^\circ\), and \( \cos(90^\circ) = 0 \). Thus, the work done by gravity is \( 0 \, \text{J} \).
02

Calculating Work Done by the Tension in the Rope

The work done by the tension force is calculated using \( W = F \cdot s \cdot \cos(\theta) \). Here, the tension \( F = 5 \, \text{N} \), the displacement \( s = 1.5 \, \text{m} \), and the angle \( \theta = 30^\circ \). Substitute these into the equation to get \( W = 5 \, \text{N} \cdot 1.5 \, \text{m} \cdot \cos(30^\circ) \). Simplifying gives \( W = 5 \cdot 1.5 \cdot 0.866 = 6.495 \, \text{J} \).
03

Calculating Work Done by Friction

The frictional force opposes the direction of displacement, meaning the angle \( \theta \) between the force and displacement is \(180^\circ\). The formula is \( W = F \cdot s \cdot \cos(\theta) \). The frictional force \( F = 1 \, \text{N} \) and \( s = 1.5 \, \text{m} \). Thus, \( W = 1 \cdot 1.5 \cdot \cos(180^\circ) = 1.5 \, \text{J} \) (since \( \cos(180^\circ) = -1 \), the work is negative). So, the work done by friction is \(-1.5 \, \text{J} \).
04

Work Done by the Normal Force

The normal force acts perpendicular to the direction of displacement. Since the angle \( \theta \) between the normal force and displacement is \(90^\circ\), the work done by the normal force is \( W = F \cdot s \cdot \cos(\theta) = 0 \), as \( \cos(90^\circ) = 0 \). Thus, the work done by the normal force is \( 0 \, \text{J} \).
05

Calculating Total Work Done on the Box

The total work done is the sum of the work done by all forces on the box. Adding the work done by tension \(6.495 \, \text{J}\), by gravity \(0 \, \text{J}\), by friction \(-1.5 \, \text{J}\), and by the normal force \(0 \, \text{J}\), we get \(6.495 + 0 + (-1.5) + 0 = 4.995 \, \text{J}\). Thus, the total work done on the box is \(4.995 \, \text{J}\).

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Key Concepts

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

Friction
Friction is a force that opposes the motion of objects in contact. In the given problem, it acts between the box and the floor as the box is being pulled by the rope. Frictional force is calculated as the product of the coefficient of friction and the normal force. However, in this exercise, it is directly provided as 1 N. It acts along the same line as the direction of motion but opposite in sense. This is why, when calculating the work done by friction using the equation \[ W = F \cdot s \cdot \cos(\theta) \] we use \( \theta = 180^\circ \). Remember that \( \cos(180^\circ) = -1 \), which results in negative work, showing that friction takes energy away from the system.When objects move and friction acts on them, energy is spent mainly to overcome this resistance. In our example,
  • The work done by friction is \(-1.5 \, \text{J}\).
  • It converts mechanical energy, which could have been used for movement, into heat energy.
  • The negative sign in work indicates an energy loss due to friction.
Understanding friction's impact is crucial for calculating net work and analyzing energy expenditure in a system.
Tension
Tension is the force that is transmitted through the rope in our exercise. This force is responsible for pulling the box along the floor. Since the tension force is not acting purely horizontally but at an angle, a component of this force acts in the direction of pull.When solving for work done by tension, we use the formula:\[ W = F \cdot s \cdot \cos(\theta) \]Here, \( F \) is the tension force (5 N), \( s \) is the displacement (1.5 m), and \( \theta \) is the angle between the force and the direction of displacement (30°). The use of trigonometric functions allows us to accurately reflect the component of force in the actual path of movement. Thus,
  • \( \cos(30^\circ) \approx 0.866 \)
  • Work done by tension calculates to \( 6.495 \, \text{J} \)
The positive value indicates that the tension is contributing energy to the system, making the box move along the floor.Understanding tension is essential for any system involving ropes, strings, or cables, as it defines the force exerted across these mediums.
Normal Force
Normal force is a contact force that acts perpendicular to surfaces in contact, such as between the box and the floor. In the context of our problem, the normal force solely balances out the weight of the box under the influence of gravity.Since the normal force is perpendicular to the direction of the box's movement,
  • The angle \( \theta \) between the normal force and the path of displacement is \( 90^\circ \).
  • This leads to a work done calculation of \( W = F \cdot s \cdot \cos(90^\circ) \), which is zero because \( \cos(90^\circ) = 0 \).
  • Thus, no work is done by the normal force.
This illustrates a key point: even though forces can be present, not all forces do work. Understanding the role of normal force helps in analyzing motion, especially when surfaces are inclined or curved.
Physics Problem Solving
Physics problem solving involves breaking down complex problems into manageable steps. In exercises like these, it's critical to identify each force acting on the system and understand its orientation with respect to the motion.The key steps in problem solving include:
  • Identifying all forces involved and the nature of each force (tension, friction, gravity, normal force).
  • Understanding direction: analyzing angles and directions between forces and displacement, as this impacts the work calculation through the cosine of the angle.
  • Using systematic calculations: applying formulas correctly, such as \( W = F \cdot s \cdot \cos(\theta) \), to find the work done by different forces.
  • Putting it all together: summing the work of individual forces to determine total work done, revealing the net effect on the object.
Developing these skills enables thorough analysis and comprehension, not just for solving textbook exercises, but also real-life physical problems.

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Most popular questions from this chapter

Human terminal velocity. By landing properly and on soft ground (and by being lucky!), humans have survived falls from airplanes when, for example, a parachute failed to open, with astonishingly little injury. Without a parachute, a typical human eventually reaches a terminal velocity of about \(62 \mathrm{~m} / \mathrm{s}\). Suppose the fall is from an airplane \(1000 \mathrm{~m}\) high. (a) How fast would a person be falling when he reached the ground if there were no air drag? (b) If a \(70 \mathrm{~kg}\) person reaches the ground traveling at the terminal velocity of \(62 \mathrm{~m} / \mathrm{s},\) how much mechanical energy was lost during the fall? What happened to that energy?

The total height of Yosemite Falls is \(2425 \mathrm{ft}\). (a) How many more joules of gravitational potential energy are there for each kilogram of water at the top of this waterfall compared with each kilogram of water at the foot of the falls? (b) Find the kinetic energy and speed of each kilogram of water as it reaches the base of the waterfall, assuming that there are no losses due to friction with the air or rocks and that the mass of water had negligible vertical speed at the top. How fast (in \(\mathrm{m} / \mathrm{s}\) and \(\mathrm{mph}\) ) would a \(70 \mathrm{~kg}\) person have to run to have that much kinetic energy? (c) How high would Yosemite Falls have to be so that each kilogram of water at the base had twice the kinetic energy you found in part (b); twice the speed you found in part (b)?

While a roofer is working on a roof that slants at \(36^{\circ}\) above the horizontal, he accidentally nudges his \(85.0 \mathrm{~N}\) toolbox, causing it to start sliding downward, starting from rest. If it starts \(4.25 \mathrm{~m}\) from the lower edge of the roof, how fast will the toolbox be moving just as it reaches the edge of the roof if the kinetic friction force on it is \(22.0 \mathrm{~N} ?\)

A wooden rod of negligible mass and length \(80.0 \mathrm{~cm}\) is pivoted about a horizontal axis through its center. A white rat with mass \(0.500 \mathrm{~kg}\) clings to one end of the stick, and a mouse with mass \(0.200 \mathrm{~kg}\) clings to the other end. The system is released from rest with the rod horizontal. If the animals can manage to hold on, what are their speeds as the rod swings through a vertical position?

On flat ground, a \(70 \mathrm{~kg}\) person requires about \(300 \mathrm{~W}\) of metabolic power to walk at a steady pace of \(5.0 \mathrm{~km} / \mathrm{h}(1.4 \mathrm{~m} / \mathrm{s})\) Using the same metabolic power output, that person can bicycle over the same ground at \(15 \mathrm{~km} / \mathrm{h}\). A \(70 \mathrm{~kg}\) person walks at a steady pace of \(5.0 \mathrm{~km} / \mathrm{h}\) on a treadmill at a \(5.0 \%\) grade (that is, the vertical distance covered is \(5.0 \%\) of the horizontal distance covered). If we assume the metabolic power required is equal to that required for walking on a flat surface plus the rate of doing work for the vertical climb, how much power is required? A. \(300 \mathrm{~W}\) B. 315 W C. \(350 \mathrm{~W}\) D. \(370 \mathrm{~W}\)

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