Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

Two 25.0-N weights are suspended at opposite ends of a rope that passes over a light, frictionless pulley. The pulley is attached to a chain from the ceiling. (a) What is the tension in the rope? (b) What is the tension in the chain?

Short Answer

Expert verified
(a) 25.0 N; (b) 50.0 N

Step by step solution

01

Understanding the System

The setup consists of two identical weights, each with downward force due to gravity, suspended by a rope over a pulley. The pulley is frictionless and light (meaning its mass is negligible) and does not affect the tension directly.
02

Analyzing Forces on the Weights

Each weight exerts a force due to gravity on the rope. Both weights are 25.0 N. Since the pulley is massless and frictionless, the tension throughout the rope must be the same.
03

Calculating the Tension in the Rope

Since the system is symmetrical with identical weights on both sides, the tension in the rope supports the 25.0 N force from each weight. Therefore, the tension in the rope is equal to the weight of one block, 25.0 N.
04

Determining the Tension in the Chain

The chain supports the entire system, including the tensions from both halves of the rope which both equal the weight of 25.0 N. Thus, the tension in the chain is the total downward force: 25.0 N + 25.0 N = 50.0 N.

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 Vaia!

Key Concepts

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

Force of Gravity
In physics, understanding the force of gravity is crucial when analyzing how objects interact with one another. Gravity is a force that pulls objects toward each other. On Earth, it gives weight to physical objects and affects their motion.
For instance, in the given exercise, each of the weights hanging from the pulley experiences a force due to gravity. This force is directed downwards toward the center of the Earth and is calculated as the product of the mass of an object and the gravitational acceleration, which is approximately 9.81 m/s².
Because both weights are 25.0 N, this value represents the gravitational force acting on them. In simpler terms, each weight "feels" a pull from the Earth that amounts to 25.0 N. Understanding how gravity operates here helps us determine the tension in the rope and chain.
Frictionless Pulley
A frictionless pulley is an ideal concept used in physics to simplify the analysis of motion. When a pulley is termed "frictionless," it means that it has no resistance to the movement of the rope passing over it.
This characteristic is crucial for solving the exercise involving weights suspended over a pulley. The absence of friction ensures that the tension in the rope is the same on both sides because no energy is lost in overcoming friction. This setup allows us to consider only the gravitational forces and the tension without complicating factors.
The frictionless nature of the pulley in the problem allows the weights' forces to balance each other out smoothly, meaning the tension supporting both weights is identical at 25.0 N. Such a simplification helps in focusing on the key aspects of equilibrium without extra noise.
System Equilibrium
When a system is in equilibrium, all forces acting on it balance each other out, and there is no net movement. In mechanical systems like the one described in the exercise, equilibrium implies that the forces on both sides of the pulley are equal, so the system remains stationary.
In the problem with the suspended weights, the weights are balanced because each has the same gravitational force pulling downwards. The tensions created by these forces are equal and opposite, ensuring stability.
We found that the tension in the rope is 25.0 N on either side because each weight is exerting that amount of force downward. As a whole, the chain holds the combined tension from both weights, 50.0 N, reflecting the total gravitational pull. Achieving this perfect balance, or equilibrium, is essential for ensuring systems function predictably and comprehensibly.

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 3.00-kg box that is several hundred meters above the earth's surface is suspended from the end of a short vertical rope of negligible mass. A time- dependent upward force is applied to the upper end of the rope and results in a tension in the rope of \(T(t) =\) (36.0 N/s)\(t\). The box is at rest at \(t =\) 0. The only forces on the box are the tension in the rope and gravity. (a) What is the velocity of the box at (i) \(t =\) 1.00 s and (ii) \(t =\) 3.00 s? (b) What is the maximum distance that the box descends below its initial position? (c) At what value of \(t\) does the box return to its initial position?

On September 8, 2004, the \(Genesis\) spacecraft crashed in the Utah desert because its parachute did not open. The 210-kg capsule hit the ground at 311 km/h and penetrated the soil to a depth of 81.0 cm. (a) What was its acceleration (in m/s\(^2\) and in g's), assumed to be constant, during the crash? (b) What force did the ground exert on the capsule during the crash? Express the force in newtons and as a multiple of the capsule's weight. (c) How long did this force last?

While a person is walking, his arms swing through approximately a 45\(^\circ\) angle in \(\frac{1}{2}\) s. As a reasonable approximation, assume that the arm moves with constant speed during each swing. A typical arm is 70.0 cm long, measured from the shoulder joint. (a) What is the acceleration of a 1.0-g drop of blood in the fingertips at the bottom of the swing? (b) Draw a free-body diagram of the drop of blood in part (a). (c) Find the force that the blood vessel must exert on the drop of blood in part (a). Which way does this force point? (d) What force would the blood vessel exert if the arm were not swinging?

A hammer is hanging by a light rope from the ceiling of a bus. The ceiling is parallel to the roadway. The bus is traveling in a straight line on a horizontal street. You observe that the hammer hangs at rest with respect to the bus when the angle between the rope and the ceiling of the bus is 56.0\(^\circ\). What is the acceleration of the bus?

You are riding in a school bus. As the bus rounds a flat curve at constant speed, a lunch box with mass 0.500 kg, suspended from the ceiling of the bus by a string 1.80 m long, is found to hang at rest relative to the bus when the string makes an angle of 30.0\(^{\circ}\) with the vertical. In this position the lunch box is 50.0 m from the curve's center of curvature. What is the speed \(\upsilon \) of the bus?

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.

Sign-up for free