/*! 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 15 (II) A grocery cart with mass of... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

(II) A grocery cart with mass of 16\(\mathrm { kg }\) is being pushed at constant speed up a flat \(12 ^ { \circ }\) ramp by a force \(F _ { \mathrm { P } }\) which acts at an angle of \(17 ^ { \circ }\) below the horizontal. Find the work done by each of the forces \(\left( m \vec { g } , \vec { \mathbf { F } } _ { \mathrm { N } } , \vec { \mathbf { F } } _ { \mathrm { P } } \right)\) on the cart if the ramp is 15\(\mathrm { m }\) long.

Short Answer

Expert verified
Work by gravity: -488.4 J, by normal force: 0 J, by pushing force: 488.4 J.

Step by step solution

01

Identify the forces involved

There are three main forces acting on the grocery cart: 1. The gravitational force, \( m\vec{g} \), acting vertically downward.2. The normal force, \( \vec{F}_N \), acting perpendicular to the ramp surface.3. The pushing force, \( \vec{F}_P \), directed at an angle of \( 17^{\circ} \) below the horizontal.
02

Calculate work done by gravitational force

The gravitational force, \( m \vec{g} \), acts vertically downwards. However, the component of gravitational force that acts along the ramp is what affects work done. This component is \( m g \sin(\theta) \), where \( \theta = 12^{\circ} \) and \( g = 9.8 \text{ m/s}^2 \).Work done by gravity: \[ W_g = m g \sin(\theta) \times d \]Given values:\( m = 16 \text{ kg} \), \( d = 15 \text{ m} \), and \( \theta = 12^{\circ} \). Substitute these into the equation:\[ W_g = 16 \times 9.8 \times \sin(12^{\circ}) \times 15 \] Calculate \( W_g \).
03

Calculate work done by the normal force

Work done by the normal force, \( \vec{F}_N \), is typically zero when moving along a frictionless surface perpendicular to the direction of motion. Since the normal force is perpendicular to the motion along the ramp, \[ W_N = 0 \].
04

Calculate work done by the pushing force

The force \( \vec{F}_P \) acts at an angle. The component of this force along the ramp is what does work.This component is \( F_P \cos(17^{\circ}) \). The angle between \( \vec{F}_P \) and the ramp is \( 17^{\circ} - 12^{\circ} = 5^{\circ} \).Work done by \( \vec{F}_P \):\[ W_P = F_P d \cos(5^{\circ}) \]At constant speed, work done by \( \vec{F}_P \) counteracts work done by gravity, therefore \[ W_P = -W_g \].
05

Summarize Work Done by Each Force

1. Work done by gravitational force: \( W_g = -488.4 \text{ J} \) (calculated in Step 2)2. Work done by normal force: \( W_N = 0 \text{ J} \) (calculated in Step 3) 3. Work done by the pushing force: \( W_P = 488.4 \text{ J} \) (calculated in Step 4)

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 91Ó°ÊÓ!

Key Concepts

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

Forces
In classical mechanics, forces are pushes or pulls that can cause an object to move, stop, or change direction. Understanding these forces is essential when analyzing motion on our daily life, such as when a grocery cart is pushed up a ramp.
  • Gravitational Force (\( m \vec{g} \)): This force pulls objects towards the center of the earth and acts vertically downwards. It's the weight of the grocery cart in this exercise.
  • Normal Force (\( \vec{F}_N \)): This force acts perpendicular to a surface. On the ramp, it prevents the cart from moving through the surface, balancing part of the gravitational pull.
  • Pushing Force (\( \vec{F}_P \)): This is the applied force that makes the cart move up the ramp. It's directed at an angle of \( 17^\circ \) below the horizontal.
These forces interact to allow the cart to move up at a constant speed, despite gravity's pull. Understanding the role of each force helps in calculating the work done on the cart.
Work and Energy
Work is a vital concept in physics that describes the process of energy transfer when an object is moved by a force. In this example, the work done by various forces helps us understand how energy is utilized as the cart moves.

Calculating Work Done

Work is defined as the force applied times the displacement in the direction of that force. It's expressed as:\[ W = F \, \cdot \, d \, \cdot \, \cos(\phi) \]Where:
  • \( W \) is the work done.
  • \( F \) is the force applied.
  • \( d \) is the displacement.
  • \( \phi \) is the angle between the force and the direction of movement.
In our scenario:
  • The gravitational force does work by opposing the upward motion of the cart, calculated as \( W_g \)
  • The normal force does no work because it acts perpendicular to the displacement.
  • The pushing force does positive work, counteracting gravity as \( W_P \)
Understanding work in terms of energy conservation helps us determine how forces balance each other out to sustain motion.
Inclined Planes
Inclined planes, like ramps, are surfaces that are tilted at an angle to the horizontal. They are crucial for understanding how forces work on slopes and they make it easier to move heavy objects up or down by reducing the force needed.

Analyzing Forces on Inclined Planes

When dealing with inclined planes, one must account for forces acting parallel and perpendicular to the plane:
  • The gravitational force needs to be split into components: parallel (causing the object to slide down) and perpendicular (balanced by the normal force).
  • The parallel component of gravity is \( m g \sin(\theta) \), where \( \theta \) is the incline angle.
  • The normal force, \( F_N \), counters the perpendicular component of gravity, calculated as \( m g \cos(\theta) \).
  • The pushing force must have a component overcoming the parallel gravitational pull to move the cart upwards.
Knowing how to break down these forces allows us to comprehend how objects can be moved more efficiently on slopes, demonstrating the practicality of inclined planes.

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

(II) An \(85 - \mathrm { g }\) arrow is fired from a bow whose string exerts an average force of 105\(\mathrm { N }\) on the arrow over a distance of 75\(\mathrm { cm } .\) What is the speed of the arrow as it leaves the bow?

(III) An elevator cable breaks when a 925 -kg elevator is 22.5\(\mathrm { m }\) above the top of a huge spring \(( k =\) \(8.00 \times 10 ^ { 4 } \mathrm { N } / \mathrm { m } )\) at the bottom of the shaft. Calculate (a) the work done by gravity on the elevator before it hits the spring; \(( b )\) the speed of the elevator just betore striking the spring; \(( c )\) the amount the spring compresses (note that here work is done by both the spring and gravity.

A \(6.10 - \mathrm { kg }\) block is pushed 9.25\(\mathrm { m }\) up a smooth \(37.0 ^ { \circ }\) inclined plane by a horizontal force of 75.0\(\mathrm { N }\) . If the initial speed of the block is 3.25\(\mathrm { m } / \mathrm { s }\) up the plane, calculate \(( a )\) the initial kinetic energy of the block; \(( b )\) the work done by the 75.0 -N force; \(( c )\) the work done by gravity; \(( d )\) the work done by the normal force; \(( e )\) the final kinetic energy of the block.

(II) A baseball \(( m = 145 \mathrm { g } )\) traveling 32\(\mathrm { m } / \mathrm { s }\) moves a fielder's glove backward 25\(\mathrm { cm }\) when the ball is caught. What was the average force exerted by the ball on the glove?

Consider a force \(F_{1}=A / \sqrt{x}\) which acts on an object during its journey along the \(x\) axis from \(x=0.0\) to \(x=1.0 \mathrm{~m},\) where \(A=2.0 \mathrm{~N} \cdot \mathrm{m}^{1 / 2},\) Show that during this journey, even though \(F_{1}\) is infinite at \(x=0.0\), the work done on the object by this force is finite.

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.