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QiC A shopper in a supermarket pushes a cart with a force of \(35 \mathrm{~N}\) directed at an angle of \(25^{\circ}\) below the horizontal. The force is just sufficient to overcome various frictional forces, so the cart moves at constant speed. (a) Find the work done by the shopper as she moves down a \(50.0-\mathrm{m}\) length aisle. (b) What is the net work done on the cart? Why? (c) The shopper goes down the next aisle, pushing horizontally and maintaining the same speed as before. If the work done by frictional forces doesn't change, would the shopper's applied force be larger, smaller, or the same? What about the work done on the cart by the shopper?

Short Answer

Expert verified
a) The work done by the shopper is approximately 1592.5 J. b) The net work done on the cart is zero because there is no acceleration. c) The applied force by the shopper would be the same but the work done would be larger since all the applied force is now in the direction of motion.

Step by step solution

01

Calculation of Work Done by the Shopper

The work done by the shopper is given by the formula: Work = Force x Distance x cos(θ). Here, Force = 35N, Distance = 50m, and θ = 25°. Therefore, Work = 35N x 50m x cos(25°). Let's calculate this.
02

Find the Net Work Done on the Cart

The net work done on the cart is the work done by the shopper minus the work done by friction. However, since the cart is moving at a constant speed, these two amounts of work must balance out to zero. So, the net work done on the cart is zero.
03

Comparison of Forces and Work in different situations

In the second situation, the shopper is applying force horizontally, so her applied force would be the same as before because the work done by frictional forces doesn't change and the cart's speed also remains unchanged. However, because the force is applied entirely in the direction of motion, all of the shopper's effort is directed to doing work against friction. Thus, the work done by the shopper on the cart will be larger in this case.

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Key Concepts

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

Work-Energy Principle
Understanding the work-energy principle is essential for solving many problems in physics, including this exercise involving a shopper pushing a cart in a supermarket. The work-energy principle states that the work done on an object is equal to the change in its kinetic energy. In mathematical terms, this is expressed as:
\[ \text{Work done} = \Delta \text{Kinetic Energy} \]
When the shopper applies a force to move the cart at a constant speed, there is no change in kinetic energy. Therefore, any work done by the shopper is used to overcome frictional forces. In the given problem, since the cart moves at constant speed, the kinetic energy remains unchanged, implying that the net work done on the cart is zero.
However, we also use the more specific formula for calculating the work done when a force is applied at an angle:
\[ \text{Work} = \text{Force} \times \text{Distance} \times \cos(\theta) \]
Applying this formula to the shopper's problem, we calculated the work done in overcoming friction as the cart moved along the aisle. This understanding of how work relates directly to kinetic energy provides insight into many real-world scenarios where forces act on objects.
Frictional Forces
Frictional forces play a significant role in everyday activities, such as pushing a shopping cart in a supermarket. Friction is the resistive force that occurs when two surfaces move across each other. It acts opposite to the direction of motion and can significantly affect the amount of work done when an object is moved.
In our example, frictional forces must be overcome for the shopper to move the cart. These forces include rolling resistance from the cart wheels and air resistance. The force that the shopper applies must be equal to the frictional force to maintain constant speed, as any additional force would accelerate the cart.
Thus, when calculating the work done by the shopper on the cart, it's important to note that all of it goes into overcoming these frictional forces. This holds true as long as the cart's speed doesn't change, meaning the applied force is transforming completely into work to counteract friction, with no surplus force contributing to an increase in kinetic energy.
Constant Speed

Maintaining Equilibrium

When an object, such as a shopping cart, is pushed at a constant speed, it's in a state of dynamic equilibrium. This means that all the forces acting on the cart balance out. The force applied by the shopper equals the frictional force opposing the cart's motion, resulting in no net force and therefore no acceleration.

Implications of Constant Speed on Work Done

Maintaining constant speed has implications for the work being done on an object. As our step-by-step solution pointed out, when a shopper moves a cart down an aisle with a constant speed, the work done by frictional forces equals the work done by the shopper. If the shopper were to push the cart with the same force but now directly in the direction of motion (horizontally), there would be no component of force lost to the vertical direction.
Consequently, even though the force required to maintain the constant speed remains the same, the entire magnitude of the force is now used to do work in the direction of motion, resulting in a greater amount of work being done over the same distance. This concept is crucial for understanding how forces are applied in various scenarios and how they affect the overall work done on an object.

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Most popular questions from this chapter

A light spring with force constant \(3.85 \mathrm{~N} / \mathrm{m}\) is compressed by \(8.00 \mathrm{~cm}\) as it is held between a \(0.250-\mathrm{kg}\) block on the left and a \(0.500\)-kg block on the right, both resting on a horizontal surface. The spring exerts a force on each block, tending to push them apart. The blocks are simultaneously released from rest. Find the acceleration with which each block starts to move, given that the coefficient of kinetic friction between each block and the surface is (a) 0 , (b) \(0.100\), and (c) \(0.462\).

QIC A \(0.250-\mathrm{kg}\) block along a horizontal track has a speed of \(1.50 \mathrm{~m} / \mathrm{s}\) immediately before colliding with a light spring of force constant \(4.60 \mathrm{~N} / \mathrm{m}\) located at the end of the track. (a) What is the spring's maximum compression if the track is frictionless? (b) If the track is not frictionless, would the spring's maximum compression be greater than, less than, or equal to the value obtained in part (a)?

A mechanic pushes a \(2.50 \times 10^{3}-\mathrm{kg}\) car from rest to a speed of \(v\), doing \(5000 \mathrm{~J}\) of work in the process. During this time, the car moves \(25.0 \mathrm{~m}\). Neglecting friction between car and road, find (a) \(v\) and (b) the horizontal force exerted on the car.

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A running \(62-\mathrm{kg}\) cheetah has a top speed of \(32 \mathrm{~m} / \mathrm{s}\). (a) What is the cheetah's maximum kinetic energy? (b) Find the cheetah's speed when its kinetic energy is one half of the value found in part (a).

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