/*! 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 49 Block Pulled at Constant Speed A... [FREE SOLUTION] | 91Ó°ÊÓ

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Block Pulled at Constant Speed A \(100 \mathrm{~kg}\) block is pulled at a constant speed of \(5.0 \mathrm{~m} / \mathrm{s}\) across a horizontal floor by an applied force of \(122 \mathrm{~N}\) directed \(37^{\circ}\) above the horizontal. What is the rate at which the force does work on the block?

Short Answer

Expert verified
The rate at which the force does work on the block is 488 W.

Step by step solution

01

Identify the given data

The mass of the block: \( m = 100 \ \text{kg} \)The speed of the block: \( v = 5.0 \ \text{m/s} \)The applied force: \( F = 122 \ \text{N} \)The angle of the force above the horizontal: \( \theta = 37^{\text{∘}} \)
02

Understand the concept of work done by a force

Work done by a force is given by the formula: \( W = F \times d \times \cos{\theta} \). When the object moves with constant speed, the distance \( d \) is not required to find the work rate, as we can relate the power and work done.
03

Calculate the rate of work done (Power)

Since power is the rate at which work is done, it can be calculated using the formula: \( P = F \times v \times \cos{\theta} \).
04

Substitute the known values

Substitute \( F = 122 \ \text{N} \), \( v = 5.0 \ \text{m/s} \), and \( \theta = 37^{\text{∘}} \):\[ P = 122 \ \text{N} \times 5.0 \ \text{m/s} \times \cos{37^{\text{∘}}} \]
05

Calculate \( \cos{37^{\text{∘}}} \)

\( \cos{37^{\text{∘}}} \approx 0.8 \)
06

Perform the final calculation

Using the values:\[ P = 122 \ \text{N} \times 5.0 \ \text{m/s} \times 0.8 \]\[ P = 488 \ \text{W} \]

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Key Concepts

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

power calculation
To understand the rate at which work is done by a force, it's essential to grasp the concept of power. Power is defined as the rate at which work is done or energy is transferred. The formula to calculate power (\text{P}) when an object is moving at a constant speed is given by: \[P = F \times v \times \text{cos}(\theta)\] where \(F\) is the applied force, \(v\) is the constant velocity, and \(\text{cos}(\theta)\) is the cosine of the angle between the force direction and the direction of motion.

In our exercise, we calculated power using the given data: force \(F = 122 \text{ N}\), velocity \(v = 5.0 \text{ m/s}\), and angle \(\theta = 37^\text{∘}\). By plugging these values into the formula and knowing that \(\text{cos}(37^\text{∘}) \approx 0.8\), we found that the power is \(488 \text{ W}\).

This means that the force is doing work at a rate of \(488 \text{ Watts}\).
constant speed
When an object moves at a constant speed, it means its velocity does not change over time. In physics, moving at constant speed implies that the net force acting on the object is zero. This is because any force applied to the object is balanced by other forces, such as friction or air resistance.

In the exercise, the block is moving at a constant speed of \(5.0 \text{ m/s}\). This lets us know that the horizontal component of the applied force balances out the resistive forces (like friction). It's crucial to understand that even though the speed is constant, work is still being done because there is displacement and an applied force.

At constant speed, the entire process simplifies power calculation as we only need to consider the force component in the direction of motion without worrying about acceleration.
horizontal force component
Forces often act at an angle, and splitting them into components helps us understand their effects. When dealing with forces at an angle, it's crucial to break them into horizontal and vertical components using trigonometric functions.

In our exercise, the force of \(122 \text{ N}\) is applied at \(37^\text{∘}\) above the horizontal. To find the horizontal component of this force, we use the cosine function: \(F_{\text{horizontal}} = F \times \text{cos}(\theta)\).

Given \(F = 122 \text{ N}\) and \( \theta = 37^\text{∘}\), we have: \[F_{\text{horizontal}} = 122 \text{ N} \times \text{cos}(37^\text{∘}) \approx 122 \text{ N} \times 0.8 \approx 97.6 \text{ N}\]

The horizontal component \(97.6 \text{ N}\) is the effective force doing the work in moving the block horizontally. Understanding this helps in calculating the power correctly and in analyzing the actual force moving the object.

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Most popular questions from this chapter

Freight Car A railroad freight car of mass \(3.18 \times 10^{4} \mathrm{~kg}\) collides with a stationary caboose car. They couple together, and \(27.0 \%\) of the initial kinetic energy is transferred to nonconservative forms of energy (thermal, sound, vibrational, and so on). Find the mass of the caboose. Hint: Translational momentum is conserved.

Lowering a Block A cord is used to vertically lower an initially stationary block of mass \(M\) at a constant downward acceleration of \(g / 4\). When the block has fallen a distance \(d\), find (a) the work done by the cord's force on the block, (b) the work done by the gravitational force on the block, (c) the kinetic energy of the block, and (d) the speed of the block.

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Fan Carts \(\mathbf{P \& E}\) Two fan carts labeled \(A\) and \(B\) are placed on opposite sides of a table with their fans pointed in the same direction as shown in Fig. 9-40. Cart \(A\) is weighted with iron bars so it is twice as massive as cart B. When each fan is turned on, it provides the same constant force on the cart independent of its mass. Assume that friction is small enough to be neglected. The fans are set with a timer so that after they are switched on, they stay on for a fixed length of time, \(\Delta t\), and then turn off. (a) Just after the fans turn off, which of the following statements is true about the magnitude of the momenta of the two carts? (i) \(p_{A}>p_{B}\) (ii) \(p_{A}=p_{B}\) (iii) \(p_{A}K_{B}\) (ii) \(K_{A}=K_{B}\) (iii) \(K_{A}

Coin on a Frictionless Plane A coin slides over a frictionless plane and across an \(x y\) coordinate system from the origin to a point with \(x y\) coordinates \((3.0 \mathrm{~m}, 4.0 \mathrm{~m})\) while a constant force acts on it. The force has magnitude \(2.0 \mathrm{~N}\) and is directed at a counterclockwise angle of \(100^{\circ}\) from the positive direction of the \(\bar{x}\) axis. How much work is done by the force on the coin during the displacement?

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