/*! 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

Large Meteorite vs. TNT On August 10,1972, a large meteorite skipped across the atmosphere above western United States and Canada, much like a stone skipped across water. The accompanying fireball was so bright that it could be seen in the daytime sky (see Fig. \(9-22\) for a similar event). The meteorite's mass was about \(4 \times 10^{6} \mathrm{~kg}\) : its speed was about \(15 \mathrm{~km} / \mathrm{s}\). Had it entered the atmosphere vertically, it would have hit Earth's surface with about the same speed. (a) Calculate the meteorite's loss of kinetic energy (in joules) that would have been associated with the vertical impact. (b) Express the energy as a multiple of the explosive energy of 1 megaton of \(\mathrm{TNT}\), which is \(4.2 \times 10^{15} \mathrm{~J}\). (c) The energy associated with the atomic bomb explosion over Hiroshima was equivalent to 13 kilotons of TNT. To how many Hiroshima bombs would the meteorite impact have been equivalent?

Two Pulleys and a Canister In Fig. \(9-28\), a cord runs around two massless, frictionless pulleys; a canister with mass \(m=20 \mathrm{~kg}\) hangs from one pulley; and you exert a force \(\vec{F}\) on the free end of the cord. (a) What must be the magnitude of \(\vec{F}\) if you are to lift the canister at a constant speed? (b) To lift the canister by \(2.0 \mathrm{~cm}\), how far must you pull the free end of the cord? During that lift, what is the work done on the canister by (c) your force (via the cord) and (d) the gravitational force on the canister? (Hint: When a cord loops around a pulley as shown, it pulls on the pulley with a net force that is twice the tension in the cord.)

Block Dropped on a Spring A \(250 \mathrm{~g}\) block is dropped onto a relaxed vertical spring that has a spring constant of \(k=\) \(2.5 \mathrm{~N} / \mathrm{cm}\) (Fig. \(9-29)\). The block becomes attached to the spring and compresses the spring \(12 \mathrm{~cm}\) before turning around. While the spring is being compressed, what work is done on the block by (a) the gravitational force on it and (b) the spring force? (c) What is the speed of the block just before it hits the spring? (Assume that friction is negligible.) (d) If the speed at impact is doubled, what is the maximum compression of the spring?

Swimmer A swimmer moves through the water at a constant speed of \(0.22 \mathrm{~m} / \mathrm{s}\). The average drag force opposing this motion is \(110 \mathrm{~N}\). What average power is required of the swimmer?

Rope Tow A skier is pulled by a tow rope up a frictionless ski slope that makes an angle of \(12^{\circ}\) with the horizontal. The rope moves parallel to the slope with a constant speed of \(1.0 \mathrm{~m} / \mathrm{s}\). The force of the rope does \(900 \mathrm{~J}\) of work on the skier as the skier moves a distance of \(8.0 \mathrm{~m}\) up the incline. (a) If the rope moved with a constant speed of \(2.0 \mathrm{~m} / \mathrm{s}\), how much work would the force of the rope do on the skier as the skier moved a distance of \(8.0 \mathrm{~m}\) up the incline? At what rate is the force of the rope doing work on the skier when the rope moves with a speed of (b) \(1.0 \mathrm{~m} / \mathrm{s}\) and \((\mathrm{c})\) \(2.0 \mathrm{~m} / \mathrm{s} ?\)

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