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A crate with mass 32.5 kg initially at rest on a warehouse floor is acted on by a net horizontal force of 14.0 N. (a) What acceleration is produced? (b) How far does the crate travel in 10.0 s? (c) What is its speed at the end of 10.0 s?

Short Answer

Expert verified
(a) 0.431 m/sĀ², (b) 21.55 m, (c) 4.31 m/s.

Step by step solution

01

Identify the Given Data

To solve the problem, we first need to identify the given values:- Mass of the crate \( m = 32.5 \text{ kg} \).- Net horizontal force \( F = 14.0 \text{ N} \).- Initial velocity \( u = 0 \text{ m/s} \) (since the crate is initially at rest).- Time \( t = 10.0 \text{ s} \).
02

Calculate the Acceleration

Use Newton's second law to find the acceleration:\[ F = m \cdot a \]Where \( F \) is the force, \( m \) is the mass, and \( a \) is the acceleration. Rearrange the formula to solve for \( a \):\[ a = \frac{F}{m} = \frac{14.0}{32.5} \text{ m/s}^2 \approx 0.431 \text{ m/s}^2 \].
03

Calculate the Distance Travelled

Use the kinematic equation for distance:\[ s = ut + \frac{1}{2} a t^2 \]Since the initial velocity \( u = 0 \), the equation simplifies to:\[ s = \frac{1}{2} \times 0.431 \times (10.0)^2 \]Calculate:\[ s = \frac{1}{2} \times 0.431 \times 100 = 21.55 \text{ m} \].
04

Calculate the Final Speed

Use the kinematic equation for the final velocity:\[ v = u + at \]Since \( u = 0 \):\[ v = 0 + 0.431 \times 10.0 \]Calculate:\[ v = 4.31 \text{ m/s} \].

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Key Concepts

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

Kinematic Equations
Kinematic equations play a crucial role when analyzing the motion of objects under the influence of constant forces. These equations allow us to predict an object's movement through parameters such as initial velocity, final velocity, acceleration, time, and displacement.

The basic set of kinematic equations include:
  • Final velocity: \( v = u + at \)
  • Displacement: \( s = ut + \frac{1}{2} a t^2 \)
  • Final velocity squared: \( v^2 = u^2 + 2as \)
In these formulas, \( u \) is the initial velocity, \( v \) is the final velocity, \( a \) is the acceleration, \( t \) accounts for the time, and \( s \) represents displacement.

For example, if you know the object's acceleration and initial velocity, you can calculate how far it will travel over a given period by simply substituting values into the displacement equation. In the problem, since the crate was initially at rest, using the simplification for initial velocity (\( u = 0 \)) showed how to directly compute the distance with just acceleration and time values.
Acceleration Calculation
Determining an object's acceleration becomes intuitive when using Newton's Second Law of motion. This law states that the acceleration \( a \) of an object is directly proportional to the net force \( F \) acting upon it and inversely proportional to its mass \( m \). The mathematical expression for this law is:
  • \( a = \frac{F}{m} \)
In our example, since the force applied to the crate is 14.0 N, and its mass is 32.5 kg, substituting these values into Newtonā€™s formula gives:
\( a = \frac{14.0}{32.5} \approx 0.431 \text{ m/s}^2 \).

This acceleration means for every second, the crate's velocity changes by approximately 0.431 meters per second. Understanding the relationship between force, mass, and acceleration allows us to predict how objects will behave when forces are applied to them.
Force and Motion
The interaction between force and motion can be effectively understood by exploring Newton's Second Law. Newton's Second Law provides a framework to analyze how a force will change an object's motion.

When a net force is exerted on an object, it causes the object to accelerate in the direction of the force, proportional to the magnitude of the net force and inversely proportional to the object's mass. In simpler terms, heavier objects require more force to achieve the same acceleration as lighter ones.

Let's consider the crate example: a net horizontal force of 14.0 N causes it to accelerate at approximately 0.431 m/sĀ². This change in motion over time results in two important outcomes:
  • The crate's position changes (it moves a distance, calculated using kinematic equations).
  • The crate's speed increases (final speed can be determined using its acceleration and the time factor).
This understanding helps visualize how varied forces alter motions, affecting factors such as distance traveled and speed achieved over time. It brings to life the intricate link between force and the resulting motion, as demonstrated with our example of the crate on a warehouse floor.

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Most popular questions from this chapter

An 8.00-kg box sits on a level floor. You give the box a sharp push and find that it travels 8.22 m in 2.8 s before coming to rest again. (a) You measure that with a different push the box traveled 4.20 m in 2.0 s. Do you think the box has a constant acceleration as it slows down? Explain your reasoning. (b) You add books to the box to increase its mass. Repeating the experiment, you give the box a push and measure how long it takes the box to come to rest and how far the box travels. The results, including the initial experiment with no added mass, are given in the table: In each case, did your push give the box the same initial speed? What is the ratio between the greatest initial speed and the smallest initial speed for these four cases? (c) Is the average horizontal force \(f\) exerted on the box by the floor the same in each case? Graph the magnitude of force \(f\) versus the total mass \(m\) of the box plus its contents, and use your graph to determine an equation for \(f\) as a function of \(m\).

Two dogs pull horizontally on ropes attached to a post; the angle between the ropes is 60.0\(^\circ\). If Rover exerts a force of 270 N and Fido exerts a force of 300 N, find the magnitude of the resultant force and the angle it makes with Rover's rope.

The froghopper (\(Philaenus spumarius\)), the champion leaper of the insect world, has a mass of 12.3 mg and leaves the ground (in the most energetic jumps) at 4.0 m/s from a vertical start. The jump itself lasts a mere 1.0 ms before the insect is clear of the ground. Assuming constant acceleration, (a) draw a free-body diagram of this mighty leaper during the jump; (b) find the force that the ground exerts on the froghopper during the jump; and (c) express the force in part (b) in terms of the froghopper's weight.

Crates \(A\) and \(B\) sit at rest side by side on a frictionless horizontal surface. They have masses \(m_A\) and \(m_B\), respectively. When a horizontal force \(\vec{F}\) is applied to crate \(A\), the two crates move off to the right. (a) Draw clearly labeled free-body diagrams for crate \(A\) and for crate \(B\). Indicate which pairs of forces, if any, are third-law action-reaction pairs. (b) If the magnitude of \(\vec{F}\)is less than the total weight of the two crates, will it cause the crates to move? Explain.

You have just landed on Planet X. You release a 100-g ball from rest from a height of 10.0 m and measure that it takes 3.40 s to reach the ground. Ignore any force on the ball from the atmosphere of the planet. How much does the 100-g ball weigh on the surface of Planet X?

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