/*! 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 29 A 45.0 -kg crate of tools rests ... [FREE SOLUTION] | 91Ó°ÊÓ

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A 45.0 -kg crate of tools rests on a horizontal floor. You exert a gradually increasing horizontal push on it and observe that the crate just begins to move when your force exceeds 313 \(\mathrm{N}\) . After that you must reduce your push to 208 \(\mathrm{N}\) to keep it moving at a steady 25.0 \(\mathrm{cm} / \mathrm{s}\) (a) What are the coefficients of static and kinetic friction between the crate and the floor? (b) What push must you exert to give it an acceleration of 1.10 \(\mathrm{m} / \mathrm{s}^{2} ?\) (c) Suppose you were performing the same experiment on this crate but were doing it on the moon instead, where the acceleration due to gravity is 1.62 \(\mathrm{m} / \mathrm{s}^{2}\) . (i) What magnitude push would cause it to move? (ii) What would its acceleration be if you maintained the push in part (b)?

Short Answer

Expert verified
(a) \( \mu_s \approx 0.71 \), \( \mu_k \approx 0.47 \); (b) 257.5 N; (c)(i) 51.76 N, (ii) 4.96 m/s².

Step by step solution

01

Identify Given Information

We have a crate with mass \( m = 45.0 \text{ kg} \). The force required to initiate movement is \( F_s = 313 \text{ N} \) and the force required to maintain constant velocity is \( F_k = 208 \text{ N} \). We will find the coefficients of static friction \( \mu_s \) and kinetic friction \( \mu_k \).
02

Calculate the Normal Force

The normal force \( N \) on an object resting on a horizontal surface is equal to its weight. Thus, \( N = mg \), where \( g = 9.8 \text{ m/s}^2 \). Therefore, \( N = 45.0 \times 9.8 = 441 \text{ N} \).
03

Find Coefficient of Static Friction

The coefficient of static friction \( \mu_s \) can be found using the formula \( F_s = \mu_s N \). Solving for \( \mu_s \), we get: \[ \mu_s = \frac{F_s}{N} = \frac{313}{441} \approx 0.71 \]
04

Find Coefficient of Kinetic Friction

The coefficient of kinetic friction \( \mu_k \) can be found using the formula \( F_k = \mu_k N \). Solving for \( \mu_k \), we get: \[ \mu_k = \frac{F_k}{N} = \frac{208}{441} \approx 0.47 \]
05

Calculate Force for a Given Acceleration

To find the force \( F \) required to accelerate the crate at \( a = 1.10 \text{ m/s}^2 \), use the equation: \[ F = ma + F_k = 45.0 \times 1.10 + 208 \] \[ F = 49.5 + 208 = 257.5 \text{ N} \]
06

Moon Experiment - Calculate Moon Normal Force and Static Friction

On the moon, the gravitational acceleration is \( g = 1.62 \text{ m/s}^2 \). The normal force becomes \( N = mg = 45 \times 1.62 = 72.9 \text{ N} \). Thus, \( F_s = \mu_s N = 0.71 \times 72.9 \approx 51.76 \text{ N} \).
07

Moon Experiment - Calculate Acceleration with Given Force

Using the force \( F = 257.5 \text{ N} \) (from part b) on the moon and the kinetic friction, we find \( F_k = \mu_k N = 0.47 \times 72.9 \approx 34.26 \text{ N} \). The net force \( F_{net} = F - F_k = 257.5 - 34.26 = 223.24 \text{ N} \).\[ a = \frac{F_{net}}{m} = \frac{223.24}{45} \approx 4.96 \text{ m/s}^2 \]

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Key Concepts

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

Static Friction
Static friction is the resistance that keeps an object at rest when a force is applied to it. It must be overcome to set the object in motion. This frictional force opposes the initial movement of the object, maintaining it stationary until the applied force is sufficiently high.
In the exercise provided, static friction is what kept the 45.0-kg crate from moving until we applied a force greater than 313 N.
The formula to calculate static friction is \[ F_s = \mu_s N \]where:
  • \( F_s \) is the force of static friction,
  • \( \mu_s \) is the coefficient of static friction,
  • \( N \) is the normal force.
By using the known maximum static force and the normal force of 441 N, we found the static friction coefficient to be approximately 0.71 in this example.
Kinetic Friction
Once an object is in motion, kinetic friction comes into play. This is the force opposing the object's movement as it slides over a surface. Unlike static friction, kinetic friction remains constant once the object starts moving. It is usually less than static friction for the same pair of surfaces.
For the 45.0-kg crate, after it started moving, the kinetic friction required to maintain its motion was met with a 208 N force.
The equation for kinetic friction is:\[ F_k = \mu_k N \]where:
  • \( F_k \) is the force of kinetic friction,
  • \( \mu_k \) is the coefficient of kinetic friction,
  • \( N \) is the normal force.
Through calculation, the coefficient for kinetic friction in this case turned out to be approximately 0.47.
Normal Force
The normal force is an essential concept in understanding friction. It acts perpendicular to the surface on which an object rests. This force balances the object's weight when on a flat surface, thereby preventing it from falling through. In our scenario, the crate's normal force is equivalent to its weight, calculated as the product of mass and gravitational acceleration.
For the crate with a mass of 45.0 kg on Earth:\[ N = mg \]\[ N = 45.0 \times 9.8 = 441 \text{ N} \] This formula becomes crucial when calculating both static and kinetic frictions, because these frictions depend directly on the normal force.
Acceleration
Acceleration is the rate at which the velocity of an object changes. It reflects how quickly an object speeds up, slows down, or changes direction. In the exercise, we needed to apply additional force to accelerate the crate at a rate of 1.10 m/s².
The force required to achieve this acceleration, after considering kinetic friction, is calculated using Newton's second law:\[ F = ma + F_k \]where:
  • \( F \) is the total force applied,
  • \( m \) is the mass of the object (45 kg),
  • \( a \) is the desired acceleration (1.10 m/s²),
  • \( F_k \) is the kinetic friction (208 N).
Hence, the total initial force required to accelerate the crate is 257.5 N.
Gravitational Acceleration
Gravitational acceleration is the acceleration due to the force of gravity. On Earth, this acceleration is approximately 9.8 m/s². However, it varies depending on the celestial body.
In the moon experiment, gravitational acceleration changed to 1.62 m/s², altering the normal force and subsequently the forces of static and kinetic frictions.
This lower gravitational pull meant a smaller force was sufficient to move the crate on the moon compared to Earth.
  • Normal force on moon: \( N = 45 \times 1.62 = 72.9 \text{ N} \)
  • Maximum static force on moon: \( F_s = \mu_s N \approx 51.76 \text{ N} \)
Understanding gravitational acceleration is crucial as it directly impacts how forces like friction depend on weight, varying as gravity varies.

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Most popular questions from this chapter

Block \(A\) in Fig. P5.72 weighs 60.0 \(\mathrm{N} .\) The coefficient of static friction between the block and the surface on which it rests is \(0.25 .\) The weight \(w\) is 12.0 \(\mathrm{N}\) and the system is in equilibrium. (a) Find the friction force exerted on block \(A .\) (b) Find the maximum weight \(w\) for which the system will remain in equilibrium.

A pickup truck is carrying a toolbox, but the rear gate of the truck is missing, so the box will slide out if it is set moving. The coefficients of kinetic and static friction between the box and the bed of the truck are 0.355 and 0.650 , respectively. Starting from rest, what is the shortest time this truck could accelerate uniformly to 30.0 \(\mathrm{m} / \mathrm{s}\) without causing the box to slide? Include a free-body diagram of the toolbox as part of your solution.

A horizontal wire holds a solid uniform ball of mass \(m\) in place on a tilted ramp that rises \(35.0^{\circ}\) above the horizontal. The surface of this ramp is perfectly smooth, and the wire is directed away from the center of the ball (Fig. P5.60). (a) Draw a free-body diagram for the ball. (b) How hard does the surface of the ramp push on the ball? (c) What is the tension in the wire?

A 2.00 -kg box is moving to the right with speed 9.00 \(\mathrm{m} / \mathrm{s}\) on a horizontal, frictionless surface. At \(t=0\) a horizontal force is applied to the box. The force is directed to the left and has magnitude \(F(t)=\left(6.00 \mathrm{N} / \mathrm{s}^{2}\right) t^{2}\) . (a) What distance does the box move from its position at \(t=0\) before its speed is reduced to zero? (b) If the force continues to be applied, what is the speed of the box at \(t=3.00 \mathrm{s} ?\)

Two blocks with masses 4.00 \(\mathrm{kg}\) and 8.00 \(\mathrm{kg}\) are connected by a string and slide down a \(30.0^{\circ}\) inclined plane (Fig. \(\mathrm{P5.98).~The~}\) coefficient of kinetic friction between the \(4.00-\) kg block and the plane is \(0.25 ;\) that between the 8.00 -kg block and the plane is 0.35 (a) Calculate the acceleration of each block. (b) Calculate the tension in the string. (c) What happens if the positions of the blocks are reversed, so the \(4.00-\mathrm{kg}\) block is above the 8.00 -kg block?

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