/*! 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 36 A 9.75-m ladder with a mass of \... [FREE SOLUTION] | 91Ó°ÊÓ

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A 9.75-m ladder with a mass of \(23.2 \mathrm{kg}\) lies flat on the ground. A painter grabs the top end of the ladder and pulls straight upward with a force of \(245 \mathrm{N}\). At the instant the top of the ladder leaves the ground, the ladder experiences an angular acceleration of \(1.80 \mathrm{rad} / \mathrm{s}^{2}\) about an axis passing through the bottom end of the ladder. The ladder's center of gravity lies halfway between the top and bottom ends. (a) What is the net torque acting on the ladder? (b) What is the ladder's moment of inertia?

Short Answer

Expert verified
Net torque: 84.75 Nm; Moment of inertia: 47.08 kg·m².

Step by step solution

01

Understanding the Concept of Torque

To find the net torque, we need to understand that torque (\( \tau \)) is the rotational equivalent of force, given by the formula \( \tau = r \cdot F \cdot \sin(\theta) \), where \( r \) is the distance from the axis of rotation to the point where the force is applied, \( F \) is the force applied, and \( \theta \) is the angle between \( r \) and \( F \). In this scenario, the force is applied perpendicular to the ladder, so \( \theta = 90^\circ \)and \( \sin(90^\circ) = 1 \). The center of gravity is at the midpoint, 4.875 m from the bottom.
02

Calculate the Force of Gravity

The force of gravity acting on the ladder is given by its weight, calculated using \( F_{gravity} = m \cdot g \), where \( m = 23.2 \text{ kg}\) is the mass of the ladder and \( g \approx 9.81 \, \text{m/s}^2 \) is the acceleration due to gravity. So, \( F_{gravity} = 23.2 \, \text{kg} \cdot 9.81 \, \text{m/s}^2 = 227.592 \, \text{N} \).
03

Determine Net Torque

Calculate the torque due to the force of gravity (\( \tau_{gravity} = r \cdot F_{gravity} \)) and subtract it from the torque due to the applied force (\( \tau_{applied} = r \cdot F_{applied} \)). \( \tau_{applied} = 0.875 \cdot 245 = 1193.75 \, \text{Nm} \)\( \tau_{gravity} = 4.875 \cdot 227.592 = 1109.00 \, \text{Nm} \)Net torque \( \tau_{net} = \tau_{applied} - \tau_{gravity} = 1193.75 - 1109.00 = 84.75 \, \text{Nm} \)
04

Understand the Moment of Inertia

The moment of inertia (\( I \)) of an object represents its resistance to rotational acceleration. It can be calculated when torque and angular acceleration are known using the formula \( \tau = I \cdot \alpha \), where \( \alpha = 1.80 \, \text{rad/s}^{2} \)is the angular acceleration.
05

Calculate the Moment of Inertia

Rearrange the torque formula to find \( I = \frac{\tau}{\alpha} \). Using the net torque from Step 3 and the given angular acceleration:\[ I = \frac{84.75 \, \text{Nm}}{1.80 \, \text{rad/s}^{2}} = 47.0833 \, \text{N\,m}\,s^2 = \text{kg}\,\text{m}^2 \]
06

Conclusion

The net torque acting on the ladder is 84.75 Nm. The ladder's moment of inertia is \( 47.0833 \, \text{kg} \cdot \text{m}^2 \).

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Key Concepts

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

Understanding Torque Calculation
Torque is like the rotational twin of force. When you want to make something rotate—like a wheel or, in this case, a ladder—you need to apply a torque. Think about pushing a door open: you apply the force at a distance from the hinge to make it swing. Here, in our ladder problem, the formula to determine torque \( \tau \) is \( \tau = r \cdot F \cdot \sin(\theta) \). Here’s what each element means:
  • \( r \): The 'lever arm' or distance from the pivot point—in our scenario, halfway down the ladder at 4.875 meters from the end.
  • \( F \): The applied force—which is provided by our friendly painter pulling with 245 N.
  • \( \theta \): The angle between \( r \) and \( F \). Our ladder is being pulled straight up, making the angle 90 degrees, and the sine of 90 is 1.
To calculate net torque, consider both the force of the painter and the gravitational pull at the center of gravity. Subtract the gravitational torque from the applied torque to get a net torque of 84.75 Nm. This tells us how much rotational power is being applied to the ladder.
Exploring Angular Acceleration
Angular acceleration is how quickly something speeds up or slows down its spinning. Unlike linear acceleration, which relates to straight-line motion, angular acceleration works on circular paths. It measures how quickly the rotational speed, or angular velocity, of an object changes. The unit is radians per second squared (\( \text{rad/s}^2 \)).

If you've ever spun a wheel, you might notice that it starts slowly and then speeds up. Angular acceleration is the measure of this speeding up. In our case, the ladder experiences an angular acceleration of \( 1.80 \text{ rad/s}^2 \) as it begins to lift from the ground. Since torque is directly related to angular acceleration (\( \tau = I \cdot \alpha \)), knowing the angular acceleration helps us solve for the moment of inertia, showing the ladder’s resistance to this rotational change.
Center of Gravity in Action
The center of gravity is the balancing point of an object. Think about balancing a spoon on your finger: it stays flat if your finger is under its center of gravity. For our ladder, the center of gravity is crucial because it influences stability and rotation. By situating at the midpoint, 4.875 meters from either end, it determines where you calculate gravitational force's torque.
  • In practical terms, this midpoint is where all the ladder's mass can be considered concentrated for calculations related to weight and balance.
  • When the ladder is lifted, gravity acts here, making this point critical for figuring out how much torque gravity actually contributes.
Recognizing the center of gravity helps you grasp not just balance but also how weight distribution affects torque and rotation, as shown in this textbook problem with our artistically inclined ladder.

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Most popular questions from this chapter

A man drags a 72 -kg crate across the floor at a constant velocity by pulling on a strap attached to the bottom of the crate. The crate is tilted \(25^{\circ}\) above the horizontal, and the strap is inclined \(61^{\circ}\) above the horizontal. The center of gravity of the crate coincides with its geometrical center, as indicated in the drawing. Find the magnitude of the tension in the strap.

Multiple-Concept Example 10 offers useful background for problems like this. A cylinder is rotating about an axis that passes through the center of each circular end piece. The cylinder has a radius of \(0.0830 \mathrm{m}\), an angular speed of \(76.0 \mathrm{rad} / \mathrm{s},\) and a moment of inertia of \(0.615 \mathrm{kg} \cdot \mathrm{m}^{2} . \mathrm{A}\) brake shoe presses against the surface of the cylinder and applies a tangential frictional force to it. The frictional force reduces the angular speed of the cylinder by a factor of two during a time of 6.40 s. (a) Find the magnitude of the angular deceleration of the cylinder. (b) Find the magnitude of the force of friction applied by the brake shoe.

Two spheres are each rotating at an angular speed of \(24 \mathrm{rad} / \mathrm{s}\) about axes that pass through their centers. Each has a radius of \(0.20 \mathrm{m}\) and a mass of 1.5 kg. However, as the figure shows, one is solid and the other is a thin-walled spherical shell. Suddenly, a net external torque due to friction (magnitude \(=0.12 \mathrm{N} \cdot \mathrm{m}\) ) begins to act on each sphere and slows the motion down. Concepts: (i) Which sphere has the greater moment of inertia and why? (ii) Which sphere has the angular acceleration (a deceleration) with the smaller magnitude? (iii) Which sphere takes a longer time to come to a halt? Calculations: How long does it take each sphere to come to a halt?

Two disks are rotating about the same axis. Disk A has a moment of inertia of \(3.4 \mathrm{kg} \cdot \mathrm{m}^{2}\) and an angular velocity of \(+7.2 \mathrm{rad} / \mathrm{s} .\) Disk \(\mathrm{B}\) is rotating with an angular velocity of \(-9.8 \mathrm{rad} / \mathrm{s} .\) The two disks are then linked together without the aid of any external torques, so that they rotate as a single unit with an angular velocity of -2.4 rad/s. The axis of rotation for this unit is the same as that for the separate disks. What is the moment of inertia of disk B?

A solid disk rotates in the horizontal plane at an angular velocity of \(0.067 \mathrm{rad} / \mathrm{s}\) with respect to an axis perpendicular to the disk at its center. The moment of inertia of the disk is \(0.10 \mathrm{kg} \cdot \mathrm{m}^{2}\). From above, sand is dropped straight down onto this rotating disk, so that a thin uniform ring of sand is formed at a distance of \(0.40 \mathrm{m}\) from the axis. The sand in the ring has a mass of \(0.50 \mathrm{kg} .\) After all the sand is in place, what is the angular velocity of the disk?

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