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A ceiling fan is turned on and a net torque of \(1.8 \mathrm{~N} \cdot \mathrm{m}\) is applied to the blades. The blades have a total moment of inertia of \(0.22 \mathrm{~kg} \cdot \mathrm{m}^{2}\). What is the angular acceleration of the blades?

Short Answer

Expert verified
Angular acceleration is approximately 8.18 rad/s².

Step by step solution

01

Identify the formula

To find the angular acceleration, we can use Newton's second law for rotation, which states: \( \tau = I \alpha \). Here, \( \tau \) is the torque, \( I \) is the moment of inertia, and \( \alpha \) is the angular acceleration.
02

Rearrange the formula

We need to solve for \( \alpha \), the angular acceleration, from the equation \( \tau = I \alpha \). Rearranging gives: \( \alpha = \frac{\tau}{I} \).
03

Substitute known values

Now, replace \( \tau \) with \(1.8 \mathrm{~N} \cdot \mathrm{m}\) and \( I \) with \(0.22 \mathrm{~kg} \cdot \mathrm{m}^{2}\) in the formula: \( \alpha = \frac{1.8}{0.22} \).
04

Calculate the angular acceleration

Perform the calculation: \( \alpha = \frac{1.8}{0.22} \approx 8.18 \). Thus, the angular acceleration \( \alpha \) is approximately \( 8.18 \) rad/s².

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Key Concepts

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

Newton's Second Law for Rotation
When you hear about Newton's laws, you probably think of motion in a straight line. However, there is a rotational counterpart, known as Newton's second law for rotation. This law helps us understand how objects like spinning wheels, gears, and even ceiling fans behave when they're subject to forces.

According to Newton's second law for rotation, when a net torque ( \( \tau \) ) is applied to an object, it causes an angular acceleration ( \( \alpha \) ). The formula for this relationship is given by: \[ \tau = I \alpha \]Here, \( I \) represents the moment of inertia, which acts like mass in linear motion, determining how much torque is needed to get an object rotating.
  • \( \tau \) is the torque applied to the object
  • \( I \) is the moment of inertia
  • \( \alpha \) is the angular acceleration

When this formula is rearranged to find angular acceleration, you get: \( \alpha = \frac{\tau}{I} \). This fundamental law helps solve many problems involving rotating systems, making it a key tool in physics.
Torque
Torque is somewhat like force in the rotational world. It makes things spin. Imagine using a wrench to unscrew a bolt. Torque is the twisting force that the wrench applies to the bolt. It's not just about the force's strength but also about where it's applied.

Torque is calculated as the product of the applied force and the distance from the point of rotation (lever arm). Its formula is: \[ \tau = r \times F \times \sin(\theta) \]where:
  • \( \tau \) stands for torque
  • \( r \) is the distance from the axis of rotation
  • \( F \) is the applied force
  • \( \theta \) is the angle between force and lever arm

In our ceiling fan example, a net torque of \( 1.8 \, \mathrm{N} \cdot \mathrm{m} \) was applied to initiate the fan's motion. Torque effectively determines the rotational capacity of engines, bicycles, and even compact appliances.
Moment of Inertia
The moment of inertia is a key concept when dealing with rotating objects. Think of it as the rotational equivalent of mass. It tells us how difficult it is to change an object's rotational state.

In mathematical terms, the moment of inertia ( \( I \) ) depends on how an object's mass is distributed relative to its axis of rotation. A simple expression for a point mass is: \[ I = mr^2 \]where \( m \) is mass and \( r \) is the distance from the rotation axis.
  • Larger distances increase the moment of inertia
  • More mass means a higher moment of inertia

In our ceiling fan scenario, the moment of inertia was given as \( 0.22 \, \mathrm{kg} \cdot \mathrm{m}^2 \). This value directly impacts how much torque is necessary to produce a certain angular acceleration. In essence, the moment of inertia decides how much 'effort' it takes to spin or stop an object.
Ceiling Fan
Ceiling fans are a common household feature, and understanding their operation involves physics concepts like torque and moment of inertia. When a ceiling fan starts to spin, the motor provides torque, which initiates the fan blades' rotation. This movement is described by angular acceleration.

The moment of inertia of the fan blades tells us how much torque is required to change their speed. For instance, heavier or larger blades need more torque to achieve the same spin speed as lighter ones. The fan's motor is designed to handle this by supplying sufficient torque, allowing it to accelerate and circulate air in the room efficiently.
  • Fans rely on torque generated by electric motors
  • Angular acceleration determines how quickly the fan reaches its operating speed
  • The design of the blades, including their size and weight, influences their moment of inertia

By understanding these principles, one can appreciate the balance of design and physics that makes ceiling fans effective in cooling spaces.

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Most popular questions from this chapter

Calculate the kinetic energy that the earth has because of (a) its rotation about its own axis and (b) its motion around the sun. Assume that the earth is a uniform sphere and that its path around the sun is circular. For comparison, the total energy used in the United States in one year is about \(9.3 \times 10^{19} \mathrm{~J}\).

See Multiple-Concept Example 12 to review some of the concepts that come into play here. The crane shown in the drawing is lifting a 180 -kg crate upward with an acceleration of \(1.2 \mathrm{~m} / \mathrm{s}^{2} .\) The cable from the crate passes over a solid cylindrical pulley at the top of the boom. The pulley has a mass of \(130 \mathrm{~kg}\). The cable is then wound onto a hollow cylindrical drum that is mounted on the deck of the crane. The mass of the drum is \(150 \mathrm{~kg},\) and its radius is \(0.76 \mathrm{~m} .\) The engine applies a counterclockwise torque to the drum in order to wind up the cable. What is the magnitude of this torque? Ignore the mass of the cable.

Multiple-Concept Example 10 provides one model for solving this type of problem. Two wheels have the same mass and radius. One has the shape of a hoop and the other the shape of a solid disk. Each wheel starts from rest and has a constant angular acceleration with respect to a rotational axis that is perpendicular to the plane of the wheel at its center. Each makes the same number of revolutions in the same time. (a) Which wheel, if either, has the greater angular acceleration? (b) Which, if either, has the greater moment of inertia? (c) To which wheel, if either, is a greater net external torque applied? Explain your answers.

A flat uniform circular disk (radius \(=2.00 \mathrm{~m}\), mass \(=1.00 \times 10^{2} \mathrm{~kg}\) ) is initially stationary. The disk is free to rotate in the horizontal plane about a frictionless axis perpendicular to the center of the disk. A \(40.0-\mathrm{kg}\) person, standing \(1.25 \mathrm{~m}\) from the axis, begins to run on the disk in a circular path and has a tangential speed of \(2.00 \mathrm{~m} / \mathrm{s}\) relative to the ground. Find the resulting angular speed of the disk (in \(\mathrm{rad} / \mathrm{s}\) ) and describe the direction of the rotation.

A flywheel is a solid disk that rotates about an axis that is perpendicular to the disk at its center. Rotating flywheels provide a means for storing energy in the form of rotational kinetic energy and are being considered as a possible alternative to batteries in electric cars. The gasoline burned in a 300 -mile trip in a typical midsize car produces about \(1.2 \times 10^{9} \mathrm{~J}\) of energy. How fast would a \(13-\mathrm{kg}\) flywheel with a radius of \(0.30 \mathrm{~m}\) have to rotate to store this much energy? Give your answer in rev/min.

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