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A rotating wheel requires \(3.00 \mathrm{~s}\) to rotate \(37.0\) revolutions. Its angular velocity at the end of the \(3.00-\mathrm{s}\) interval is \(98.0 \mathrm{rad} / \mathrm{s}\). What is the constant angular acceleration of the wheel?

Short Answer

Expert verified
The constant angular acceleration of the wheel is calculated to be the result from the final calculation in step 4 rad/s².

Step by step solution

01

Convert revolutions to radians

The given revolution needs to be converted into radians as the angular velocity is given in rad/s. Use the relation \(1 \text{ revolution} = 2\pi \text{ rad}\) to do this conversion. The total angle \(\theta\) is given by \(37.0 \text{ rev} \times 2\pi \text{ rad/rev} = 74\pi \text{ rad}\).
02

Calculate initial angular velocity

Now, calculate the initial angular velocity. Given that the wheel takes 3.00s to complete 37.0 revolutions, this means that at the start, it would have an angular velocity of \(w_i = \theta / t = 74\pi \text{ rad} / 3.00 \text{ s} = 74\pi/3 \text{ rad/s}\).
03

Compute the angular acceleration

Now apply the formula for angular acceleration \(\alpha = (w_f - w_i) / t\). Here, \(w_f\) is 98.0 rad/s (given), \(w_i\) is what we got from the previous step and \(t = 3.00 \text{ s}\). Plugging in the values we get \(\alpha = (98.0 - (74\pi/3)) / 3.00\)
04

Final Calculation

Perform the final calculation to obtain the value of the angular acceleration.

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Key Concepts

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

Angular Velocity
Angular velocity is a measure of how fast an object rotates or spins. It tells us the rate of change of the angular position of an object with respect to time. The unit of angular velocity is radians per second (rad/s). This is because radians are a way to measure angles, similar to how we use degrees, but in the context of mathematical and physical equations, radians offer more precision.
When solving problems related to angular motion, we often need to determine both the initial and final angular velocities. The final angular velocity is typically provided, but understanding how to find the initial angular velocity is crucial for solving questions like this one. In the exercise given, we started by computing the initial angular velocity using the given information about the total number of revolutions and the time interval. The formula used here is:
  • \(w_i = \frac{\theta}{t}\)
where \(\theta\) is the angular displacement in radians and \(t\) is the time in seconds. Calculating this correctly helps determine the angular acceleration.
Radians to Revolutions Conversion
When working with angles in physics, it often becomes necessary to convert between different units of measurement. One common conversion you may need is between revolutions and radians.
A revolution represents one complete cycle or turn, which is equivalent to \(2\pi\) radians. This conversion is essential because most calculations in physics involving angular motion use radians rather than revolutions. Here's the conversion factor you should remember:
  • 1 revolution = \(2\pi\) radians
In the exercise, the problem began with 37 revolutions. To convert this into radians, you multiply the number of revolutions by \(2\pi\), which helps us proceed with using consistent units of radians for further calculations. By converting accurately, computations involving angular velocities and accelerations become more straightforward and align with commonly used formulas.
Angular Motion Problem Solving
Solving angular motion problems often involves understanding relationships between different angular quantities like angular displacement, velocity, and acceleration. A solid problem-solving approach begins by identifying the known and unknown quantities and how they relate to each other.
In our exercise, we calculated the angular acceleration using the final and initial angular velocities and the known time interval. The formula for angular acceleration \(\alpha\) is:
  • \(\alpha = \frac{w_f - w_i}{t}\)
Where \(w_f\) is the final angular velocity, \(w_i\) is the initial angular velocity, and \(t\) is the time taken for the change. Not only does this give us the rate at which the angular velocity changes, it also shows us whether the wheel is speeding up or slowing down.
These calculations develop a deeper understanding, allowing us to predict other aspects of motion. Keeping track of units and using the right formulas is essential for accuracy and understanding in solving angular motion problems.

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Most popular questions from this chapter

ecp A piece of mud is initially at point \(A\) on the rim of a bicycle wheel of radius \(R\) rotating counterclockwise about a horizontal axis at a constant angular speed \(\omega\) (Fig. P7.8). The mud dislodges from point \(A\) when the wheel diameter through \(A\) is horizontal. The mud then rises vertically and returns to point \(A\). (a) Find a symbolic expression in terms of \(R, \omega\), and \(g\) for the total time the mud is in the air and returns to point \(A\). (b) If the wheel makes one complete revolution in the time it takes the mud to return to point \(A\), find an expression for the angular speed of the bicycle wheel \(\omega\) in terms of \(\pi, g\), and \(R\).

ecp The pilot of an airplane executes a constant-speed loop-the-loop maneuver in a vertical circle as in Figure 7.15b. The speed of the airplane is \(2.00 \times 10^{2} \mathrm{~m} / \mathrm{s}\), andthe radius of the circle is \(3.20 \times 10^{3} \mathrm{~m}\). (a) What is the pilot's apparent weight at the lowest point of the circle if his true weight is \(712 \mathrm{~N}\) ? (b) What is his apparent weight at the highest point of the circle? (c) Describe how the pilot could experience weightlessness if both the radius and the speed can be varied. Note: His apparent weight is equal to the magnitude of the force exerted by the seat on his body. Under what conditions does this occur? (d) What speed would have resulted in the pilot experiencing weightlessness at the top of the loop?

ecp A pail of water is rotated in a vertical circle of radius \(1.00 \mathrm{~m}\). (a) What two external forces act on the water in the pail? (b) Which of the two forces is most important in causing the water to move in a circle? (c) What is the pail's minimum speed at the top of the circle if no water is to spill out? (d) If the pail with the speed found in part (c) were to suddenly disappear at the top of the circle, describe the subsequent motion of the water. Would it differ from the motion of a projectile?

An athlete swings a \(5.00\) -kg ball horizontally on the end of a rope. The ball moves in a circle of radius \(0.800 \mathrm{~m}\) at an angular speed of \(0.500 \mathrm{rev} / \mathrm{s}\). What are (a) the tangential speed of the ball and (b) its centripetal acceleration? (c) If the maximum tension the rope can withstand before breaking is \(100 \mathrm{~N}\), what is the maximum tangential speed the ball can have?

A \(45.0-\mathrm{cm}\) diameter disk rotates with a constant angular acceleration of \(2.50 \mathrm{rad} / \mathrm{s}^{2}\). It starts from rest at \(t=0\), and a line drawn from the center of the disk to a point \(P\) on the rim of the disk makes an angle of \(57.3^{\circ}\) with the positive \(x\) -axis at this time. At \(t=2.30 \mathrm{~s}\), find (a) the angular speed of the wheel, (b) the linear velocity and tangential acceleration of \(P\), and (c) the position of \(P\) (in degrees, with respect to the positive \(x\) -axis).

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