Required information The ability of the human eye to rapidly rotate was studied using contact lenses fitted with accelerometers. While a subject, whose eyeball has radius 1.25 cm, watches a moving object her eyeball rotates through 20.0 in a time interval of 71.3 ms. Assume that the eye starts at rest, rotates with a constant angular acceleration during the first half of the interval, and then the rotation slows with a constant angular acceleration during the second half until it comes to rest. What is the magnitude of the angular acceleration of the eye? 68 6115 radis2

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### Understanding Angular Acceleration of the Eye

#### Required Information

The ability of the human eye to rapidly rotate was studied using contact lenses fitted with accelerometers. While a subject, whose eyeball has a radius of 1.25 cm, watches a moving object, her eyeball rotates through 200° in a time interval of 713 ms.

#### Task

Assume that the eye starts at rest, rotates with a constant angular acceleration during the first half of the interval, and then the rotation slows with a constant angular acceleration during the second half until it comes to rest. What is the magnitude of the angular acceleration of the eye?

#### Calculation

To solve this, consider the given information:

- Eyeball radius: 1.25 cm
- Total rotation: 200°
- Time interval: 713 ms
- The motion is split into two equal halves: acceleration and deceleration.

The angular acceleration (α) can be calculated considering that the eye goes through a uniform acceleration phase for the first half of the time and decelerates uniformly during the second half of the time.

\[
\theta = 200° \quad (\text{Angular displacement})
\]

First, convert the angular displacement to radians:

\[
200° \times \frac{\pi \text{ rad}}{180°} = \frac{200\pi}{180} \approx 3.49 \text{ rad}
\]

The total time given is 713 ms, which is:

\[
713 \text{ ms} = 0.713 \text{ s}
\]

Therefore, half the time interval (for acceleration or deceleration phases) is:

\[
t = \frac{0.713}{2} \text{ s} = 0.3565 \text{ s}
\]

Using the kinematic equation for angular motion:

\[
\theta = \frac{1}{2} \alpha t^2
\]

\(\alpha\) can be isolated and solved:

\[
\alpha = \frac{2 \theta}{t^2}
\]

Substitute \(\theta = 3.49 \text{ rad}\) and \(t = 0.3565 \text{ s}\):

\[
\alpha = \frac{2 \times 3.49 \text{ rad}}{(0.3565 \text{ s})^2}
\]

\[
\alpha =
Transcribed Image Text:### Understanding Angular Acceleration of the Eye #### Required Information The ability of the human eye to rapidly rotate was studied using contact lenses fitted with accelerometers. While a subject, whose eyeball has a radius of 1.25 cm, watches a moving object, her eyeball rotates through 200° in a time interval of 713 ms. #### Task Assume that the eye starts at rest, rotates with a constant angular acceleration during the first half of the interval, and then the rotation slows with a constant angular acceleration during the second half until it comes to rest. What is the magnitude of the angular acceleration of the eye? #### Calculation To solve this, consider the given information: - Eyeball radius: 1.25 cm - Total rotation: 200° - Time interval: 713 ms - The motion is split into two equal halves: acceleration and deceleration. The angular acceleration (α) can be calculated considering that the eye goes through a uniform acceleration phase for the first half of the time and decelerates uniformly during the second half of the time. \[ \theta = 200° \quad (\text{Angular displacement}) \] First, convert the angular displacement to radians: \[ 200° \times \frac{\pi \text{ rad}}{180°} = \frac{200\pi}{180} \approx 3.49 \text{ rad} \] The total time given is 713 ms, which is: \[ 713 \text{ ms} = 0.713 \text{ s} \] Therefore, half the time interval (for acceleration or deceleration phases) is: \[ t = \frac{0.713}{2} \text{ s} = 0.3565 \text{ s} \] Using the kinematic equation for angular motion: \[ \theta = \frac{1}{2} \alpha t^2 \] \(\alpha\) can be isolated and solved: \[ \alpha = \frac{2 \theta}{t^2} \] Substitute \(\theta = 3.49 \text{ rad}\) and \(t = 0.3565 \text{ s}\): \[ \alpha = \frac{2 \times 3.49 \text{ rad}}{(0.3565 \text{ s})^2} \] \[ \alpha =
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