Diving from a high cliff, Cliff begins with a moderate rotational speed of a half rotation per second. Rank the following positions (and their moments of inertia) that cliff can assume during his dive, from the lowest rotational speed he will experience to the highest. + 1. Standing straight up, spinning about a head-to-toe axis: I = 0.3 kg m2 I 2. Bent in half, about an axis through his waist: I = 4 kg m2 + 3. Standing straight upwards, about an axis through his waist: I = 16 kg m2 1 4. Mass tucked inwards into a ball: 1 = 0.8 kg m2 + 5. Arms out, spinning about a head-to-toe axis: I = 1.2 kg m2

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**Title: Understanding Rotational Motion in Cliff Diving**

**Introduction:**
Diving from a high cliff, Cliff begins with a moderate rotational speed of half a rotation per second. Below is a list ranking the positions he can assume during his dive, organized by their moments of inertia (I) from the lowest rotational speed to the highest.

**Positions:**

1. **Standing Straight Up (Head-to-Toe Axis)**
   - Moment of Inertia: \( I = 0.3 \, \text{kg m}^2 \)

2. **Bent in Half (Axis Through Waist)**
   - Moment of Inertia: \( I = 4 \, \text{kg m}^2 \)

3. **Standing Straight Upwards (Axis Through Waist)**
   - Moment of Inertia: \( I = 16 \, \text{kg m}^2 \)

4. **Mass Tucked Inwards (Ball Position)**
   - Moment of Inertia: \( I = 0.8 \, \text{kg m}^2 \)

5. **Arms Out (Head-to-Toe Axis)**
   - Moment of Inertia: \( I = 1.2 \, \text{kg m}^2 \)

**Explanation:**
The moment of inertia reflects how mass is distributed in relation to the axis of rotation, affecting the diver's rotational speed. A lower moment of inertia allows for faster rotation, whereas a higher one results in slower rotation. Each position changes how Cliff's mass is distributed, demonstrating fundamental principles of rotational dynamics in a practical scenario.
Transcribed Image Text:**Title: Understanding Rotational Motion in Cliff Diving** **Introduction:** Diving from a high cliff, Cliff begins with a moderate rotational speed of half a rotation per second. Below is a list ranking the positions he can assume during his dive, organized by their moments of inertia (I) from the lowest rotational speed to the highest. **Positions:** 1. **Standing Straight Up (Head-to-Toe Axis)** - Moment of Inertia: \( I = 0.3 \, \text{kg m}^2 \) 2. **Bent in Half (Axis Through Waist)** - Moment of Inertia: \( I = 4 \, \text{kg m}^2 \) 3. **Standing Straight Upwards (Axis Through Waist)** - Moment of Inertia: \( I = 16 \, \text{kg m}^2 \) 4. **Mass Tucked Inwards (Ball Position)** - Moment of Inertia: \( I = 0.8 \, \text{kg m}^2 \) 5. **Arms Out (Head-to-Toe Axis)** - Moment of Inertia: \( I = 1.2 \, \text{kg m}^2 \) **Explanation:** The moment of inertia reflects how mass is distributed in relation to the axis of rotation, affecting the diver's rotational speed. A lower moment of inertia allows for faster rotation, whereas a higher one results in slower rotation. Each position changes how Cliff's mass is distributed, demonstrating fundamental principles of rotational dynamics in a practical scenario.
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