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
Angular Momentum
The momentum of an object is given by multiplying its mass and velocity. Momentum is a property of any object that moves with mass. The only difference between angular momentum and linear momentum is that angular momentum deals with moving or spinning objects. A moving particle's linear momentum can be thought of as a measure of its linear motion. The force is proportional to the rate of change of linear momentum. Angular momentum is always directly proportional to mass. In rotational motion, the concept of angular momentum is often used. Since it is a conserved quantity—the total angular momentum of a closed system remains constant—it is a significant quantity in physics. To understand the concept of angular momentum first we need to understand a rigid body and its movement, a position vector that is used to specify the position of particles in space. A rigid body possesses motion it may be linear or rotational. Rotational motion plays important role in angular momentum.
Moment of a Force
The idea of moments is an important concept in physics. It arises from the fact that distance often plays an important part in the interaction of, or in determining the impact of forces on bodies. Moments are often described by their order [first, second, or higher order] based on the power to which the distance has to be raised to understand the phenomenon. Of particular note are the second-order moment of mass (Moment of Inertia) and moments of force.
![**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.](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F8af962f0-9f45-405e-8070-77ecf45b3b6d%2Feb59fc49-dbc1-4b67-9de6-189d8111e6d8%2Fd65a3ja_processed.jpeg&w=3840&q=75)
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