A ball moves with an initial velocity vo, as shown below. It is then struck by a tennis racket. After leaving the racket. the ball moves with velocity v. How would the vector that represents the direction of the average force that the racket exerts on the ball look like?

Glencoe Physics: Principles and Problems, Student Edition
1st Edition
ISBN:9780078807213
Author:Paul W. Zitzewitz
Publisher:Paul W. Zitzewitz
Chapter6: Motion In Two Dimensions
Section: Chapter Questions
Problem 90A
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**Diagram Explanation:**

The image depicts a physics diagram illustrating motion with velocity vectors. The diagram features two circles, which likely represent objects or points in motion.

1. The first circle (top left) has an arrow pointing rightwards labeled as **V**. This arrow extending from the center of the circle represents the velocity vector **V** at a certain point in time.
2. The second circle (bottom left) is connected to the first circle by a dashed line, forming an angle between the dashed line and the arrow labeled **V**.
3. From the center of the lower circle, another arrow extends downwards labeled as **V0**. This arrow also represents a velocity vector at the initial point.

**Detailed Explanation:**

- **Circles**: Represent two states or positions of an object or a particle at different times.
- **Vector V**: Indicates the velocity of the object at the position of the upper circle.
- **Vector V0**: Indicates the initial velocity of the object at the position of the lower circle.
- **Dashed Lines**: Likely represent the path or trajectory of the motion between the two points over time.

This diagram is likely used in an educational context to depict concepts of initial and final velocities and their directions, helping students understand the components of motion in a visual manner.
Transcribed Image Text:**Diagram Explanation:** The image depicts a physics diagram illustrating motion with velocity vectors. The diagram features two circles, which likely represent objects or points in motion. 1. The first circle (top left) has an arrow pointing rightwards labeled as **V**. This arrow extending from the center of the circle represents the velocity vector **V** at a certain point in time. 2. The second circle (bottom left) is connected to the first circle by a dashed line, forming an angle between the dashed line and the arrow labeled **V**. 3. From the center of the lower circle, another arrow extends downwards labeled as **V0**. This arrow also represents a velocity vector at the initial point. **Detailed Explanation:** - **Circles**: Represent two states or positions of an object or a particle at different times. - **Vector V**: Indicates the velocity of the object at the position of the upper circle. - **Vector V0**: Indicates the initial velocity of the object at the position of the lower circle. - **Dashed Lines**: Likely represent the path or trajectory of the motion between the two points over time. This diagram is likely used in an educational context to depict concepts of initial and final velocities and their directions, helping students understand the components of motion in a visual manner.
**Educational Content: Dynamics of a Ball Hit by a Tennis Racket**

In this lesson, we will explore the principles of motion in the context of a ball being struck by a tennis racket. 

### Physics of Motion

A ball initially moves with a velocity represented by \(\vec{v_0}\). After being struck by a tennis racket, it leaves with a new velocity, indicated as \(\vec{v}\). The significant change in motion raises the following question:

**Question:** How does the vector that represents the direction of the average force exerted by the racket on the ball appear?

### Explanation

1. **Initial Velocity (\(\vec{v_0}\)):**
   - The ball initiates its motion with a certain velocity in a particular direction. This is denoted by the vector \(\vec{v_0}\).

2. **Impact with the Racket:**
   - The tennis racket exerts a force on the ball, altering its velocity. The direction and magnitude of the force determine the new velocity of the ball.

3. **Final Velocity (\(\vec{v}\)):**
   - After impact, the ball moves away with a new velocity, represented by the vector \(\vec{v}\).

### Force Vector

The force applied by the racket changes the ball’s velocity. This is a direct result of Newton's Second Law of Motion:
\[ \vec{F} = \frac{\Delta \vec{p}}{\Delta t} \]
where \(\vec{F}\) is the average force, \(\Delta \vec{p}\) is the change in momentum, and \(\Delta t\) is the time over which the force acts.

- **Change in Momentum (\(\Delta \vec{p}\)):**
  \[ \Delta \vec{p} = m(\vec{v} - \vec{v_0}) \]
  where \(m\) is the mass of the ball.

- **Direction of Force:**
  The vector representing the force will point in the direction of \(\vec{v} - \vec{v_0}\).

### Diagram Explanation

While the diagram is not provided here, it can be understood as follows:
- Draw the initial velocity vector \(\vec{v_0}\) from the origin.
- Draw the final velocity vector \(\vec{v}\) from the same point.
- The force vector \(\vec
Transcribed Image Text:**Educational Content: Dynamics of a Ball Hit by a Tennis Racket** In this lesson, we will explore the principles of motion in the context of a ball being struck by a tennis racket. ### Physics of Motion A ball initially moves with a velocity represented by \(\vec{v_0}\). After being struck by a tennis racket, it leaves with a new velocity, indicated as \(\vec{v}\). The significant change in motion raises the following question: **Question:** How does the vector that represents the direction of the average force exerted by the racket on the ball appear? ### Explanation 1. **Initial Velocity (\(\vec{v_0}\)):** - The ball initiates its motion with a certain velocity in a particular direction. This is denoted by the vector \(\vec{v_0}\). 2. **Impact with the Racket:** - The tennis racket exerts a force on the ball, altering its velocity. The direction and magnitude of the force determine the new velocity of the ball. 3. **Final Velocity (\(\vec{v}\)):** - After impact, the ball moves away with a new velocity, represented by the vector \(\vec{v}\). ### Force Vector The force applied by the racket changes the ball’s velocity. This is a direct result of Newton's Second Law of Motion: \[ \vec{F} = \frac{\Delta \vec{p}}{\Delta t} \] where \(\vec{F}\) is the average force, \(\Delta \vec{p}\) is the change in momentum, and \(\Delta t\) is the time over which the force acts. - **Change in Momentum (\(\Delta \vec{p}\)):** \[ \Delta \vec{p} = m(\vec{v} - \vec{v_0}) \] where \(m\) is the mass of the ball. - **Direction of Force:** The vector representing the force will point in the direction of \(\vec{v} - \vec{v_0}\). ### Diagram Explanation While the diagram is not provided here, it can be understood as follows: - Draw the initial velocity vector \(\vec{v_0}\) from the origin. - Draw the final velocity vector \(\vec{v}\) from the same point. - The force vector \(\vec
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