The drive propeller of a ship starts from rest and accelerates at 2.85 x 10-3 rad/s² for 2.44 x 10³ s. For the next 1.65 x 10³ s the propeller rotates at a constant angular speed. Then it decelerates at 2.30 x 10-3 rad/s² until it slows (without reversing direction) to an angular speed of 2.66 rad/s. Find the total angular displacement of the propeller. Number i ! Units rad

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### Problem Statement

The drive propeller of a ship starts from rest and accelerates at \(2.85 \times 10^{-3} \, \text{rad/s}^2\) for \(2.44 \times 10^3 \, \text{s}\). For the next \(1.65 \times 10^3 \, \text{s}\) the propeller rotates at a constant angular speed. Then it decelerates at \(2.30 \times 10^{-3} \, \text{rad/s}^2\) until it slows (without reversing direction) to an angular speed of \(2.66 \, \text{rad/s}\). Find the total angular displacement of the propeller.

### Solution

To find the total angular displacement, we need to consider three distinct phases:
1. **Acceleration Phase:** The propeller accelerates from rest.
2. **Constant Speed Phase:** The propeller rotates at a constant angular speed.
3. **Deceleration Phase:** The propeller slows down until it reaches a final angular speed.

Let's analyze each phase in detail.

#### Phase 1: Acceleration from Rest
- Initial angular speed, \( \omega_0 = 0 \, \text{rad/s} \)
- Angular acceleration, \( \alpha = 2.85 \times 10^{-3} \, \text{rad/s}^2 \)
- Time, \( t_1 = 2.44 \times 10^3 \, \text{s} \)

Using the kinematic equation:
\[ \omega_1 = \omega_0 + \alpha t_1 \]
\[ \omega_1 = 0 + (2.85 \times 10^{-3})(2.44 \times 10^3) \]
\[ \omega_1 = 6.954 \, \text{rad/s} \]

Total displacement during this phase:
\[ \theta_1 = \omega_0 t + \frac{1}{2} \alpha t_1^2 \]
\[ \theta_1 = 0 + \frac{1}{2} (2.85 \times 10^{-3})(2.44 \times 10^3)^2 \]
\[ \theta_1 = 8499 \, \text{rad} \]

#### Phase 2: Constant Angular Speed
- Angular speed
Transcribed Image Text:### Problem Statement The drive propeller of a ship starts from rest and accelerates at \(2.85 \times 10^{-3} \, \text{rad/s}^2\) for \(2.44 \times 10^3 \, \text{s}\). For the next \(1.65 \times 10^3 \, \text{s}\) the propeller rotates at a constant angular speed. Then it decelerates at \(2.30 \times 10^{-3} \, \text{rad/s}^2\) until it slows (without reversing direction) to an angular speed of \(2.66 \, \text{rad/s}\). Find the total angular displacement of the propeller. ### Solution To find the total angular displacement, we need to consider three distinct phases: 1. **Acceleration Phase:** The propeller accelerates from rest. 2. **Constant Speed Phase:** The propeller rotates at a constant angular speed. 3. **Deceleration Phase:** The propeller slows down until it reaches a final angular speed. Let's analyze each phase in detail. #### Phase 1: Acceleration from Rest - Initial angular speed, \( \omega_0 = 0 \, \text{rad/s} \) - Angular acceleration, \( \alpha = 2.85 \times 10^{-3} \, \text{rad/s}^2 \) - Time, \( t_1 = 2.44 \times 10^3 \, \text{s} \) Using the kinematic equation: \[ \omega_1 = \omega_0 + \alpha t_1 \] \[ \omega_1 = 0 + (2.85 \times 10^{-3})(2.44 \times 10^3) \] \[ \omega_1 = 6.954 \, \text{rad/s} \] Total displacement during this phase: \[ \theta_1 = \omega_0 t + \frac{1}{2} \alpha t_1^2 \] \[ \theta_1 = 0 + \frac{1}{2} (2.85 \times 10^{-3})(2.44 \times 10^3)^2 \] \[ \theta_1 = 8499 \, \text{rad} \] #### Phase 2: Constant Angular Speed - Angular speed
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