A wind turbine is initially spinning at a constant angular speed. As the wind's strength gradually increases, the turbine experiences a constant angular acceleration 0.107 rad/s². After making 2870 revolutions, its angular speed is 130 rad/s. (a) What is the initial angular velocity of the turbine? (b) How much time elapses while the turbine is speeding up? (a) Number i 129.848 Units rad/s (b) Number i 1.327 Units S

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### Wind Turbine Angular Motion Problem

#### Problem Statement
A wind turbine is initially spinning at a constant angular speed. As the wind's strength gradually increases, the turbine experiences a constant angular acceleration of 0.107 rad/s². After making 2870 revolutions, its angular speed is 130 rad/s.

1. **(a)** What is the initial angular velocity of the turbine?
2. **(b)** How much time elapses while the turbine is speeding up?

#### Answers
1. **(a) Initial Angular Velocity**
   - **Number:** 129.848
   - **Units:** rad/s

2. **(b) Time Elapsed**
   - **Number:** 1.327
   - **Units:** s

This problem explores the concepts of angular motion, including initial angular velocity and the time required for the turbine to reach a given angular speed under constant angular acceleration. The primary formulae used for solving these types of problems are derived from rotational kinematics.
Transcribed Image Text:### Wind Turbine Angular Motion Problem #### Problem Statement A wind turbine is initially spinning at a constant angular speed. As the wind's strength gradually increases, the turbine experiences a constant angular acceleration of 0.107 rad/s². After making 2870 revolutions, its angular speed is 130 rad/s. 1. **(a)** What is the initial angular velocity of the turbine? 2. **(b)** How much time elapses while the turbine is speeding up? #### Answers 1. **(a) Initial Angular Velocity** - **Number:** 129.848 - **Units:** rad/s 2. **(b) Time Elapsed** - **Number:** 1.327 - **Units:** s This problem explores the concepts of angular motion, including initial angular velocity and the time required for the turbine to reach a given angular speed under constant angular acceleration. The primary formulae used for solving these types of problems are derived from rotational kinematics.
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