Chapter 26: Problem 30
The angular acceleration \(\alpha\) is the time rate of change of angular velocity \(\omega\) of a rotating object. See Fig. \(26.3 .\) When starting up. the angular acceleration of a helicopter blade is \(\alpha=\sqrt{8 t+1}\) Find the expression for \(\theta\) if \(\omega=0\) and \(\theta=0\) for \(t=0\)
Short Answer
Step by step solution
Understanding the Given Function
Finding Angular Velocity
Finding Angular Displacement
Final Expression for Angular Displacement
Unlock Step-by-Step Solutions & Ace Your Exams!
-
Full Textbook Solutions
Get detailed explanations and key concepts
-
Unlimited Al creation
Al flashcards, explanations, exams and more...
-
Ads-free access
To over 500 millions flashcards
-
Money-back guarantee
We refund you if you fail your exam.
Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!
Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Angular Velocity
Angular velocity can be calculated from the angular acceleration by integrating over time. Since angular acceleration is the rate of change of angular velocity, by adding up these small changes over time (integration), we can find out how fast an object is currently rotating.
In this exercise, we start with a given angular acceleration function, and we want to find the velocity. This involves carrying out an integration process using our angular acceleration function. It tells us:
- The formula for angular velocity in this scenario after integration is: \[ \omega = \frac{1}{12} (8t + 1)^{3/2} - \frac{1}{12} \]
- The constant \( C_1 \) is determined using initial conditions (when \( t = 0 \), \( \omega = 0 \)).
Angular Acceleration
The angular acceleration, denoted by \( \alpha \), represents the derivative of angular velocity (\( \omega \)), or, in simpler terms, how quickly angular velocity changes. In the given function for this problem, the angular acceleration \( \alpha \) is expressed as \( \sqrt{8t + 1} \). This function tells us how angular speed picks up with time.
- To find out how it translates to angular velocity, we integrate this acceleration over time.
- Integration helps us transition from acceleration to the specific velocity at any given time.
Integration Techniques
For functions like our angular acceleration, we might use substitution to simplify the integration. Substitution replaces a difficult part of an expression with something simpler, allowing easier integration.
In this exercise, the substitution \( u = 8t + 1 \) enabled us to convert our complex function into a simpler form which we could integrate more easily.
- We used the substitution to perform integration on \( \alpha \) and \( \omega \).
- Resulting in \( \int \sqrt{u} \, du \), which is easier to solve.
Initial Conditions in Calculus
In this exercise, we were given that at time zero both the angular velocity and angular displacement start from zero - \( \omega = 0 \) and \( \theta = 0 \). This is essential to determine the constants of integration, \( C_1 \) and \( C_2 \), that arise during integration.
- These initial values ensure the solutions are tailored specifically to match the starting conditions.
- Without initial conditions, results would only show generality and not a specific scenario like the one involving the helicopter blade.