The radius of the wheel is r=3 m. The tangential acceleration of the point on the edge of the wheel, as whown, is a=2t (m/s2). At t=0, the initial angular position θ0=0 and initial velocity V0=0. After the time of t=6s, determine (2) the of magnitude of the angular velocity, ω=___________ rad/s
The radius of the wheel is r=3 m. The tangential acceleration of the point on the edge of the wheel, as whown, is a=2t (m/s2). At t=0, the initial angular position θ0=0 and initial velocity V0=0. After the time of t=6s, determine (2) the of magnitude of the angular velocity, ω=___________ rad/s
Elements Of Electromagnetics
7th Edition
ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
ChapterMA: Math Assessment
Section: Chapter Questions
Problem 1.1MA
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The radius of the wheel is r=3 m. The tangential acceleration of the point on the edge of the wheel, as whown, is a=2t (m/s2). At t=0, the initial angular position θ0=0 and initial velocity V0=0. After the time of t=6s, determine
(2) the of magnitude of the angular velocity, ω=___________ rad/s
![### Problem Statement
The radius of the wheel is \( r = 3 \) m. The tangential acceleration of the point on the edge of the wheel, as shown, is \( a = 2t \) (m/s^2). At \( t = 0 \), the initial angular position \( \theta_0 = 0 \) and initial velocity \( V_0 = 0 \). After the time of \( t = 6 \) s, determine:
1. The magnitude of the angular velocity, \( \omega = \) __________ rad/s.
### Diagram Explanation
The diagram is a circular representation of the wheel indicating its radius \( r \). There is a vector shown at the edge of the wheel representing the tangential acceleration \( a_T \). The wheel is depicted as a circle with the radius marked, indicating the tangential acceleration acting at the edge.
### Solution Approach
To find the magnitude of the angular velocity \( \omega \) after \( t = 6 \) seconds, we need to integrate the given tangential acceleration to find the angular velocity.
Given:
- Radius \( r = 3 \) m
- Tangential acceleration \( a_T = 2t \) (m/s^2)
- Initial angular position \( \theta_0 = 0 \)
- Initial velocity \( V_0 = 0 \)
We can use the relationship between tangential acceleration \( a_T \) and angular acceleration \( \alpha \):
\[ a_T = r \alpha \]
Since \( a_T = 2t \):
\[ 2t = 3 \alpha \]
\[ \alpha = \frac{2t}{3} \]
Now, integrate the angular acceleration \( \alpha \) to get the angular velocity \( \omega \):
\[ \omega = \int \alpha \, dt = \int \frac{2t}{3} \, dt \]
\[ \omega = \frac{2}{3} \int t \, dt \]
\[ \omega = \frac{2}{3} \left( \frac{t^2}{2} \right) + C \]
\[ \omega = \frac{t^2}{3} + C \]
Using the initial condition \( \omega (0) = 0 \):
\[ 0 = \frac{0^2}{3} + C \]
\[ C = 0 \](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F0daff6b4-7b3b-4798-aa81-781ef422795b%2F98244b65-e22a-4f93-b000-3eca8e986006%2Ft2eb4e4_processed.png&w=3840&q=75)
Transcribed Image Text:### Problem Statement
The radius of the wheel is \( r = 3 \) m. The tangential acceleration of the point on the edge of the wheel, as shown, is \( a = 2t \) (m/s^2). At \( t = 0 \), the initial angular position \( \theta_0 = 0 \) and initial velocity \( V_0 = 0 \). After the time of \( t = 6 \) s, determine:
1. The magnitude of the angular velocity, \( \omega = \) __________ rad/s.
### Diagram Explanation
The diagram is a circular representation of the wheel indicating its radius \( r \). There is a vector shown at the edge of the wheel representing the tangential acceleration \( a_T \). The wheel is depicted as a circle with the radius marked, indicating the tangential acceleration acting at the edge.
### Solution Approach
To find the magnitude of the angular velocity \( \omega \) after \( t = 6 \) seconds, we need to integrate the given tangential acceleration to find the angular velocity.
Given:
- Radius \( r = 3 \) m
- Tangential acceleration \( a_T = 2t \) (m/s^2)
- Initial angular position \( \theta_0 = 0 \)
- Initial velocity \( V_0 = 0 \)
We can use the relationship between tangential acceleration \( a_T \) and angular acceleration \( \alpha \):
\[ a_T = r \alpha \]
Since \( a_T = 2t \):
\[ 2t = 3 \alpha \]
\[ \alpha = \frac{2t}{3} \]
Now, integrate the angular acceleration \( \alpha \) to get the angular velocity \( \omega \):
\[ \omega = \int \alpha \, dt = \int \frac{2t}{3} \, dt \]
\[ \omega = \frac{2}{3} \int t \, dt \]
\[ \omega = \frac{2}{3} \left( \frac{t^2}{2} \right) + C \]
\[ \omega = \frac{t^2}{3} + C \]
Using the initial condition \( \omega (0) = 0 \):
\[ 0 = \frac{0^2}{3} + C \]
\[ C = 0 \
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