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courses:phy101l:3 [2023/10/28 20:58] – [1. Introduction and theory] asadcourses:phy101l:3 [2023/10/31 03:36] (current) – [4. Moment of inertia] asad
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 ====== 3. Moment of inertia of a flywheel ====== ====== 3. Moment of inertia of a flywheel ======
-[[https://colab.research.google.com/drive/1mVmVE4wY7OsXLviG2Ht6e4ddznz1XtHZ?usp=sharing|Google Colab]]+[[https://colab.research.google.com/drive/1mVmVE4wY7OsXLviG2Ht6e4ddznz1XtHZ?usp=sharing|Report sample in Google Colab]]
  
 ===== - Introduction and theory ===== ===== - Introduction and theory =====
Line 14: Line 14:
 $$ h = 2\pi r n_1 $$ $$ h = 2\pi r n_1 $$
 ===== - Method and data ===== ===== - Method and data =====
 +{{:courses:phy101l:flywheel.png?nolink|}}
 +
 +Number of rotations before the mass falls, $n_1=$
 +
 +Radius of the axle, $r=[(a+vb)/2]$ cm; where $a$ is the main scale reading, $b$ is the Vernier scale reading, and $v$ is the Vernier constant.
 +
 +^ Mass [g] ^ $n_2$ ^ $t$ [s] ^
 +| 1000 |  |  |
 +| 1500 |  |  |
 +| 2000 |  |  |
 +| 2500 |  |  |
  
 ===== - Angular velocity ===== ===== - Angular velocity =====
  
 ===== - Moment of inertia ===== ===== - Moment of inertia =====
 +Mean
 +
 +$$ \mu = \frac{1}{N} \sum_{i=0}^{N-1} x_i. $$
 +
 +Standard deviation
 +
 +$$ \sigma = \sqrt{ \frac{1}{N} \sum_{i=0}^{N-1} (x_i-\mu)^2}. $$
 +
 +The final result of an experiment is quoted as
  
 +$$ \text{ value } = \mu \pm \sigma. $$
 ===== - Discussion and conclusion ===== ===== - Discussion and conclusion =====
   - Why does the flywheel come to a stop?   - Why does the flywheel come to a stop?
courses/phy101l/3.1698548299.txt.gz · Last modified: 2023/10/28 20:58 by asad

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