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courses:phy101l:3 [2023/10/28 21:23] – [4. Moment of inertia] 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 =====
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 $$ h = 2\pi r n_1 $$ $$ h = 2\pi r n_1 $$
 ===== - Method and data ===== ===== - Method and data =====
 +{{:courses:phy101l:flywheel.png?nolink|}}
 +
 Number of rotations before the mass falls, $n_1=$ 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. 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^ $n_2$ ^ $t$ ^+^ Mass [g^ $n_2$ ^ $t$ [s] ^
 | 1000 |  |  | | 1000 |  |  |
 | 1500 |  |  | | 1500 |  |  |
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 ===== - Moment of inertia ===== ===== - Moment of inertia =====
- 
 Mean Mean
  
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 $$ \sigma = \sqrt{ \frac{1}{N} \sum_{i=0}^{N-1} (x_i-\mu)^2}. $$ $$ \sigma = \sqrt{ \frac{1}{N} \sum_{i=0}^{N-1} (x_i-\mu)^2}. $$
 +
 +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/3.1698549829.txt.gz · Last modified: by asad

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