In: Physics
Lab 1: Measurements and uncertainty estimation
Introduction:
The purpose of this lab is to measure a quantity related to the static friction of glass. Static friction is the force required to start moving an object from rest. You will place a coin on the glass and lift one end until the coin begins to move. Your goal is to measure the angle at which the coin moves and understand what affects the precision and accuracy of your measurements.
1) Pick a coin to use based on your birth month and the list here:
Jan – March |
$0.05 |
Apr – June |
$0.10 |
July – Sept |
$0.25 |
Sept – Dec |
$1.00 |
FOR HEADS
Trial # |
Length |
Height (Cm) |
Angle (in Radians) |
1 |
28.3 Cm |
10 cm |
0.35 |
2 |
28.3 Cm |
9.4 |
0.33 |
3 |
28.3 Cm |
9.4 |
0.33 |
4 |
28.3 Cm |
9 |
0.31 |
5 |
28.3 Cm |
9.2 |
0.32 |
8) Compute the average angle and average uncertainty. Compute the difference between the measured angles in each trial and the averaged angle. Quantitatively how do the differences compare to the average uncertainty?
9) Based on 8) would you say that the average uncertainty accounts for the different trial measurements (i.e. are the differences large or small compared to the uncertainty)?
10) Repeat the steps 2-9 for the coin “tails up”.
FOR TAILS
Trial # |
Length |
Height (Cm) |
Angle (in Radians) |
1 |
28.3 Cm |
9.5 cm |
0.33 |
2 |
28.3 Cm |
9.7 |
0.34 |
3 |
28.3 Cm |
10.4 |
0.37 |
4 |
28.3 Cm |
9.7 |
0.34 |
5 |
28.3 Cm |
9.6 |
0.34 |
Consider the following arrangement where a book is used and a fair coin of your choice is placed over it and then book cover is tilted such that it makes an angle θ with the hotizontal;
Now, from this FBD, for static case
Length (L) in cm | Height(H) in cm | θ in rad | θ - <θ> | (θ - <θ>)² |
28.3 | 10 | 0.3611 | 0.0226 | 0.00051076 |
28.3 | 9.4 | 0.3385 | 0.0000 | 0 |
28.3 | 9.4 | 0.3385 | 0.0000 | 0 |
28.3 | 9.0 | 0.3236 | 0.0149 | 0.0002223 |
28.3 | 9.2 | 0.3310 | 0.0075 | 0.0000570 |
Average of θ, <θ> = 0.33855 | Average of uncertainty = 0.009012 |
In this table we have used ;
and
From table it is evident that the differences are very much small between the average measured values, hence the value is close to 0.33855. Similar procedure can be followed for the second case.