Lab2 Physics, Balgabayeva S
.docx
Lab No.2: Study of kinematics and dynamics on the Atwood’s machine
Balgabayeva Sara
IS-126
IT department, International IT university, Dzhandosov str. 8a, 050040, Almaty
Abstract
We used the Atwood’s machine to study uniformly and uniformly accelerated motion of the loads. The Newton’s second law was proved in the third task of the experiment. I calculated the uncertainties using the Student’s method.
Introduction
Newton’s second law (Fnet = ma) can be experimentally tested with an
apparatus known as an “Atwood’s Machine”. The Atwood’s machine was
constructed by R.G. Atwood in 1784. He used this machine to verify the
mechanical laws of motion with constant acceleration. Atwood’s machine consists of vertical stand with scale ruler. The three supporting arms are fixed on this scale ruler (the upper supporting arm with constant fixation is not shown in Fig. 1). On the stand is set up electromagnet and light pulley, which is able to rotate with insignificant friction. Over the pulley is thrown over the light string with the same mass m. Electromagnet holds the pulley with loads in the rest. Middle supporting arm is furnished by ring for taking off the overload m1. At the moment when the load m moves over the ring, the timer is switch on. The timer measures time t of uniformly motion of loads on the path h. Measuring the distance, which was passed by the load with uniformly accelerated S motion and uniformly h motion, respectively, also the time t, it is possible to prove the main laws of kinematics and dynamics for translational motion and to calculate the free fall acceleration.
Data, results and uncertainties
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Study of uniformly motion
I set up the height of the uniformly motion of the load h=21 cm. I started the experiment and write down the readings of height and time in the table 1. I have repeated this experiment 5 times with changed height. I calculate the magnitude of the velocity by v=h/t. The results are given in the third column
of the table 1.
Table №1
№ |
h, m |
t, sec |
V, m/sec
|
ΔVi |
ΔVi2 |
1 |
0,21 |
0,292 |
0,7191 |
0,0007 |
4,9*10^-7 0,00000049 |
2 |
0,19 |
0,264 |
0,7197 |
0,0013 |
16,9*10^-7 0,00000169 |
3 |
0,17 |
0,236 |
0,7203 |
0,0019 |
36,1*10^-7 0,00000361 |
4 |
0,15 |
0,209 |
0,7177 |
-0,0007 |
4,9*10^-7 0,00000049 |
5 |
0,13 |
0,181 |
0,7182 |
-0,0002 |
0,4*10^-7 0,00000004 |
6 |
0,11 |
0,153 |
0,7189 |
0,0005 |
2,5*10^-7 0,00000025 |
7 |
0,09 |
0,125 |
0,72 |
0,0016 |
25.6*10^-7 0,00000256 |
8 |
0,07 |
0,097 |
0,7216 |
0,0032 |
102,4*10^-7 0,00001024 |
9 |
0,05 |
0,070 |
0,7143 |
-0,0041 |
168,1*10^-7 0,00001681 |
10 |
0,03 |
0,042 |
0,7143 |
-0,0041 |
168,1*10^-7 0,00001681 |
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|
|
|
|
|
Vm =0,7184
I have calculated the arithmetic mean value V of all results and obtained the following results.
= = =0,7184
I calculated the deviation of individual measurements Vi and their
squares i2, to make them in the table №1, 5 and 6 columns.
Δ Vi = Vi – V0 , where i=1, 2, ..., n;
I calculated the mean square error of the individual measurement:
Then the mean square error of the arithmetic mean
Absolute deviation is
<v>
Where tp is the Student’s coefficient; tp =2 for n=2. I suppose that the error probability α=0.95
Relative error is
Final result for the velocity is
) m/sec
-
Study of uniformly accelerated motion
By changing the positions of upper support arm from 25 until 35, I set up distance of uniformly motion S and uniformly accelerated motion h of load. I wrote down the reading in the table №2.
I measured time of uniformly motion of load t for different distances between support arms h.
Table №2
№ |
h, m |
S, m |
t, sec |
a, m/sec2 |
Δai |
Δai2 |
1 |
0,22 |
0,21 |
0,359 |
0,8946 |
0,00173 |
29,93*10^-8 |
2 |
0,23 |
0,20 |
0,385 |
0,8921 |
-0,00077 |
59,29*10^-8 |
3 |
0,24 |
0,19 |
0,412 |
0,8930 |
0,00013 |
1,69*10^-8 |
4 |
0,25 |
0,18 |
0,441 |
0,8928 |
-0,00007 |
0,49*10^-8 |
5 |
0,26 |
0,17 |
0,472 |
0,8929 |
0,00003 |
0,09*10^-8 |
6 |
0,27 |
0,16 |
0,505 |
0,8933 |
0,00043 |
18,49*10^-8 |
7 |
0,28 |
0,15 |
0,541 |
0,8929 |
0,00003 |
0,09*10^-8 |
8 |
0,29 |
0,14 |
0,580 |
0,8928 |
-0,00007 |
9,49*10^-8 |
9 |
0,3 |
0,13 |
0,623 |
0,8920 |
-0,00087 |
75,69*10^-8 |
10 |
0,31 |
0,12 |
0,670 |
0,8923 |
-0,00057 |
32,49*10^-8 |
|
|
|
|
am=0,89287 |
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|
Then I calculated the acceleration a for different values of S and h.
And wrote down the reading in the table №2.
I have calculated the arithmetic mean value am of all results and obtained the following results.
= =
I calculated the deviation of individual measurements ∆ai and their
squares ∆ai2, to make them in the table №2, 6 and 7 columns.
Δ ai = ai – a0 , where i=1, 2, ..., n;
I have calculated the uncertainty of the experiment and obtained the following results.
Standard deviation is
Absolute deviation is
<a>
Where tp is the Student’s coefficient; tp =2 for n=2. I suppose that the error probability α=0.95
Relative error is
Final result for the acceleration is
) m/sec2
3. Verification of Newton’s second law
I set up distance h of uniformly accelerated motion of load.
By changing the m1 from 30 until 40 and S from 50 to 30, measure time t of uniformly motion of load at different magnitudes of h.
I wrote down the readings in Tab.3. Calculated the acceleration a.
Then I checked the relation a1 / m1 = a2 / m2 = const, where m1, m2 are masses of overloads.
m1, kg |
S, m |
t, sec |
a, m/sec2 |
a/m |
Δa/m |
Δ(a/m)2 |
0,01 |
0,5 |
1,596 |
0,1963 |
19,63 |
0,004 |
16*10^1-6 |
0,014 |
0,49 |
1,336 |
0,2745 |
19,6171 |
-0,0089 |
79,21*10^-6 |
0,018 |
0,48 |
1,166 |
0,3531 |
19,6267 |
0,0007 |
0,49*10^-6 |
0,022 |
0,47 |
1,043 |
0,4320 |
19,6363 |
0,0103 |
106,09*10^-6 |
0,026 |
0,46 |
0,950 |
0,5096 |
19,6 |
-0,026 |
676*10^-6 |
0,03 |
0,45 |
0,874 |
0,5891 |
19,6367 |
0,0107 |
111,49*10^-6 |
0,034 |
0,44 |
0,812 |
0,6674 |
19,6294 |
0,0034 |
11,56*10^-6 |
0,038 |
0,43 |
0,759 |
0,7464 |
19,6421 |
0,0161 |
259,21*10^-6 |
0,042 |
0,42 |
0,714 |
0,8238 |
19,6142 |
-0,0118 |
139,24*10^-6 |
0,046 |
0,41 |
0,674 |
0,9024 |
19,6173 |
-0,0087, |
75,69*10^-6 |
|
|
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|
a/m avg = 19,6260 |
|
|
I have calculated the arithmetic mean value a/mm of all results and obtained the following results.
= =
I calculated the deviation of individual measurements ∆a/m and their
squares ∆a/m2, to make them in the table №2, 6 and 7 columns.
I have calculated the uncertainty of the experiment and obtained the following results.
Standard deviation is
Absolute deviation is
<a>
Where tp is the Student’s coefficient; tp =2 for n=2. I suppose that the error probability α=0.95
Relative error is