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LAB 8 2022 Group 4

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KING MONGKUT’S INSTITUTE OF TECHNOLOGY LATKRABANG
SCHOOL OF ENGINEERING GROUP OF
KMIDS
01006702/01006724– PHYSICS -I LABORATORY
LINEAR MOMENTUM & COLLISIONS
INSTRUCTED BY: SUPUN DISSANAYAKA, KASUN HETTIHEWA
NAME: WANTANA, NAPHAT,
SINGHANART, PAWARIT, KRITTAPAS
ID NUMBER: 1707070, 1707023,
1707054, 170704, 1707015
GROUP NO: KMIDS, 2
DATE OF SES.: 9/11/2022
DATE OF SUB.: 03/12/2022
Purpose:
1)
2)
3)
4)
5)
To understand the concepts of momentum and how to apply it.
Understand how to classify and differentiate different collisions.
Understand the concept of impulse and how to apply it.
Know the relationship between kinetic energy and momentum.
Understand how momentum is conserve and apply it to the real-world.
Theory:
Linear Momentum
• Momentum is always conserved.
• The momentum formula is defined as
π‘€π‘Žπ‘ π‘  ∗ π‘£β…‡π‘™π‘œπ‘π‘–π‘‘π‘¦
Or
𝑝 =π‘š∗𝑣
• The unit of momentum is equal to kilogram meter per second
π‘˜π‘” ∗ π‘š
𝑠
Impulse and Average Force
• The amount of time requires to the change the momentum
𝐼 = π‘šπ‘“ 𝑣𝑓 − π‘šπ‘– 𝑣𝑖
• Average force is defined by the force multiply by time equal to the change in
momentum
𝐹⃗ =
π‘šπ‘“ 𝑣𝑓 − π‘šπ‘– 𝑣𝑖
𝐼
=
π›₯𝑑
π›₯𝑑
Collisions
• In all types of collisions momentum is conserved.
𝑝1𝑖 + 𝑝2𝑖 = 𝑝1𝑓 + 𝑝2𝑓
Or
• If we express, it in respect of masses and velocities.
π‘š1𝑖 𝑣1𝑖 + π‘š2𝑖 𝑣2𝑖 = π‘š1𝑓 𝑣1𝑓 + π‘š2𝑓 𝑣2𝑓
Elastic collision
• The total kinetic energy and momentum are conserved.
1
1
1
1
2
2
2
2
π‘š1 𝑣1𝑖
+ π‘š2 𝑣2𝑖
= π‘š1 𝑣1𝑓
+ π‘š2 𝑣2𝑓
2
2
2
2
Perfectly inelastic collision
• The momentum is conserved however the total energy is not conserved.
Pre-Lab Exercise:
EX: 1)
What will happen to the system’s momentum and what is it? Find the u
velocity.
-
The momentum will be conserved since momentum is conserved in all collisions. The
type of collision is an explosion.
Since in all collision
π‘šπ‘– 𝑣𝑖 = π‘šπ‘“ 𝑣𝑓
We can infer that
π‘šπ‘– 𝑣π‘₯𝑖 = π‘šπ‘“ 𝑣π‘₯𝑓 π‘Žπ‘›π‘‘ π‘šπ‘– 𝑣𝑦𝑖 = π‘šπ‘“ 𝑣𝑦𝑓
Now, the formula for our horizontal momentum is:
π‘šπ‘— 𝑣π‘₯𝑖 = π‘š3.8 (𝑣3.8π‘₯ ) + π‘š4.2 (𝑣4.2π‘₯ ) + π‘š2 (𝑒 π‘π‘œπ‘  πœƒ)
Which mean our 𝑒 π‘π‘œπ‘  πœƒ is equal:
𝑒 π‘π‘œπ‘  πœƒ =
π‘šπ‘— 𝑣π‘₯𝑖 − π‘š3.8 𝑣3.8π‘₯ − π‘š4.2 𝑣4.2π‘₯
π‘š2
Thus,
𝑒 π‘π‘œπ‘  πœƒ =
10(0) − 3.8 ∗ (−21π‘π‘œπ‘ 20) − 4.2 ∗ (12π‘π‘œπ‘ 30)
2
𝑒 π‘π‘œπ‘  πœƒ = 15.669 π‘š/𝑠
Now, the formula for our vertical momentum is:
π‘šπ‘— 𝑣𝑦𝑖 = π‘š3.8 (𝑣3.8𝑦 ) + π‘š4.2 (𝑣4.2𝑦 ) + π‘š2 (𝑒 𝑠𝑖𝑛 πœƒ)
Which mean our 𝑒 𝑠𝑖𝑛 πœƒ is equal:
𝑒 𝑠𝑖𝑛 πœƒ =
π‘šπ‘— 𝑣𝑦𝑖 − π‘š3.8 𝑣3.8𝑦 − π‘š4.2 𝑣4.2𝑦
π‘š2
Therefore,
𝑒 𝑠𝑖𝑛 πœƒ =
10(0) − 3.8 ∗ (21𝑠𝑖𝑛20) + 4.2 ∗ (12𝑠𝑖𝑛30)
2
𝑒 𝑠𝑖𝑛 πœƒ = −1.0466 π‘š/𝑠
To find 𝒖 we must find our theta first by find π‘‘π‘Žπ‘› πœƒ
π‘ˆ 𝑠𝑖𝑛 πœƒ
1.0466
=−
= π‘‘π‘Žπ‘› πœƒ
π‘ˆ π‘π‘œπ‘  πœƒ
15.669
πœƒ = π‘‘π‘Žπ‘›−1 (−
1.0466
)
15.669
πœƒ = −3.821°
15.669
= 15.703
π‘π‘œπ‘  πœƒ
π‘ˆ=
π‘ˆ = 15.703 π‘š/𝑠
EX: 2)
What was the original speed of the bullet?
From the law of conservation of momentum
π‘šπ‘– 𝑣𝑖 = π‘šπ‘“ 𝑣𝑓
The momentum of our system is defined as:
π‘šπ‘π‘’π‘™π‘™π‘’π‘‘ 𝑣𝑖 = (π‘šπ‘π‘’π‘™π‘™π‘’π‘‘ + π‘šπ‘€π‘œπ‘œπ‘‘ )𝑣𝑓
The formula for our initial velocity is:
𝑣𝑖 =
(π‘šπ‘π‘’π‘™π‘™π‘’π‘‘ + π‘šπ‘€π‘œπ‘œπ‘‘ )𝑣𝑓
π‘šπ‘π‘’π‘™π‘™π‘’π‘‘
Thus
𝑣𝑖 =
(0.010 + 5)0.600
0.010
𝑣𝑖 = 300.6 π‘š/𝑠
Experiment:
Elastic Collisions (Fixed Object)
Procedure:
1.
2.
3.
4.
5.
6.
Set up two carts on the track.
Set up end stop with holders of magnets on the end of the track.
Starting each trial with the reference poles to track the result.
Move the two carts to each of the end sides on the track.
Push one of the carts to other end side of the track.
Record the results of collision by video camera.
Observation:
The moving cart hit the fixed cart and gradually moving back with a low speed.
Calculations:
π‘š = 527.5 𝑔 π‘œπ‘Ÿ 0.53 π‘˜π‘”
Calculating the initial and final velocity:
Trial
1
2
3
Avg.
d1 (cm)
72.6
72.6
72.6
t1 (s)
2.46
2.64
3.45
Vi (cm/s)
29.5
27.5
21.04
26.01
0.26 m/s
d2 (cm)
33
43
22.8
𝑣𝑖 = 0.26 m/s
𝑣𝑓 = 0.13 m/s
Momentum:
Equation used:
𝑝𝑖 = 𝑝𝑓
π‘šπ‘£1 = π‘šπ‘£2
Therefore
0.53 × 0.26 = 0.53 × 0.13
0.14
π‘˜π‘” × π‘š
π‘˜π‘” × π‘š
= 0.069
𝑠
𝑠
t2 (s)
1.83
3.5
2.66
Vf (cm/s)
18.03
12.29
8.57
12.96
0.13 m/s
Kinetic Energy:
Equations used:
𝐾𝐸𝑖 = 𝐾𝐸𝑓
1
1
π‘šπ‘£12 = π‘šπ‘£22
2
2
Therefore
1
1
× 0.53 × (0.26)2 = × 0.53 × (0.13)2
2
2
0.018 𝐽 = 0.0045 𝐽
Results:
Momentum:
0.14
π‘˜π‘” × π‘š
π‘˜π‘” × π‘š
= 0.069
𝑠
𝑠
Momentum is not conserved.
Kinetic Energy:
0.018 𝐽 = 0.0045 𝐽
Kinetic Energy is not conserved
Conclusion:
According to the theory, momentum is always conserved as well as kinetic energy
for elastic collision. However, the results above show that this is not true. This
might be because in the real world there are factors like friction, human error,
energy transfer, impulse, etc. These factors might cause the result to be inaccurate.
Elastic Collisions (Moving Object)
Procedure:
1) Set up two carts on the track.
2) Set up the magnets on the cart so that both have the same pole facing each
other.
3) Starting each trial with the reference poles to track the result.
4) Push one of the cart towards the other to make them collide.
5) Record the results of collision by video camera.
Observation:
Calculations:
π‘š1 = 527.5 𝑔 π‘œπ‘Ÿ 0.53 π‘˜π‘”
π‘š1 = 521 𝑔 π‘œπ‘Ÿ 0.52 π‘˜π‘”
Calculate the initial and final velocity for both carts
Trial
1
2
3
Avg.
d1 (cm)
30
30
30
t1 (s)
1.87
1.35
1.3
v1 (cm/s)
16.04
22.2
28.7
22.31
0.22 m/s
d2 (cm)
19.55
49.3
39.7
t2 (s)
3.31
4.21
3.9
𝑣1𝑖 = 0.22 m/s
𝑣1𝑓 = 0 m/s
𝑣2𝑖 = 0 m/s
𝑣2𝑓 = 0.13 m/s
Momentum:
Equation used:
𝑝𝑖 = 𝑝𝑓
π‘š1 𝑣1𝑖 + π‘š2 𝑣2𝑖 = π‘š1 𝑣1𝑓 + π‘š2 𝑣2𝑓
Therefore
0.53 × 0.22 + 0.52 × 0 = 0.53 × 0 + 0.52 × 0.13
0.12 + 0 = 0 + 0.068
v2 (cm/s)
16.24
11.71
10.18
12.71
0.13 m/s
0.12
π‘˜π‘” × π‘š
π‘˜π‘” × π‘š
= 0.068
𝑠
𝑠
Kinetic Energy:
Equation used:
𝐾𝐸𝑖 = 𝐾𝐸𝑓
1
1
1
1
2
2
2
2
π‘š1 𝑣1𝑖
+ π‘š2 𝑣2𝑖
= π‘š1 𝑣1𝑓
+ π‘š2 𝑣2𝑓
2
2
2
2
Therefore
1
1
1
1
× 0.53 × (0.22)2 + × 0.52 × (0)2 = × 0.53 × (0)2 + × 0.52 × (0.13)2
2
2
2
2
0.013 + 0 = 0 + 0.0044
0.013 𝐽 = 0.0044 𝐽
Results:
Momentum:
0.12
π‘˜π‘” × π‘š
π‘˜π‘” × π‘š
= 0.068
𝑠
𝑠
Momentum is not conserved
Kinetic Energy:
0.013 𝐽 = 0.0044 𝐽
Kinetic Energy is not conserved
Conclusion:
According to the theory, momentum is always conserved as well as kinetic
energy for elastic collision. However, the results above show that this is not true.
This might be because in the real world there are factors like friction, human error,
energy transfer, impulse, etc. These factors might cause the result to be inaccurate.
Inelastic Collisions (Moving Object)
Procedure:
1) Set up two carts and place them on the track.
2) Set up a reference pole
3) Set up the magnets on the cart, so that they have opposite pole so that
they could attract when they collide.
4) Push one cart towards the other so that they could collide
5) Use a recording device to record the collision.
Observation:
When two carts hit each other. It attract and continues moving forward at a
lower speed in the same direction.
Calculations:
π‘š1 = 527.5 𝑔 π‘œπ‘Ÿ 0.53 π‘˜π‘”
π‘š2 = 521 𝑔 π‘œπ‘Ÿ 0.52π‘˜π‘”
π‘š3 = 0.53 + 0.52 = 1.05 π‘˜π‘”
Calculate the initial and final velocity of the carts
Trial
1
2
3
Avg.
d1 (cm)
30
30
30
t1 (s)
1.2
1
1.53
v1 (cm/s) d2 (cm)
25
39.9
30
39.5
19.6
19.55
24.87
0.28 m/s
𝑣1𝑖 = 0.28 m/s
𝑣2𝑖 = 0 m/s
𝑣3𝑓 = 0.0079 m/s
Momentum:
Equation used:
𝑝𝑖 = 𝑝𝑓
t2 (s)
4.25
4.8
3.2
v2 (cm/s)
9.4
8.2
6.1
7.9
0.079 m/s
π‘š1 𝑣1𝑖 + π‘š2 𝑣2𝑖 = π‘š3 𝑣3𝑓
Therefore
0.53 × 0.28 + 0.52 × 0 = 1.05 × 0.0079
0.15 + 0 = 0.0083
0.15
π‘˜π‘” × π‘š
π‘˜π‘” × π‘š
= 0.0083
𝑠
𝑠
Kinetic Energy:
Equation used:
1
1
2
2
π‘š1 𝑣1𝑖
+ π‘š2 𝑣2𝑖
2
2
1
2
𝐾𝐸𝑓 = π‘š3 𝑣3𝑓
2
𝐾𝐸𝑖 =
Therefore
𝐾𝐸𝑖 =
1
1
× 0.53 × (0.28)2 + × 0.52 × (0)2
2
2
𝐾𝐸𝑖 = 0.021 𝐽
𝐾𝐸𝑓 =
1
× 1.05 × (0.0079)2
2
𝐾𝐸𝑓 = 0.000033 𝐽
π‘²π‘¬π’Š ≠ 𝑲𝑬𝒇
Results:
Momentum:
0.15
π‘˜π‘” × π‘š
π‘˜π‘” × π‘š
= 0.0083
𝑠
𝑠
Momentum is not conserved
Kinetic Energy:
𝐾𝐸𝑖 = 0.021 𝐽
𝐾𝐸𝑓 = 0.000033
𝐾𝐸𝑖 ≠ 𝐾𝐸𝑓
Kinetic Energy is not conserved
Conclusion:
According to the theory, momentum will always be conserved, but kinetic
energy is not with inelastic collisions. In this experiment, the results show that both
momentum and kinetic energy are not conserved. This shows that kinetic energy is
not conserved with inelastic collisions. Kinetic energy is either converted or
transferred into other types of energy, thus decreasing. However, momentum is not
conserved in this experiment. This might be because of factors like friction,
impulse, and human error.
Discussion:
There might be many factors that affect the experiment. One of the factors is
friction. In the real-world scenarios, there will always be friction that will occur
when there is movement. Thus, we cannot really neglect the fact that friction will
always occur in our experiment. The other factor is the use of initial velocity to
calculate the momentum. However, during the experiment we couldn't find the
initial velocity, so we decided to use the average velocity instead, so the
calculations might not be accurate. Another factor might be energy, the possibility
of conserving all the energy might be difficult because there will always be energy
conversion or transfer of energy, whether it is heat, sound, etc. Finally, there might
be human errors while conducting the experiment that might impact the results.
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