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Apr 3, 2024
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Experiment one: Density of Matter
1.
Introduction:
The purpose of this experiment was to study the density of solid objects. The greater the
volume of an object, the smaller the density of an object as they have an inversely proportional
relationship. In this lab, density will be found from found masses and volumes calculated from
measurements taken during the lab.
The mathematical equation used to calculate the volume of cylindrical solids is:
V
=
(1)
Π𝑟
2
?
where V is the volume of the cylinder,
is the ratio of the circumference of a circle to its
Π radius, r is the radius of the cylinder, and l is the length of the cylinder.
The mathematical equation used to calculate the volume of a solid rectangular prism is:
(2)
𝑉 = ??ℎ
where V is the volume of the rectangular prism, l is the length of the rectangular prism, w
is the width of the rectangular prism, and h is the height of the rectangular prism.
The mathematical equation used to calculate the density of an object is:
(3)
ρ =
𝑀
𝑉
where
is the density of an object, M is the mass of the object, and V is the volume of an
ρ object.
2.
Experiment procedures:
The materials and equipment used for this lab included the following: 3 aluminum
cylinders of varied sizes, 3 cardboard rectangular prisms of varied sizes, a balance, and vernier
calipers.
Part 1:
-
Step 1: The balance was turned on and zeroed.
-
Step 2: The mass of a cylinder was measured on the balance.
-
Step 3: The radius and height of the cylinder were measured by putting the cylinder in
between the ends of the vernier calipers.
-
Step 4: The volume was found by multiplying the square of the radius by the height of
the cylinder by pi.
-
Step 5: The density was calculated by dividing the found mass of the cylinder by the
found volume of the cylinder.
-
Step 6: Steps 1-5 were repeated twice for two other cylinders.
Description: The aluminum used were smooth, opaque, silver cylinders.
Part 2:
-
Step 7: Steps 1 and 2 were repeated for the rectangular prism.
-
Step 8: The height, length, and width of the prism were measured by putting the prism in
between the ends of the vernier calipers.
-
Step 9: The volume was found by multiplying the length by the height by the width of the
cylinder.
-
Step 10: Step 5 was repeated.
-
Step 11: Steps 7-10 were repeated twice for the other rectangular prisms.
Description: The rectangular prisms used were made of cardboard. The largest was red, the
second largest was yellow, and the smallest was blue. They were hollow and opaque with a
semi-matte finish.
3.
Results, analysis, and questions:
Table 1: Table one shows the mass, length, radius, volume, and density of the aluminum
cylinders.
Column
1
mass
(grams)
length
(cm)
diameter
(cm)
radius (cm)
volume (m^3
x10^-6)
density
(kg/m^3)
cylinder
1
27.52
7.7
1.1
0.55
7.32
3760
cylinder
2
12.56
3.1
1.1
0.55
2.95
4258
cylinder
3
6.36
7.5
0.6
0.3
2.12
3000
Based on table 1, the graph illustrated the relationship between volume versus mass of the
cylinders.
Graph 1:
From graph 1, the slope of best fit was 0.000254, which demonstrates
(based on equation 3).
1
ρ
Therefore, the density of aluminum is theoretically 3,979 kilograms per meter cubed. The
average experimental density of the aluminum cylinders was found to be approximately 3,673
kilograms per meter cubed, which means that there was around a 7.69% error. The coefficient of
determination was calculated to be 0.981. This demonstrates that the data from this part of the
experiment was relatively accurate. A likely source of error was from measuring the cylinders
with the vernier calipers, where the cylinder may not have gripped tight enough for accuracy.
Table 2: Table 2 shows the mass, height, length, width, volume and density of the blocks.
Mass
(grams)
Height (cm)
Length (cm)
Width (cm)
Volume (m^3 x
10^-3)
Density
(kg/m^3)
Block 1
(red)
134.18
303
74
150
3.36
40
Block 2
(yellow)
86.6
75
152
152
1.73
50
Block 3
(blue)
50.01
146
73
73
0.78
64
Based on table 2, the graph 2 illustrates the relationship between mass and volume of the blocks.
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From graph 2, the slope of best fit was 0.0308, which demonstrates
(based on equation 3).
1
ρ
Therefore, the density of cardboard was 32.47 kilograms per meter cubed. The average
experimental density was 51.3 kilograms per meter cubed, giving a 36.8% error. The coefficient
of determination was calculated to be 0.994. This demonstrates that the data from this part of the
experiment was precise, but not accurate. A source of error was likely due to the inexact
measuring of the blocks due to a tightened grip on the vernier calipers. It is possible that the
cardboard may have been compressed, making the measurements more inaccurate.
4.
Conclusion:
Through this experiment, the density of solid objects was studied. A deeper
understanding of laboratory procedures and precise measurements were also examined. The
density of solid objects was studied. One was calculated with the volume of a set of cylinders,
and the other was calculated using a set of cardboard blocks.
was used in both parts of the
ρ experiment to represent density. The errors in this lab stemmed from improper measuring. To be
repeated with greater accuracy, the lab should be redone with measurements taken on a flat
surface.
5.
Data Sheet:
Next Page under Density of Matter
Experiment one: Hooke’s Law
1.
Introduction:
The purpose of this experiment was to study Hooke’s Law and its properties. This
lab explores the opposing directions of force and the change in position of the spring.
Force and the change in distance (extension) of springs were found with differing
weights. The further a spring’s position changes from equilibrium, the greater the
resultant force will be.
The equation to calculate the change in distance (position) is:
(4)
∆? = ?
𝑓
− ?
𝑖
Where
is the change in position,
is the final position, and
is the initial position of
∆? ?
𝑓
?
𝑖 the spring.
The equation to calculate the force of a spring is:
(5)
𝐹 =− ?∆?
Where F is the spring force, k is the spring constant, and
is the change in position.
∆?
2.
Experimental Procedures:
Materials and equipment needed for this procedure are: a force sensor, 850
Universal Interface, PASCO Capstone software (on computer), 2 springs (with different
spring constants), and a set of weights.
-
Step 1: Connect the force sensor to the 850 Universal Interface.
-
Step 2: Open the PASCO Capstone software on a computer.
-
Step 3: Locate the TOOLS tab and click Hardware setup, then choose the port that
is connected to the force sensor, and select the correct sensor from the dropdown
menu.
-
Step 4: Find the Displays tab (far right of the window) and click “graph” twice for
a force versus time graph.
-
Step 5: Hook the 50 gram weight holder to the force sensor.
-
Step 6: Click “Record” to collect data.
-
Step 7: Press the tare button on the force sensor to set the sensor to zero.
-
Step 8: Measure the position of the spring as the initial position.
-
Step 9: Add 40 grams of weight to the holder, then measure the change in distance
once the spring has finished oscillation.
-
Step 10: Repeat step 9 four more times.
-
Step 11: With a different spring, repeat steps 7-10.
3.
Results, analysis, and questions:
Table 1: Table 1 shows the change in position and the spring force of Spring 1 with an
initial position of 0.449 meters from the force sensor when the 50 grams of the weight
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holder on it. (40 grams is added each time to change the position of the spring.) The
calculated spring constant is also included.
Force (N)
Change in position (m)
Spring constant (k)
0.396
0.029
13.7
0.784
0.059
13.3
1.165
0.085
13.7
1.557
0.122
12.8
1.946
0.155
12.6
Based on table 1, graph 1 shows the relationship between the change in position and force
on Spring 1.
From graph 1, the line of best fit is 0.0814, which represents
(based on equation 4).
1
?
Therefore, the spring constant of Spring 1 is theoretically 12.3. The average experimental
spring constant of Spring 1 was found to be 13.2, which means that there was around a
7.32% error. The coefficient of determination was calculated to be 0.997. This
demonstrates that the data from this part of the experiment is relatively accurate. A
source of error is likely due to inexact estimations of the spring force from failing to
exactly determine the value on the computer.
Table 2: Table 2 shows the change in position and the spring force of Spring 2 with an
initial position of 0.464 meters from the force sensor when the 50 grams of the weight
holder is on it. (40 grams is added each time to change the position of the spring.) The
calculated spring constant is also included.
Force (N)
Change in position (m)
Spring constant (k)
0.423
0.067
6.31
0.816
0.125
6.53
1.203
0.192
6.27
1.608
0.239
6.73
1.995
0.307
6.5
Based on Table 2, graph 2 shows the relationship between the change in position and
spring force of Spring 2.
From graph 2, the slope of best fit was found to be 0.151, which represents
(based on
1
?
equation 4). Therefore, the spring constant of Spring 2 is theoretically 6.62. The average
experimental spring constant was calculated to be 6.41, meaning that there was a 3.17%
error. The coefficient of determination was calculated to be 0.997. This demonstrates that
the data from this experiment was very accurate. A possible source of error was likely
due to inexact estimations of the spring force from failing to exactly determine the value
on the computer.
4.
Conclusion:
Through this experiment, spring force and displacement were explored. The
slopes of the force versus change in position were
(as seen with equation 4). This law
1
?
determined that Hooke’s Law is dependent on which spring is used as springs have varied
properties, such as their durability and stiffness. Springs have different spring constants
that determine the amount of force needed to displace their position from equilibrium.
Hooke’s Law was found to not hold for larger forces as there is a point that a mass so
significant will be enacted on the spring that it either deforms it or will break the spring.
The errors in this experiment were due inexact estimations from computer rapid computer
readings. To increase the accuracy of the data, the lab should be repeated with spring’s
measurements being taken when the spring is completely done oscillating.
5.
Data sheet:
See above under Hooke’s Lab
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