The
purpose of this experiment is to make a comparison of various methods which are
used to calculate the buoyant force to the metal cylinder. The experiment also
intends students to understand and apply the Archimedes' principle which states
that the buoyant force is the weight of the fluid displaced by an object.
The
experiment was conducted in three methods by using a force probe, a string, a
beaker, a metal cylinder with hook, a meter stick, and a graduated cylinder. In
part A of the experiment, the weight of the metal cylinder in air and in water
were measured using the force probe, and the buoyant force was computed by
subtracting the weight of the metal in the water to that of the metal in the
air. In part B, the mass of a dry beaker was measured using the balance. The
cylinder was filled with full amount of water until it stops dripping. Next,
the metal cylinder was put into the cylinder, and let the water in the cylinder
overflows into the beaker. The mass of the water overflow was calculated by subtracting
the mass of the combination of the beaker and the water to the mass of the
beaker. The buoyant force was obtained by multiplying the mass of the beaker
and the acceleration due to gravity. In part C, the height and the diameter of
the metal cylinder were measured, and the volume of the cylinder was
calculated. The computed volume was used to calculate the buoyant force, B.
Figure-1: Measuring the weight of the metal cylinder using force
probe. This measurement was used in method A.
Figure-2: Overflow of water from
the graduated cylinder upon adding the metal into the cylinder. The water
overflow was captured by the beaker. This method was used to compute buoyant force
in part B.
Data and Analysis
Table-1: Recorded data for each method
Method
A
|
Method
B
|
Method
C
|
Wair =
1.13 ± 0.05 N
Wwater =
0.67 ± 0.05 N
|
Wbeaker=
0.15086 ± 0.00005 kg
Wbeaker+water=
0.19177 ± 0.00005 kg
|
h=0.076 ± 0.005 m
d=0.025 ± 0.005 m
|
Table-2: Comparison of buoyant force, B
Method
|
Equation
used to compute B
|
B(N)
|
Largest
possible B(N)
|
Smallest
possible B(N)
|
A
|
Wair -
Wwater
|
0.46 ± 0.10
|
0.56
|
0.36
|
B
|
(mbeaker+water -
mbeaker)g
|
0.40092 ± 0.00098
|
0.40190
|
0.39994
|
C
|
ρgV
|
0.37 ± 0.29
|
0.66
|
0.08
|
Discussion
According
to table-2, the values of the buoyant force calculated from different methods
were within the uncertainties of each other even though B value in each method
was greater or smaller than the others. Yet the results fell within their
uncertainties. For instance, the largest possible B in method A was 0.56N and
the smallest possible was 0.36N. Both of these numbers were within the values
of the other two methods. In same manner, the largest and smallest possible
buoyant force in method B and method C were within uncertainties of method A.
Among
these three methods, according to table-2, the method B was the most accurate
since it had the smallest uncertainty. In addition, as shown in table-1, the
devices used in method B measured to more decimal places comparing to the
devices used in other methods. Thus, less deviation from the actual values,
hence, greater accuracy. In contrast, method C had very great inaccuracy since
the only device used in method C was a meter stick. Since everyone reads the
measurements differently and the way each person measured were not the same; it
led to possible large deviations from actual values. The meter stick also did
not read to smaller decimal points which led to greater inaccuracy in the
measurement.
If
the cylinder had been touching the bottom of the water container in part A, the
buoyant force will be larger since there will be less tension detected by the force probe. Since there will also be a normal force adding to an upward force, smaller buoyant force will be required to equal to the same weight of the metal.
Conclusion
By applying the Archimedes’ principle in this
experiment, it was found that values of buoyant force in three different
methods were within the uncertainties of each other. Among these methods,
method B was the most accurate method.
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