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Texas Tech University *
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Civil Engineering
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Apr 3, 2024
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Lab Report #1: Page 1
TEXAS TECH UNIVERSITY
DEPARTMENT OF CIVIL, ENVIRONMENTAL, AND CONSTRUCTION
ENGINEERING
Lab Report #1: Fluid Properties
CE 3105 – Fluid Laboratory
Section: 303
Team Number: 2
Instructor: Theodore Cleveland
Authors:
Bradley Brooks
Conner Jeter
Ruben Ramos
Gabriel Vega
Date of Experiment: 1/29/2024
Date of Submission: 2/5/2024
Lab Report #1: Page 2
Table of Contents
Theory
........................................................................................................................................................
3
Apparatus
...................................................................................................................................................
7
Results
........................................................................................................................................................
9
Discussion
.................................................................................................................................................
10
Data Appendix
.........................................................................................................................................
11
Error Calculations
...................................................................................................................................
11
Sample Calculations
................................................................................................................................
11
List of Figures
Figure 1: Shear Stress Between Two Parallel Planes
Figure 2: Hydrometer and Other Specific Tools Used
Figure 3: Water Density and Specific Gravity Graph
Figure 4: Saltwater Density and Specific Gravity Graph
Figure 5: Glycerin Density and Specific Gravity Graph
List of Tables
Table 1: Recorded and Calculated results from the Density Measurements
Table 2: Calculated Salt Mass Results
Table 3: Recorded and Calculated Results of Specific Gravity
Table 4: Kinematic and Dynamic Viscosity
Table 5: Data Appendix with Calculated Results
Lab Report #1: Page 3
Theory
Density
is a crucial characteristic inherent to all substances, fluids included. It's commonly denoted by the symbol ρ and is defined as the ratio of a fluid's mass to the volume it occupies. Expressing it mathematically, density can be articulated as:
Density
=
Mass of the Liquid
Volume of the Liquid
ρ
=
M
V
At given temperature and pressures, the density of a fluid is constant. With that, the assumption that as mass of the liquid increases, so will the volume, with constant density. Density is measured in units of kg
m
3
(SI) or lb
ft
3
(US).
Specific Weight
is the weight per unit volume of a liquid. Weight is a force that can be calculated by multiplying the mass of a liquid by acceleration due to gravity (g).
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Lab Report #1: Page 4
SpecificWeight
=
Weight
Volume
γ
=
mg
V
At constant pressures and temperature, the specific weight of a fluid is constant.
Specific Gravity
, another significant property of fluids, is defined as the ratio of a fluid's density
to the density of water at the same temperature. Notably, water has a specific gravity of 1.0. Fluids with a higher density than water exhibit a specific gravity greater than 1, whereas those with a lower density than water have a specific gravity less than 1.
The formula for specific gravity can be defined as:
SpecificGravity
=
ρ
s
ρ
H
2
O
As a dimensionless quantity derived from the ratio of two densities, specific gravity plays a pivotal role in determining whether a fluid will float or sink in water. Moreover, it facilitates consistent comparisons of fluids across various units. Fluids, defined as substances unable to completely resist shear stresses, initiate flow when subjected to such stresses. Notably, different fluids exhibit varying flow rates under identical magnitudes of shear stress. Viscosity
serves as a metric for a fluid's resistance to shear stress, akin to internal resistance. Conceptually, viscosity represents the frictional forces between layers of fluid in relative motion. Dynamic viscosity
quantifies the tangential force per unit area needed to move one horizontal plane relative to another at a unit velocity while maintaining a unit distance apart.
Lab Report #1: Page 5
According to Newton’s law of viscosity, the shear stress τ
is proportional to the velocity gradient. Dynamic viscosity μ
is the constant of proportionality. It can be represented with the following equation:
τ
=
μ
du
dy
Figure 1: Shear Stress between two Parallel Planes
Dynamic Viscosity can be described as a ratio of shear force to the velocity gradient. It can be written in units of lb
ft
∗
s
(US). It can be found, especially in fluid mechanics, to encounter the
Lab Report #1: Page 6
ratio of dynamic viscosity over density, which is described as kinematic viscosity
. It can be described as:
υ
=
μ
ρ
Kinematic viscosity has units of m
2
s
(SI) or ft
2
s
(US). One way to calculate viscosity is recording
a table where the rate of a sphere will fall through a specific fluid of interest. Under equilibrium, the frictional forces that the sphere experiences will equal it’s weight. The sphere will fall at a constant velocity (terminal velocity). This phenomenon can be described as Stokes Law
. Using it, we can write out the equation:
u
=
gd
2
18
ν
(
σ
ρ
−
1
)
In the following equation, g is described as the acceleration due to gravity, d is the diameter of the sphere, ν
is the kinematic viscosity, σ
is the density of the sphere, and ρ
is the density of the given fluid.
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Lab Report #1: Page 7
Apparatus
Figure 2: Hydrometer and Other Specific Tools Used
Variables Used/Measured
Mass of beaker (g)
Beaker + Fluid (g)
Volume (mL)
Density of solution (g/mL)
Specific Gravity
Density of Sphere (kg/m^3)
Diameter of steel ball (in)
Diameter of Graduated Cylinder (mm)
Length (m)
Time (s)
Kinematic Viscosity (m^2/s)
Dynamic Viscosity (kg*m/s)
Density of Fluid (kg/m^3)
Lab Report #1: Page 8
Procedure
Part One: Density
1.
Take the temperature of the fluid using a thermometer.
2.
Use a scale to weigh the provided beaker.
3.
Fill the beaker with the fluid and record the combined mass (beaker + fluid) using the scale.
4.
Measure the volume of the fluid in the beaker accurately, either by using a graduated cylinder or estimating it by observing the fluid level in the beaker.
5.
Repeat all the above steps for each of the three liquids, ensuring consistency in the measurement process.
Part Two: Specific Gravity
1.
Carefully place the calibrated hydrometer into the fluid, ensuring it is fully immersed, and record the value corresponding to the lower meniscus.
2.
Repeat the measurement process three times for each assigned fluid to ensure consistency
and accuracy.
Part Three: Viscosity 1.
Take the steel ball (sphere) assigned to your group and measure its diameter.
2.
Gently release the ball into the ball guide, ensuring it falls smoothly.
3.
Record the volume readings corresponding to the upper and lower level markers (i.e., the two rubber bands).
4.
Begin timing with the stopwatch as soon as the ball reaches the first level marker (upper rubber band).
5.
Stop the stopwatch once the ball reaches the second level marker (lower rubber band).
6.
Use the density of stainless steel (7800 kg/m³) to calculate the volume of the sphere based
on the recorded volume readings.
7.
Repeat the entire process for each sphere assigned to your group.
Lab Report #1: Page 9
Results
Table 1. Part 1: Density Fluid
Mean (g/mL)
Std. Dev. (g/mL)
Water
.925
0.05173
Salt Water
.973
0.00
Glycerin
1.65
0.05050
Table 2. Part 1: Mass salt in Brackish Water Fluid
Salt Mass (g)
Mean (g)
Std. Dev. (g/mL)
Trial 1 Salt Water
.933
1.02
0.886
Trial 2 Salt Water
.975
Trial 3 Salt Water 1.01
Table 3: Part 1: Specific Gravity Fluid Mean Std. Dev.
Water
1
0
Salt Water
1.063
.01528
Glycerin
1.245
.02092
Figure 3. Water Density vs. Specific Gravity Figure 4. Salt Water Density vs. Specific Gravity
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Lab Report #1: Page 10
Figure 5. Glycerin Density vs. Specific Gravity
Table 4. Part 2: Kinematic and Dynamic Viscosity Variable
Mean (kg/ms)
Std. Dev. (kg/ms)
Kinematic Viscosity
.000576
.742
Dynamic Viscosity
.000656
.846
Discussion
During the experiment, several complications that may have occurred influenced the set
experiment are the following. One is the inclusion of foreign agents within the precision 10ml
(about 0.34 oz) dropper, and the beakers being potentially contaminated with other reactants.
And for the following experiments proceeding the instruments have yet to be calibrated to a set
0. And the final experiment of viscosity on the surface of an object could have human and
instrumentation error.
The first experiment consisting of the fluid's density cannot be completely accessed without a
shadow of skepticism because the container/ beaker is potentially influenced by other products
residual from past experiments. Despite our efforts to rinse and wipe the influence from small
traces although minuscule are still present. For further consideration, a set of containers should
be reserved for certain fluids such water and salt water and glycerin.
The second experiment preceding is the specific gravity. A major issue was the instrument of
measurement struggle to give a reading to glycerin, perhaps due to its uncalibrated nature. One
other notion to consider is the opportunity that is presented when an external force influences the
placement of the instrument in the fluid.
For the final experiment since the method of recording involves human judgement from a
recording. It is subject to some form of biases and weights that prohibit it from being completely
empirical. Therefore, the analysis should be considered with the variance of a sd of a human
factor in mind.
Lab Report #1: Page 11
Data Appendix
Error Calculations
Some of the calculations we found can have minor inaccuracies in the data with human error on reporting density calculations in the lab. It may have appeared that some of the density calculations for water may be inaccurate, which may have been caused by an accidental water spill on the scale of the scale.
Sample Calculations
ρ
=
M
V
=
(
166.85
−
115.86
)
g
30
mL
=
1.70
g
mL
mean
=
Σ a
i
n
=
(
1.70
+
1.64
+
1.60
)
3
=
1.65
g
mL
Std .dev .
=
√
(
1
n
−
1
)
Σ
(
x
i
−
x
)
2
=
√
(
1
3
−
1
)
(
(
1.7
−
1.65
)
2
+
(
1.64
−
1.65
)
2
+
…
)
=
.05050
g
Mass of Salt
=
(
M
s
=
V
sw
(
ρ
sw
−
ρ
w
)
)
=
30
(
1.01
−
1.00
)
=
.300
g
Length
=
V
π d
2
4
=
400
mL
π
(
60
mm
)
2
4
=
0.14
m
Velcocity
=
L
t
avg
=
.14
m
(
1.76
+
2.27
)
2
=
0.0693
m
s
Lab Report #1: Page 12
Dynamic Vis.
=
gd
2
18
u
(
σ
ρ
−
1
)
=
(
9.81
m
s
2
)
(
0.06
m
)
2
(
7800
kg
m
3
1285
kg
m
3
−
1
)
18
(
0.0693
m
s
)
=
0.144
kg
m
⋅
s
Kinematic Vis.
=
μ
ρ
=
0.144
kg
m
⋅
s
1285
kg
m
⋅
s
=
0.000112
m
2
s
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Lab Report #1: Page 13
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