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The Effect of Different Steel Structures on the Signal Strength of Radio Waves
Thanvir Ahmed and Nafis Jaigirdar
Macomb Mathematics Science Technology Center
Advanced Placement Physics
12 B
Mr. McMillan / Mrs. Cybulski / Mr. Acre / Mrs. Dewey
17 December 2015
The Effect of Different Steel Structures on the Signal Strength of Radio Waves
This experiment was conducted in order to research six different structural designs
and the effect that they would have upon the signal strength of a Samsung Galaxy S6 cell
phone. This was done because different structural designs have different effects on
electromagnetic waves. The different structural designs that were tested within this
experiment were: Solid Plate, Bubbled Plate, Striped Plate, Concave-Up Plate, Concave-
Down Plate, and a Base Plate. The response variable, or the dependent variable was the
signal strength of cell phone (dBm), this is the strength of the radio waves that reach the cell
phone. This research demonstrates which structures should be implemented in certain
scenarios, such as military bunkers preventing radio waves, or satellite dishes utilizing radio
waves.
This was done by placing the cell phone within a steel box, and then placing the
structure (the plate) being tested on top of the box. The cell phone had a preloaded
application to measure the signal strength which was launched prior to placing the phone
within the box. The signal strength of the phone was then recorded. The hypothesis stating
that the Concave Down Plate would cause the most amount of signal interference, and that
Concave Up Plate would cause the least amount of interference was accepted. This is based
on the results of the ANOVA test and the two-sample t tests. The t tests concluded that only
the Bubble Plate and the Striped Plate produced the same amount of interference. Box plots
and visual analysis concluded that the Concave Up Plate caused the least amount of
interference, and the Concave Down Plate caused the most.
Table of Contents
Introduction............................................................................................................................1
Review of Literature..............................................................................................................3
Problem Statement.................................................................................................................8
Experimental Design..............................................................................................................9
Data and Observations...........................................................................................................13
Data Analysis and Interpretation...........................................................................................16
Conclusion.............................................................................................................................22
Appendix A: Constructing Plates...........................................................................................27
Appendix B: Formulas and Sample Calculations..................................................................29
Appendix C: Professional Contact Conversation..................................................................32
Works Cited...........................................................................................................................40
Introduction
Communication is a vital part of human civilization. Communication serves as a
means to spread information, expanding knowledge beyond horizons never before imagined.
Today, the most used device is a cellular phone with 90% of adults in the United States
using a cell phone (Livingston). With the press of a couple of buttons, cell phones are able
connect people to the entire world. This connectivity, however, depends entirely on radio
waves. Cell phones operate and transmit data via electromagnetic waves with a frequency of
about 1900 MHz, known as radio waves. Interference of these radio waves can be caused by
many different factors. The wave can be reflected off of the surface of the material, refracted
through the material, or absorbed (partially or completely) by the material. This interference
inevitably decreases the signal strength of the radio waves being transmitted to and from the
phone. Lower signal strength results in poor reception and makes communication via cell
phone difficult, if not impossible.
There are numerous factors that can affect the signal strength of radio waves. An
electromagnetic wave can be altered by being reflected off of the surface of the material,
refracted through the material, or absorbed (partially or completely) by the material. All of
these interactions with matter can alter signal strength, which ranges from -130 dBm to -60
dBm, -60 dBm being excellent signal, and -130 dBm being terrible signal. The factor with
the most profound effect upon the signal strength is the propagation of the wave. The
propagation of a wave refers to the direction in which it travels forward at the speed of light.
It is a commonly observed occurrence that cell phone signal is lost when traveling through a
tunnel or entering a very large building. This is due to the fact that the propagation of the
radio waves is altered through diffraction, absorption, and reflection. The radio waves are
absorbed by the tunnel walls and spread out as a result of diffraction. Diffraction is the
bending of electromagnetic waves due to structural blocks. Different structural designs have
different effects upon the propagation of radio waves, ultimately having an effect on the
signal strength.
This experiment was conducted in order to research six different structural designs
and the effect that they would have upon the signal strength of a Samsung Galaxy S6 cell
phone. This was done because different structural designs have different effects on
electromagnetic waves. The different structural designs that were tested within this
experiment were: Solid Plate, Bubbled Plate, Striped Plate, Concave-Up Plate, and
Concave-Down Plate, as well as a Base Plate. The Base Plate had no plate causing
interference and served as a control for comparison. These different plates represent
different structural designs within the real world such as steel lined building, tunnels,
bunkers, and even satellite dishes. The response variable, or the dependent variable was the
signal strength of cell phone (dBm), which is the strength of the radio waves that reach the
cell phone.
Being able to determine the effect of different structural designs upon the signal
strength of radio waves would allow for certain structures to be implemented in certain
scenarios. For example, a military level bunker would want to minimize the amount of radio
waves being transmitted in and out of the building for security purposes. The most effective
way to do this would be to design the bunker in a specific way to interfere with the radio
waves. An architect who knows what structural design interferes with radio waves the most
would be able to design such a building.
Review of Literature
Cell phones are a vital part of daily life. Modern day smartphones can do just about
anything; however, they are limited by the range of their signals. Wireless communications
are constricted to a small portion of the electromagnetic spectrum. Cell phones, like other
forms of wireless communication, transfer information through radio waves, a form of
electromagnetic radiation. Radio waves have the characteristics of any other electromagnetic
wave, they have wavelengths and frequencies, but more importantly they interact with
matter. An electromagnetic wave can interact with matter in four different ways. The wave
can be reflected off of the surface of the material, refracted through the material, diffracted
off of the surface, or absorbed (partially or completely) by the material. All four of these
interactions cause interference with the path of the wave, and change the direction of the
wave (How Electromagnetic Radiation Interacts With Matter). Today, most buildings,
tunnels, or any other structures most likely have steel foundations. These structures interfere
with the transmission of radio waves by altering the propagation of radio waves. The goal of
this experiment was to uncover the effect of different structural designs so that the
interference of these structures upon radio waves can be minimized.
Most forms of wireless communication are transmitted through electromagnetic
waves such as radio waves. Radio waves have the longest wavelengths of all the
electromagnetic waves, and also have the lowest frequencies (Netting). The most common
form of wireless communication is cell phone use. Cell phones have a cell receiver and a
transmitter. These are both used to communicate information between the cell phone and the
cell tower that is emitting a radio wave to the cell phone. The frequencies of radio waves
range from 3 kilohertz (kHz) to 300 gigahertz (GHz). Most cell phones operate with
frequencies of either of 800 or 1900 Megahertz (MHz) (Lucas). Originally, radio waves
scrambled and interfered with other radio waves. If two stations were sending a radio signal
at the same frequency, then they would interfere with each other. This is no longer the case,
as most radio frequencies have their own purpose, specific radio channels have their own
frequencies. Radio frequencies also experience interference from different structures and
materials, such as steel and concrete. This is why cell phone reception is weak within
tunnels (Adam). Within this experiment, a cell phone operating at 1900 MHz was used, and
different steel structures were tested.
Radio waves do not require a medium to travel through because they are
electromagnetic waves. Matter can cause an interference with the propagation of radio
waves. The propagation of radio waves can be affected significantly by interference from
matter or other waves, and by reflection off of surfaces (Communications System). A
lustrous, or shiny, surface can change the path of a radio wave. Propagation refers to the
behavior of radio waves, from one point to another (Meisels). Diffraction is the bending of
electromagnetic waves due to structural blocks. In her experiment Regina Meisels, a
researcher for the Austrian Science Organization, tested the propagation levels of
electromagnetic waves when aimed and sent through different rock structures. In her
findings Meisels concluded that the rock type played a pivotal role in the strength of the
waves that transferred through, concluding that some of the waves were diffracted and some
were absorbed. Meisels used smooth surfaced rocks and rocks with a curved and a rough
surface in her experiment. These variations in strength can be attributed to a wide variety of
factors ranged from the amount of waves propagated to the amount absorbed by the rocks
themselves. Meisels used smooth curved rocks, and found that they allowed for stronger
signals. The trials that she ran with more rectangular rocks produced weaker signals.
Similarly, satellite dishes are shaped upwards at a curve, while tunnels are shaped
downwards at a curve.
Signal strength of cell phones is dependent upon the strength of the radio waves
emitted to and from them. Modern day smartphones can record the strength of the radio
waves, and users can view these records by downloading certain applications. The signal
strength of a cell phone is measured in decibel-milliwatts (dBm), or the power ratio in
decibels (dB) of the measured power referenced to one milliwatt (mW). This ranges from -
130 dBm to -60 dBm (Livingston). The signal strength of -130 dBm would result in no
signal, while the signal strength of -60dBm would result in excellent signal. The signal
strength of -130 dBm is nearly impossible to achieve, before conducting this experiment a
Faraday Cage was replicated to get a reading with no signal. “The point of a Faraday Cage
is to see if you measure zero when you should. It is done all the time in science to make sure
you are not getting fooled by false signals.” (Cinabro). Mr. Cinabro was contacted for his
extensive knowledge within the field of radio waves, a copy of this conversation is shown in
Appendix C. This works by surrounding a receiver, such as a cell phone, and preventing any
radio waves from reaching the phone. Likewise, these signal strengths will vary in different
conditions. For example, if the cell phone is outside with nothing interfering with the radio
wave transmission and if it is fairly close to a cell tower, the signal strength would be closer
to -60 dBm than -130dBm. However, if the cell phone is put inside of a building then the
interference from that building will cause the signal strength to lean more towards -130
dBm.
Another example of how electromagnetic propagation can be manipulated was
demonstrated by Chang-Fu Yang, Professor at the Taiwan Institute of Technology. In his
experiment Yang used ray tubing to propagate light particles in order to identify the path
that individual particles travel during propagation (Yang). A ray tube is a vacuum tube that
moves an electric beam back and forth. Although Yang’s experiment used light waves
similar results can be expected from radio waves. Based on the research conducted by both
Yang and Meisels it can be said that the two main reasons signal strengths are weaker after
traveling through objects are because of the absorption of the waves by different materials
and propagation.
The temperature of the medium is also another important factor in the penetration
ability of waves. It was found that lower temperatures reflect less of the waves (Hashimoto
et al). This was a study led by Hashimoto, a professor at the Tokyo National University. In
his experiment. Hashimoto and his peers tried to identify how a wave would propagate at
different temperatures. They concluded that at higher temperatures the particles which made
up the medium were moving faster, adding more space between each of the particles, and
allowing the electromagnetic waves to travel through. To avoid an error, precautions were
taken to maintain constant temperatures when heating or cooling a structure. The
temperature of the structures remained consistent throughout the trials to ensure accurate
data collection. This experiment was conducted within a vehicle that was parked
approximately 10ft away from a cell phone tower.
Another experiment was conducted at The Institution of Electrical Engineers by an
engineer known as Feodora Berz. Berz tested microwaves to identify the effect of
diffraction on the power of the wave. The power difference between the outermost rays and
the innermost rays was about 0.05% (Berz). The innermost rays were the stronger of the
two. Likewise, it is important to note that the placement of structures can change the amount
of signals that penetrate through. Diffraction of the radio waves alters the signal strength of
the wave because it spreads some of the wave across a surface. For the purpose of this
experiment precautions were taken to ensure that the structures always blocked the signal in
the same path, minimizing the fluctuations within the signal strength, which in turn
produced more accurate data.
Elevation also plays a critical role in the strength of radio wave signals. On average,
as the floor level of the building increases the overall signal quality of cell phones decreases
(Walker). This is due to atmospheric changes and conditions, and also the distance from a
cell tower increases with height. This means that the elevation at which the radio waves are
being tested must be kept constant. Overall, many precautions were taken based on the
research of Hashimoto, Berz, and Walker to avoid errors within the experimental design.
This included keeping the temperature of the structure, elevation of the transmitter/receiver,
and layout of the structures constant.
Wireless communication utilizes radio waves in order to share information. A
common use for radio waves is cell phones. An electromagnetic wave can be altered by
being reflected off of the surface of the material, refracted through the material, or absorbed
by the material. All of these interactions with matter can alter signal strength, which ranges
from -130 dBm to -60 dBm. The temperature, the elevation, and the layout of the structure
can also affect the signal strength, thus they should be kept constant when testing for the
signal strength of radio waves.
Problem Statement
Problem Statement:
How do different steel structural designs (Solid Plate, Bubbled Plate, Striped Plate,
Concave-Up Plate, and Concave-Down Plate) affect the propagation of electromagnetic
waves?
Hypothesis:
If different steel structural designs are used to cause interference with the
transmission of radio waves, then the Concave-Up Plate will produce the least amount of
interference.
Data Measured:
There was one independent variable and one dependent variable within this
experiment. The steel structural designs were held as the explanatory variable, or
independent variable. The different types of steel structures were Solid Plate, Bubbled Plate,
Striped Plate, Concave-Up Plate, and Concave-Down Plate. All of these plates had the same
surface area to eliminate any unwanted interference. The response variable, or the dependent
variable was the signal strength of cell phone (dBm), which is the strength of the radio
waves that reach the cell phone. There were 30 trials conducted for each plate. The order
that the trials were conducted was randomized in order to eliminate any bias. The signal
strength of the radio waves was measured without any interference as base to compare all
other trials to. A One-way Analysis of Variance (ANOVA) was conducted in order to
compare the means of all of the structures and determine if the different steel structures had
a significant effect upon the signal strength of radio waves
Experimental Design
Materials:
Samsung Galaxy S6 Cell Phone Network Signal Info AppSteel Curved Plate 7” X 7” Wiss 7” Metal Shear Scissors (4) Steel Plate Vertical Slits 1.75” X 7” Ti – Nspire CX Calculator Steel Solid Plate 7” X 7” Twist-It Ruler Steel Bubbled Plate 7” x 7”SentrySafe 7” X 7” Steel Box
Procedures:
1. Construct the plates required for the experiment. Instructions on how to cut these plates can be found in Appendix A.
2. Randomize the orders in which trials should be conducted by using the random integer function on the Ti – Nspire CX Calculator. There are 30 trials per plate, meaning 180 trials in total. These trials were grouped together and then randomized. This is done by grouping every 5 trials together, such that there are 36 groups. The order of these groups was then randomized with the random integer function.
3. Place the phone inside the center of the steel box. The phone should not move from this position until the trial is completed.
4. Launch the Network Signal Info App and then place the steel plate that correlates with the trial on top of the steel box, in order to cause interference with the signal strength of the cell phone.
5. For the trials using the Base Plate, there should be nothing placed on or in the box except for the cell phone.
6. For the Bubble Plate, place the plate on top of the box, such that the entire face of the box is covered.
7. For the Solid Plate, place the plate on top of the box, such that the entire face of the box is covered.
8. For the trials using the Concave Up Plate, the plate should be placed within the box in order to maximize the interference with the signal strength.
9. For the trails using the Concave Down Plate, the plate should be placed within the box in order to maximize the interference with the signal strength.
10. For the trails using the steel slits, the slits should be placed on top of the box, in a manner in which they fully cover the top of the box.
11. Wait approximately 1 minute for the Network Signal Info App to render, and then lift the steel plate up.
12. Record the signal strength of the cell phone that is shown on the application (this is an average).
13. Repeat steps 2 through 12 for all of the trials. Analyze the data using a One Way Analysis of Variance (ANOVA Test) and two-sample t Tests accordingly.
Diagrams:
Figure 1. Materials
Figure 1 shows the materials that were used throughout this experiment. It is
important to note that the steel plates were all positioned on top of the box and covered the
top completely in order to prevent any unnecessary propagation, and to maximize the
interference that the cell phone signals undergo. The materials that were unique to this
experiment were the different steel plates, the steel box, and the Samsung Galaxy S6.
Steel Curved Plate Steel Solid Plate Steel Bubbled Plate
Metal Shears Steel Plate Slits Ti – Nspire CX Calculator
Twist-It Ruler Calculator
Steel Box Calculator
Galaxy S6
Figure 2 shows the setup of the box. The cell phone was positioned inside the box
and directly under the steel plates. As shown, the steel plates were placed on top of the box
and made stable using the rim of the box, and the Network Signal Info App was running on
the phone. The trial shown in this figure is one which used steel strips. It is important to note
that in this figure two of the strips were removed to demonstrate how the phone was placed
in the box.
Figure 2. Box Setup
Steel Box Calculator
Steel Plate Slits
Galaxy S6
Figure 3. Network Signal Info App
Figure 3 is a screenshot of the data collected by the phone. The main focus of this
figure is signal strength of the cell phone, measured in decibel-milliwatts (dBm). Note that
the closer the dBm is to zero the better the signal strength of the phone. This was a trial with
no plate, and the signal strength is about -78 dBm, which is a very strong signal strength. It
takes approximately one minute for the application to get an accurate reading.
Data and Observations
Table 1Data Table
TrialBase
(dBm)Concave Up
(dBm)Striped(dBm)
Bubbled(dBm)
Solid(dBm)
Concave Down(dBm)
1 -76 -80 -86 -88 -94 -1032 -78 -81 -85 -85 -95 -1053 -77 -79 -87 -86 -95 -1034 -80 -82 -86 -85 -93 -1055 -78 -78 -86 -87 -92 -1066 -79 -80 -85 -88 -94 -1027 -77 -80 -86 -89 -92 -1058 -78 -77 -88 -87 -95 -1039 -76 -83 -87 -86 -94 -105
10 -81 -80 -86 -86 -96 -10311 -75 -80 -88 -87 -91 -10312 -76 -81 -86 -86 -94 -10613 -77 -82 -87 -86 -94 -10314 -78 -78 -86 -85 -95 -10515 -78 -79 -86 -85 -96 -10616 -79 -80 -85 -89 -93 -10417 -76 -80 -86 -87 -92 -10618 -81 -78 -85 -85 -92 -10519 -75 -83 -87 -86 -95 -10120 -77 -82 -88 -89 -94 -10621 -78 -77 -86 -86 -96 -10122 -79 -80 -85 -88 -93 -10623 -78 -80 -87 -89 -91 -10424 -79 -80 -86 -87 -95 -10525 -79 -78 -88 -86 -94 -10326 -76 -81 -85 -87 -93 -10227 -81 -79 -86 -86 -94 -10428 -78 -80 -88 -89 -94 -10429 -79 -82 -87 -87 -94 -10230 -79 -79 -86 -85 -96 -106
Average: -77.93 -79.97 -86.33 -86.73 -93.87 -104.07
Table 1 shows all of the data that was collected within this experiment. The lowest
average signal strength is affiliated with that of the Concave Down Plate. The highest
average signal strength was produced by the Base Plate, or the trials that had no plate. The
highest signal strength produced by a plate was by the Concave Up Plate. A box plot of this
data is shown in Figure 5.
Table 2Observations Table Trial Type Observation
18 Base The metal box was accidently closed shut before trial began then reopened, trial was restarted.
27 Base The metal box was accidently closed shut before trial began then reopened, trial was restarted.
19 Concave up Plate fell into the box however trial was reset and run again.20 Concave up Plate fell into the box however trial was reset and run again.29 Concave up Plate fell into the box however trial was reset and run again.
19 Concave down
Plate was slightly off center, trial was restarted.
22 Concave down
Waited for more than 1 minute, trial was restarted.
2 Striped Striped were placed with a larger gap, trial was run again.
28 Striped Striped were too close to one another, spread out, and trial was run again.
7 Bubbled Wrong side of plate was placed over box, trial was run again.20 Bubbled Wrong side of plate was placed over box, trial was run again.11 Solid Trial concluded before 1 minute, trial was run again. 23 Solid Plate was slightly off center, trial was restarted.
Table 2 shows the observations that were made for specific plates and the trial
number that correlates with them. The observations mainly include trials that were done
incorrectly, and had to be redone. The Bubbled Plate has two different sides, the side that
was placed up was the side in which the holes were drilled. Trials that were conducted with
the drilled face down were redone. The phone was placed within the box and the trials lasted
approximately one minute. Trials that lasted longer than a minute or less than a minute were
redone as well. The plates were poorly placed for some trials; these were also redone.
Figure 4 shows the setup of the box. The cell phone was positioned inside the box
and directly under the steel plates. As shown, the steel plates were placed on top of the box
and made stable using the rim of the box, and the Network Signal Info App was running on
the phone. The trial shown in this figure is one which used steel strips. It is important to note
that in this figure two of the strips were removed to demonstrate how the Samsung Galaxy
S6 cell phone was placed in the box. The image on the right shows that the cellphone
without any plates. This was a Base Plate trial, or a control. There were plates placed on this
in order to cause interference.
Data Analysis and Interpretation
Figure 4. Box Setup Before and After
Steel Box Calculator
Steel Plate Slits
Galaxy S6
The data that was collected must be analyzed to determine which of the steel plates
had the greatest effect upon the signal strength and which one had the least effect. There
were 30 trials for each individual plate, such that there were 180 trials in total. The order of
said trials was randomized with a Ti-Nspire calculator. This was done by grouping every 5
trials together, such that there were 36 groups. The order of these groups was then
randomized. This helps make the results valid, as randomization reduces bias. Each trial was
conducted independently, meaning the results of the trials did not affect each other. A One-
way Analysis of Variance (ANOVA) was conducted in order to compare the means of all of
the structures and determine if the different steel structures had a significant effect upon the
signal strength of radio waves. Two-sample t tests were then used to further analyze the data
by comparing the means of two independent samples. These were the appropriate tests to
use because there were six independent samples within this experiment: The Solid Plate,
Bubbled Plate, Striped Plate, Concave-Up Plate, Concave-Down Plate, and the Base (which
did not use a plate). These different plates were being tested to determine which one had the
greatest effect upon the signal strength of radio waves and which one had the least. An
ANOVA test compares all of the samples, the plates, to one another in order to determine
whether or not the effect on the signal strength was equal for all of the plates. There were
some overlaps within the box plot of the data collected from individual plates.
Consequently, Two-sample t tests were utilized to determine whether or not the effect on the
signal strength was equal for two different plates. Refer to Appendix B for sample
calculations of these tests.
-81
-79-78 -77
-75
Figure 5. Box Plots of Signal Strengths
Figure 5 is a box plot that illustrates the data that was collected in decibel-milliwatts
(dBm). The data is fairly normal, and there are not outliers. The medians of the individual
box plots are relatively close to their means, further indicating that the data is symmetric.
There are mean lines for each data set, which are indicated with a long vertical line on the
boxplots. It is important to note that the striped and the bubbled data have a significant
overlap. All of the data for the Striped Plate falls within the top 75% of the data for the
bubbled data. Consequently, a two-sample t test was conducted in order to identify if the
data between the two structures were in fact equal. The same was done for the data from the
Base and Concave Up Plates, as there is a noticeable overlap between these two data sets.
The Concave Down Plate had the greatest effect on the signal strength, as that data is the
farthest away from the Base Plate data.
Key
Base
Concave Up
Striped
Bubbled
Solid
Concave Down
1
-106-105
-104-103
-101
-96
-95 -94 -93
-91
-89
-88-86.5
-86
-85
-88
-87 -86
-85
-83
-81 -80 -79
-77
Signal Strength (dBm)
The box plot indicates that the different plates had different effects on the signal
strength, but an ANOVA test was still conducted in order to prove this statistically
significant. Before conducting an ANOVA test, there are certain assumptions that must be
met. The assumptions for an ANOVA test include independence of each case and the data to
come from a normal population. The standard deviations of the different plates are also very
close, indicating that the variances are equal. The trials were conducted separately and
independent of one another. The Central Limit Theorem states that the sampling distribution
of the sampling means approaches a normal distribution as the sample size gets larger, the
sample size for each plate is 30 trials, so this supports the claim of normality. The rule of
thumb for normality is that the largest standard deviation is not more than two times the
smallest standard deviation. The largest standard deviation was the Concave Up Plate with
1.61 dBm. The smallest was 0.99 dBm, with the Striped Plate. Since this meets the rule of
thumb, the data was assumed normal. There were no outliers within any of the box plots. All
of the assumptions were met for the ANOVA test, meaning that testing could proceed. The
hypothesis for the ANOVA compares the mean values from each of the different structures.
H o : μ1=μ2=μ3=μ4=μ5=μ6
H a : Not all of μ1=μ2=μ3=μ4=μ5=μ6
The null hypothesis states that the mean signal strengths for all structures are the same. The
alternative hypothesis states that the mean signal strengths for all structures are not all the
same. The ANOVA test was conducted with this hypothesis. The alpha level for this test
was 0.05, this is the level where the null hypothesis is either rejected or is failed to be
rejected.
Figure 6. One Way Analysis of Variance Test (ANOVA)
Figure 6 contains the results of the one way ANOVA test. The p-value is essentially
zero (5.0∗10−136). Consequently, the null hypothesis was rejected at an alpha level of 0.05.
This indicates that all of the trials do not produce the same signal strength. This also means
that there is approximately a 0% chance of getting results this extreme by chance alone if
the null hypothesis is true.
The results from the ANOVA test indicate that the signal strengths of the different
plates were not all equal; the plates produced different signal strengths. However, the data of
some plates overlapped with the data of other plates. These overlapping plates needed to be
tested in order to conclude whether or not the signal strength produced was equal between
them. To compare the data of two independent samples, a two-sample t test was conducted.
A two-sample t test compares the mean of two independent samples. There are certain
assumptions that must be met in order to conduct this test. The assumptions for two-sample
t test include independence of both cases, the data comes from a normally distributed
population, and equal standard deviations. As stated above that trials were independent of
one another. All of the assumptions were met for the two-sample t test, and the test was
conducted.
H o : μn 1=μn 2
H a : μn 1≠ μn 2
The null hypothesis states that the mean signal strengths for both structures are the same.
The alternative hypothesis states that the signal strengths for both structures are not the
same. This was the hypothesis that was used for both two-sample t tests below. The alpha
level for this test was 0.05. The data produced by the Bubble Plate overlapped with that of
the Striped Plate, the two-sample t test conducted in order to test is shown in Figure 7. The
data produced by the Base Plate overlapped with that of the Concave Up Plate, the two-
sample t test conducted in order to test this is shown in Figure 8.
Figure 7. Two-sample t test for Striped Plate and Bubbled Plate
Figure 7 displays the results from the two-sample t Test conducted using the data
from the Striped Plate and the Bubbled Plate. These results indicate that the null hypothesis
was failed to be rejected at an alpha level of 0.05. The t-value of 1.29 produced a p-value of
0.19. This value is larger than the alpha level. There is about a 19% of results like this
occurring by chance alone if the null hypothesis is true. This means that the Striped Plate
and Bubbled Plate provided the same amount of signal interferences and allowed for similar
amounts of radio signals to penetrate.
Figure 8. Two-sample t Test for Base Plate and Concave Up Plate
Figure 8 displays the results from the two-sample t Test conducted using the data
from the Base Plate and Concave Up Plate. The t value calculated to equal 4.82. This
correlates to a p-value of essentially zero. The null hypothesis can be rejected at an alpha
level of 0.05. This means that there is almost no chance of results this extreme by chance
alone, if the null is true. This also means that the Base Plate and Concave Up Plate
structures have different signal strengths and cause different amounts of interference on the
transmission of radio waves.
Conclusion
The purpose of this experiment was to determine which of the different steel
structural designs had the greatest effect upon the signal strength of radio waves. The
different steel structures were different steel plate designs that were used to cause
interference with cell phone signals. The plates that were being tested were Solid Plate,
Bubbled Plate, Striped Plate, Concave-Up Plate, and Concave-Down Plate. These plates
were placed on top of a cell phone and allowed to interfere with the cell phone signals being
transmitted to and from the phone. An application on the cell phone displayed the signal
strength. The signal strength of any cell phone ranges from -60 dBm to -130 dBm, -60 dBm
being excellent reception with the highest possible signal strength, -130 dBm being no
reception at all with the lowest possible signal strength. To verify that the application was
working correctly, the cell phone was wrapped in aluminum foil and observed, it had a
signal strength of about -128 dBm during this. This was done to mimic a Faraday Cage,
which is an instrument used to jam radio signal. The hypothesis stating that the Concave
Down Plate would cause the most amount of signal interference, and that Concave Up Plate
would cause the least amount of interference was accepted. The highest signal strength, with
no plate was -75 dBm, with a Base Plate or control trial. The highest signal strength
attainted by a trial with a plate in play to cause interference was -77 dBm, with the
Concave Up Plate. The lowest signal strength was 106 dBm, with the Concave Down Plate.
Evidence that supports this decision includes the results from the ANOVA test and results
from the two-sample t tests. The results from the ANOVA test concluded that not all of the
structures produced the same amount of interference. Based on the results of the ANOVA
test and the two-sample t tests, the null hypothesis, that all the structures interfered the same,
was rejected. With a p-value of essentially 0 in the ANOVA test, it was concluded that there
is almost no chance of collecting this data by chance alone if all the structures blocked the
same amount of signals. However, some of the data from the structures overlapped with one
another. Consequently, there were two-sample t tests conducted in order to compare this
overlapping data. The data produced by the Bubble Plate overlapped with that of the Striped
Plate, and the data from the Base Plate overlapped with that of the Concave Up Plate. With a
p value of 0.1997, the t test concluded that the Bubble Plate and the Striped Plate produced
the same amount of interference. This is due to the fact that both of these plates allowed for
the same amount of radio waves to escape and penetrate through the plate. These two plates
also had similar surface areas. Another two-sample t test was conducted in order to compare
the data from the Base Plate to that of the Concave Up plate. The p value for this t tests was
calculated to be approximately 0, indicating that the Concave Up Plate produced more
interference than the Base Plate. A box plot of all the data is shown in Figure 5. From this
box plot it is concluded that the structures produced different amounts of interference, as
there is minimal overlap. The box plot indicates that the Concave Up Plate produced the
least amount of interference, while the Concave Down Plate produced the most amount of
interference. This supports the hypothesis.
This conclusion is supported by the research of Regina Meisels, a researcher for the
Austrian Science Organization. Meisels tested the propagation, path and behavior of an
electromagnetic wave, properties of electromagnetic waves when aimed and sent through
different rock structures such as rounded and rough edged rocks. In her findings Meisels
concluded that the rock structure played a pivotal role in the strength of the waves that
transferred through. Similarly, it was found that the design of each steel plate plays a key
role in the propagation of the cell phone signals, and consequently the cell phone signal
strength. Meisels found that rounded rock and smooth surfaced rocks produced the strongest
signal strengths (Meisels). This coincides with the data collected from the Concave Up
Plate. Likewise, the upward curve-like structure of the Concave Up Plate allowed signal
strength to prorogate from the sides and be transmitted. Most satellite dishes are also shaped
in this manor, an upward facing curved plate. However, satellite dishes produce all of the
electromagnetic radiation, in the form of radio waves, and then transmit that radiation. In
this experiment, the Galaxy S6 cell phone was producing the radiation, and only portions of
that radiation were being absorbed by the plates. The unique shape of an upward curved
satellite dish increases the signal strength of electromagnetic waves because the waves are
allowed reflect to a focal point, and then be concentrated together and faced in the direction
in which they should be transmitted. Similarly, the Concave Up Plate produced the least
amount of interference. A diagram is shown below as to why this might have happened.
Base Plate (No Plate) Concave Up Concave Down
Figure 9. Diagram of Radio Waves
Figure 9 shows the possible reasons for why these results occurred. The Base Plate
produced the highest signal strength, as it had no plate interfering with it. The Concave Up
Plate produced the highest signal strengths of all of the plates. The Concave Up Plate was
closer to the cell phone and the radio waves. This may have allowed it to absorb the waves
and transmit them to a focal point that is represented with a dot on the diagram, similar to
how a satellite dish works. Some of the waves were diffracted by the plate, and were sent
around the plate, and some of the waves were reflected back into the box. This is why the
Concave Up Plate did not produce better signal strengths than a trial using no plate. The
Concave Down Plate produced the lowest signal strength because it was the farthest from
the source of the radio waves, the cell phone. The waves had more room to be reflected off
of the steel plate. The control trials had no plates, and thus produced the least amount of
interference.
Additionally, Meisels also found that rocks that were compressed together produced
higher levels of interference (Meisels). This correlates with the Concave Down Plate within
this experiment. The Concave Down Plate, shaped similarly to a tunnel, produced the
weakest signals. This is due to the downward curving shape of this plate. The radio waves
were the most isolated with this plate, as the plate covered the entire cell phone and was
closer than any the other plates. As a result, the radio waves were practically trapped under
the plate. Some of the waves were still absorbed by the plate, but the downward facing
curve caused for the waves to be reflected back into the box, leading to weaker signal
strength.
The difference in signal penetration of the structures can be attributed to the change
in power of the outer and innermost rays. This is explained best by the research of Feodora
Berz from The Institution of Electrical Engineers. In his experiment Berz tested microwaves
to identify the effect of diffraction on the power of the wave. The power difference between
the outermost rays and the innermost rays was about 0.05% (Berz). This explains why
structures that block off the outermost rays have lower penetrating abilities, and structures
that allowed more outer rays produced a higher signal strength (i.e. the Concave Up Plate
produced the best signal strength and the Concave Down Plate produced the worst signal
strength).
As in any experiment, there were some errors. One of the errors that could have
altered the data was the fluctuations of signals by cell towers. Most of the times the signals
that were collected varied by 3 to 4 dBm. This variation was most likely caused by
atmospheric fluctuation, such as different wind patterns and moisture in the atmosphere.
Randomization of the trials was implemented as a way to counteract this and reduce any
bias present. In order to minimize this fluctuation, the experiment could be conducted in a
controlled lab environment with a transmitter and receiver. This experiment used cell phone
signals, which are radio waves, which generally operate at a frequency of 1,900 Mhz. To
further look into this field of research different frequencies can be tested. This could be done
by testing different parts of the electromagnetic spectrum, such as microwaves or infrared
waves. All of the structures in this experiment were made out of steel, different materials
such as aluminum or lead can be tested. This research is relevant because it shows which
structural designs should be used for what purpose. For example, a military bunker should
be dome shaped in order to prevent radio signals from escaping or entering. An office
building or a satellite dish should be arc shaped upward in order to minimize the amount of
signal interference.
Appendix A: Constructing Plates
Materials:
JET 15” Model Drill Press Wiss 7” Metal Shear Scissors 36” X 36” Steel Plate 1/16” Thick Twist-It Ruler1/8” Drill Bit
Procedures:
1. Use the ruler to measure out a four 7” X 7” square plates from the steel plate.
2. Use the shears to cut out these four square plates.
3. Take one of the newly created plates and bend it such that it has a curve. The plate should be curved such that the length from one side to the other is 5” and the height of the plate should be 2”. This is the Concave Up and Concave Down Plate.
4. Take another plate and cut it into four even rectangles, such that each rectangle has a width of 1.75” and a height of 7”. These are the steel plate slits that will be used for the Striped Plate.
5. Take another plate and drill nine holes evenly amongst the plate using the drill press and drill bit, be sure to clamp down the plate before drilling. This is the Bubbled Plate. The holes are drilled 0.75” away from each other and 1” away from the border of the plate.
Diagrams:
Steel Curved Plate Steel Solid Plate Steel Bubbled Plate
Metal Shears Steel Plate Slits Twist-It Ruler CalculatorFigure 10. Materials
Figure 10 shows the materials that were to create the plates, and it also shows what
the finished plates should look like. The drill press and the drill bit are not shown within this
picture.
Appendix B: Sample Calculations
One Way Analysis of Variance Test (ANOVA):
An ANOVA test compares all of the samples to one another in order to determine
whether or not the effects for each individual factor were equal to one another. This is done
by comparing the means to one another. The variables and equation used for an ANOVA
test are shown below. There is also a sample calculation provided.
X=n1 x1+...+ni x i
N
x=each sample¿¿
n=each sampe¿¿
x1=each samplemean
N=totalobservation∈all samples
MSG=n1 ( x1−x )2+...+ni ( x i−x )2
I−1
MSE=(n1−1 ) s1
2+...+(ni−1 ) s i2
N−I
n=obsevations∈eachsample
s=standard deviaion of eachsample
N=number of observation∈all samples
I=number of populations
F= MSGMSE
=Mean square groupMeansquare error
F = Variation among sample means between each population variation among individuals in all sample of each populationFigure 11. Variables and Notation for ANOVA Test
Figure 11 lists the different variables and equations that are needed in order to conduct an ANOVA test. A sample calculation is shown in the figure below.
MSG=
30 (−77.933−−88.15 )2+30 (−83.7333−−88.15 )2+30 (−104.06−−88.15 )2
+30 (−79.966−−88.15 )2+30 (−93.866−−88.15 )2+30 (−86.33−−88.15 )2
6−1
MSE=
(30−1 ) 1.652+ (30−1 ) 1.362892+ (30−1 ) 1.57422+ (30−1 ) 1.607812
+(30−1 )1.4322+(30−1 ) 0.9942362
180−6
F= 2879.912039342.1137095019826
F=1362.4918829379
Figure 12. Sample Calculation for One Way Analysis of Variance Test
Figure 12 shows how the ANOVA test was conducted. The F - value of 1362.49 was
compared to a F table in order to calculate the p – value. The data that was used in this
sample calculation is from all of the data within this experiment, shown in Table
Two-sample t -Test :
To analyze the number of standard deviations away the data lies from the sample
mean, t, a two-sample t- test was conducted. In this equation, the difference of the sample
means is taken. This is divided by the square root of the sum of both standard deviations
divided by the number of trials. The variable x1 is the mean of the first sample dBm. The
variable x2 is the mean of the second sample dBm. The variable s1 is the standard deviation
of the first sample. The variablen1 is the number of trials that were conducted for the first
sample. The variable s2 is the standard deviation of the second sample. The variablen2 is the
number of trials that were conducted for the second sample. The p - value is calculated by
comparing the t - value with the degrees of freedom on a t Table. An alpha level of 0.05 was
used. The following equation was used to calculate the t value. t=
x1−x2
√ s12
n1+
s22
n2
A sample calculation of this two-sample t test is shown in the figure below. This
calculation shows the two-sample t test for the Striped Plate and the Bubbled Plate data.
t=x1−x2
√ s12
n1+
s22
n2
t=−86.333333 dBm−−86.7333333 dBm
√ 0.9942362
30+ 1.362892
30
t=1.29869
Figure 13. Two-sample t test Sample Calculation
Figure 13 shows how the two-sample t test was conducted. The t - value of 1.29869
was compared to a t table in order to calculate the p – value. The data that was used in this
sample calculation is from the Striped Plate and the Bubbled Plate. This data is shown in
Table 1.
Appendix C: Professional Contact Conversation
Nafis Jaigirdar <[email protected]>
Research follow up16 messages
Nafis Jaigirdar <[email protected]> Thu, Oct 8, 2015 at 7:42 AM
To: David Cinabro <[email protected]>
Hi Mr. Cinabro I still have not heard back from you on who I can contact for my research. Currently I am on the per experimental possess and have finished the review of lit portion of my paper. If you know anyone that would be interseted in helping a great cause please send them my info thank you
Problem Statement: To determine how different structural designs affect the propagation of electromagnetic waves.
David Cinabro <[email protected]> Thu, Oct 8, 2015 at 8:07 AM
To: Nafis Jaigirdar <[email protected]>
Hi Nafis
I will be happy to help. When can we talk? Can you come down to Wayne State and meet? Can I come out to meet you?
David Cinabro, [email protected] 313-577-2918http://motor1.physics.wayne.edu/cinabro.html
[Quoted text hidden]
Nafis Jaigirdar <[email protected]> Fri, Oct 9, 2015 at 8:27 AM
To: David Cinabro <[email protected]>
Hello,
Well, I guess we can just communicate through email for now and and if needed we can set up a time we can meet either in person or via skype (if you wanna talk about the research in depth skype would be the best way). So far we have finished the background research needed and are planning our first day of data collation today after school. If you could take a look at the document so far and let us know if there's anything we could add to the propagation of the waves it would be very helpful. So far our basic understanding is that propagation is the way a wave moves similar to diffraction. This document is essentially an explanation of the research others have completed and how it helps our understanding of the science behind our experiment.
It would also be wonderful if you can stop by and watch our presentation in January just as a heads up.
Anyways, we will keep in touch, and thanks again for taking your time to respond to help us.
[Quoted text hidden]
Review of Literature & work cited.docx21K
David Cinabro <[email protected]>Tue, Oct 13, 2015 at 7:33
AM
To: Nafis Jaigirdar <[email protected]>
Hi Nafis
I read through your literature review. I am still not clear what you are trying to do. The propagation of waves can be very complex. What exactly are you trying to test and how are you doing it?
David Cinabro, [email protected] 313-577-2918http://motor1.physics.wayne.edu/cinabro.html
[Quoted text hidden]
Nafis Jaigirdar <[email protected]> Wed, Oct 14, 2015 at 9:07 AM
To: David Cinabro <[email protected]>
I think these may clarify some of the misunderstandings you may have. Thank you for your help
[Quoted text hidden]
3 attachments
Problem Statement2.docx14K
Preliminary Experimental Design2.docx19K
_seniorresearchcontract_tips_1.doc26K
David Cinabro <[email protected]> Wed, Oct 14, 2015 at 9:21 AM
To: Nafis Jaigirdar <[email protected]>
Hi Nafis
This makes things clear. What is your "structure"? A picture or drawing of an example would help to clarify.
Have you thought about entering the Junior Science and Humanities Symposium? The web site is:
http://coe.wayne.edu/ted/science/jshs-index.php
You would have to do a write up and at the Symposium in March give a talk and present a poster.
David Cinabro, [email protected] 313-577-2918http://motor1.physics.wayne.edu/cinabro.html
[Quoted text hidden]
Nafis Jaigirdar <[email protected]> Fri, Oct 16, 2015 at 8:08 AM
To: David Cinabro <[email protected]>
Thank you this is perfect we were already making a poster for the MMSTC science fair in march however we are a group and this competition is for singles so unfortunately we cant enter.
These are some of the structures we will be testing in the picture.
[Quoted text hidden]
image.jpeg236K
David Cinabro <[email protected]>Mon, Oct 19, 2015 at 11:41
AM
To: Nafis Jaigirdar <[email protected]>
Group projects have been presented before, with one person representing the group. I have been telling them for years that they need to do something to deal with group efforts which are increasingly common in science.
Structure? It looks like a box.
David Cinabro, [email protected] 313-577-2918http://motor1.physics.wayne.edu/cinabro.html
[Quoted text hidden]
Nafis Jaigirdar <[email protected]> Mon, Oct 26, 2015 at 8:14 AM
To: David Cinabro <[email protected]>
sorry i haven't been keeping you updated on our experiment however we have finished our data collection and are currently starting a statistical anova test.
also yes these are steel plates we placed a phone in it and tested the strength of the signal that travels through
here is the final experimental design it should do a better job at explaining and it includes better visual figures. Also could you take a look at the data we collected i think its interesting how the concave down plate had the worst signal strengths i was expecting the solid to have the worst.
[Quoted text hidden]
3 attachments
DATA.tns5K
data.xlsx12K
Experimental Design.docx807K
David Cinabro <[email protected]>Wed, Oct 28, 2015 at 3:07
PM
To: Nafis Jaigirdar <[email protected]>
Have you tried with a different sort of phone?
Is the box always orientated in the same way? That is it always facing east or whatever? Have you done a test to see if that matters?
Does the signal strength depend on the presence of other cell phones being nearby? I think it does not, but have you checked?
In principal no signal should be able to penetrate a box made of conducting material, which is called a Faraday Cage. Have you tried to build such an object? It is very hard, but perhaps you could wrap a phone in aluminum foil and show that no signal gets through.
David Cinabro, [email protected] 313-577-2918http://motor1.physics.wayne.edu/cinabro.html
[Quoted text hidden]
Nafis Jaigirdar <[email protected]> Thu, Oct 29, 2015 at 8:22 AM
To: David Cinabro <[email protected]>
yes we have tried multiple phones and they have provided similar results with a few variations based on the antenna on the phone itself.
because all the data was collected in consecutively after each other we never had to move the box so yes it was orientated in the same way. The positioning of the box does not matter as much simply because the change falls with in our range of data anyways. (it was orientated perpendicular to a cell tower)
we have not tried to build a Faraday Cage. all of our tests were ran using a steel safe box. That is a interesting concept however we were aiming to identify the build that allowed the most signals, so I'm not sure how i can us a Faraday's Cage in our experiment.
[Quoted text hidden]
David Cinabro <[email protected]> Fri, Oct 30, 2015 at 1:46 PM
To: Nafis Jaigirdar <[email protected]>
The point of a Faraday cage is to see if you measure zero when you should. It is done all the time in science to make sure you are not getting fooled by false signals.
David Cinabro, [email protected] 313-577-2918http://motor1.physics.wayne.edu/cinabro.html
[Quoted text hidden]
Nafis Jaigirdar <[email protected]>Wed, Nov 11, 2015 at 7:22
AM
To: David Cinabro <[email protected]>
Hi sorry for the slow response I have been occupied with the data analysis and observation of our paper. I am happy to say that I have conducted test using foil as you suggested and the tests came up with no signals so the Faraday cage works. currently we are finishing up our data analysis and will start our intro and abstract next week then we start are conclusion the following week
I would also like to take this time to thank you for taking time out of your day to help us out the suggestions and questions you have added truly helped us get a better understanding of the research and further enhanced our paper.
[Quoted text hidden]
Nafis Jaigirdar <[email protected]> Mon, Nov 16, 2015 at 8:42 AM
To: David Cinabro <[email protected]>
Hi Mr. Cinabro
I am happy to say we have finished our data analysis and are now working on the intro and conclusion we are planing to finish the final paper some time in December and i will be sure to send you a copy
Once again i would like to take this time to thank you and invite you to our presentations with will be some time between 1/6-1/8 i will give you an exact data as the day approaches. I think you will be impressed with the amount of preparation my fellow students and i take in our research.
[Quoted text hidden]
David Cinabro <[email protected]> Tue, Nov 17, 2015 at 11:06 AM
To: Nafis Jaigirdar <[email protected]>
Let me know. I should be in town and would be interested to see.
David Cinabro, [email protected] 313-577-2918http://motor1.physics.wayne.edu/cinabro.html
[Quoted text hidden]
Nafis Jaigirdar <[email protected]> Fri, Dec 11, 2015 at 9:03 AM
Draft To: David Cinabro <[email protected]>
[Quoted text hidden]
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