Uploaded by Ali JabbarzadehGangeh

Lab 6

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Ali J. Gangeh
Phys 4C
May 21, 2021
Lab 5: Acoustic Resonance and Beats
Objective:
The goal of this lab is to experiment on different frequencies and wavelengths to see if
the interfere and distort each other.
Equipment Used:
-
Phyphox app
-
Galaxy S8 phone
-
Lenovo desktop
-
Online tone generator
Procedure:
1. Create a tube with the a4 papers and tape
2. Place the ruler onto the tube with rubber bands
3. Fill the bottle with water from tap
4. Measured room temperature with Maveric thermometer (25C) and used it to calculate the
theoretical speed of sound
5. Placed my phone on top of the tube and used Phyphox app to play 1000Hz frequency
sound.
6. I lifted the bottle as far as I could along the tube (leaving 8cm at top) I then slowly
lowered it until I heard the most amount of sound.
7. I continued to do so until there was no more tube left and I recorded the distance from the
top for each peak in volume
8. I repeated this for frequencies 2000Hz, 3000Hz, and 4000Hz
9. Then I used these measurements to find the experimental wavelengths for each
frequency, subsequently finding the speed of sound.
Data:
Range of sounds I hear: 150-9000HZ
Part 2 (Beats):
All:
One period:
Expanded:
Super expanded, fast modulation:
Experimental results and analysis:
In the second graph we see half the period of a slow modulation.
The half period is: 255𝑚𝑠 − 60𝑚𝑠 = 195𝑚𝑠
A full period: 195𝑚𝑠 * 2 = 390
In the fourth graph we see the period of a fast modulation:
131. 4𝑚𝑠 − 130. 2𝑚𝑠 = 1. 2𝑚𝑠
Modeling beats:
𝑓𝑠𝑙𝑜𝑤 = 2. 564
1
𝑠
𝑓𝑠𝑙𝑜𝑤 = 833. 3
1
𝑠
ω𝑠𝑙𝑜𝑤 = 2 * π * 2. 564 =
1
2
(𝑤1 + 𝑤2) = 16. 11
1
𝑠
ω𝑓𝑎𝑠𝑡 = 2 * π * 833. 3 =
1
2
(𝑤1 − 𝑤2) = 5235. 8
1
𝑠
𝑤1 = 5235. 8
𝑤2 = 5219. 69
ω1 =
ω2 =
𝑤1
2π
𝑤2
2π
= 833. 30𝐻𝑧
= 830. 74𝐻𝑧
Conclusion and explanation of graphs:
The first two graphs show the distortion of the wavelengths. We see that in some places
the amplitude reaches almost zero as the two waves are interfering with each other, at other
places it peaks as the sound waves overlap. The amplitude is related to how loud the wave is.
Because of the distortion the amplitude of the sound wave changes over time. Once we zoom in
we see the sound wave itself. That is what the two last graphs depict. If we were only playing a
single frequency for the first two graphs we would see a blocklike structure but for the last two
we would see waves of uniform amplitude.
Through the graphs we were able to calculate the period of time it took for the slow
waves caused by distortion as well as the short waves of the sound itself. Through this period we
were able to recalculate our original frequencies. Our original frequencies were both about 20Hz
higher than our calculated frequencies. We had a percent error of 2.27% for the smaller
frequency and a error of 2.55% for the larger frequency. If I were to do this experiment again I
would further minimize this error through working in a quieter environment so random noise
wouldn’t effect my calculations.
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