Creation of Physics Experiment Kits on Sound Resonance in a Tube for Teachers in Southern Thailand

Main Article Content

Roseleena Anantanukulwong

Abstract


The objective of this research was to construct the resonance of sound waves in an air experimental media by comparing the velocity of sound waverecord at the maximum value using listening method and data logger program. The result presented that the speed of sound wave from listening was at the frequency of 500, 550, 600, 650 and 700 Hz were 349, 341, 351, 354 and 350 m/s respectively. The measurement errors were 0.14, 2.43, 0.42, 1.28 and 0.14 % respectively. The average sound velocity in the air by listening method was 349 m/s and the error percentage was at 0.12 %. The velocity of sound record by the data logger at frequency was 500, 550, 600, 650 and 700 Hz respectively, while the sound speeds were 344, 354, 346, 348 and 355 m/s respectively. The percentage error was at 1.57, 1.28, 0.42, 1.00 and 1.57 %. The data logger speed was 349.4 m/s, and the error percentage was at 0.05 %. The average speed of sound waves in the air was determined by the listening and the speed of sound using a data logger compared to the theoretical speed lof soundwith a deviation of less than 1 %, which can be used as an experimental laboratory media.

The objective of this research was to construct the resonance of sound waves in an air experimental media by comparing the velocity of sound waverecord at the maximum value using listening method and data logger program. The result presented that the speed of sound wave from listening was at the frequency of 500, 550, 600, 650 and 700 Hz were 349, 341, 351, 354 and 350 m/s respectively. The measurement errors were 0.14, 2.43, 0.42, 1.28 and 0.14 % respectively. The average sound velocity in the air by listening method was 349 m/s and the error percentage was at 0.12 %. The velocity of sound record by the data logger at frequency was 500, 550, 600, 650 and 700 Hz respectively, while the sound speeds were 344, 354, 346, 348 and 355 m/s respectively. The percentage error was at 1.57, 1.28, 0.42, 1.00 and 1.57 %. The data logger speed was 349.4 m/s, and the error percentage was at 0.05 %. The average speed of sound waves in the air was determined by the listening and the speed of sound using a data logger compared to the theoretical speed lof soundwith a deviation of less than 1 %, which can be used as an experimental laboratory media.



The objective of this research was to construct the resonance of sound waves in an air experimental media by comparing the velocity of sound waverecord at the maximum value using listening method and data logger program. The result presented that the speed of sound wave from listening was at the frequency of 500, 550, 600, 650 and 700 Hz were 349, 341, 351, 354 and 350 m/s respectively. The measurement errors were 0.14, 2.43, 0.42, 1.28 and 0.14 % respectively. The average sound velocity in the air by listening method was 349 m/s and the error percentage was at 0.12 %. The velocity of sound record by the data logger at frequency was 500, 550, 600, 650 and 700 Hz respectively, while the sound speeds were 344, 354, 346, 348 and 355 m/s respectively. The percentage error was at 1.57, 1.28, 0.42, 1.00 and 1.57 %. The data logger speed was 349.4 m/s, and the error percentage was at 0.05 %. The average speed of sound waves in the air was determined by the listening and the speed of sound using a data logger compared to the theoretical speed lof soundwith a deviation of less than 1 %, which can be used as an experimental laboratory media.


The objective of this research was to construct the resonance of sound waves in an air experimental media by comparing the velocity of sound waverecord at the maximum value using listening method and data logger program. The result presented that the speed of sound wave from listening was at the frequency of 500, 550, 600, 650 and 700 Hz were 349, 341, 351, 354 and 350 m/s respectively. The measurement errors were 0.14, 2.43, 0.42, 1.28 and 0.14 % respectively. The average sound velocity in the air by listening method was 349 m/s and the error percentage was at 0.12 %. The velocity of sound record by the data logger at frequency was 500, 550, 600, 650 and 700 Hz respectively, while the sound speeds were 344, 354, 346, 348 and 355 m/s respectively. The percentage error was at 1.57, 1.28, 0.42, 1.00 and 1.57 %. The data logger speed was 349.4 m/s, and the error percentage was at 0.05 %. The average speed of sound waves in the air was determined by the listening and the speed of sound using a data logger compared to the theoretical speed lof soundwith a deviation of less than 1 %, which can be used as an experimental laboratory media.


The objective of this research was to construct the resonance of sound waves in an air experimental media by comparing the velocity of sound waverecord at the maximum value using listening method and data logger program. The result presented that the speed of sound wave from listening was at the frequency of 500, 550, 600, 650 and 700 Hz were 349, 341, 351, 354 and 350 m/s respectively. The measurement errors were 0.14, 2.43, 0.42, 1.28 and 0.14 % respectively. The average sound velocity in the air by listening method was 349 m/s and the error percentage was at 0.12 %. The velocity of sound record by the data logger at frequency was 500, 550, 600, 650 and 700 Hz respectively, while the sound speeds were 344, 354, 346, 348 and 355 m/s respectively. The percentage error was at 1.57, 1.28, 0.42, 1.00 and 1.57 %. The data logger speed was 349.4 m/s, and the error percentage was at 0.05 %. The average speed of sound waves in the air was determined by the listening and the speed of sound using a data logger compared to the theoretical speed lof soundwith a deviation of less than 1 %, which can be used as an experimental laboratory media.


The objective of this research was to construct the resonance of sound waves in an air experimental media by comparing the velocity of sound waverecord at the maximum value using listening method and data logger program. The result presented that the speed of sound wave from listening was at the frequency of 500, 550, 600, 650 and 700 Hz were 349, 341, 351, 354 and 350 m/s respectively. The measurement errors were 0.14, 2.43, 0.42, 1.28 and 0.14 % respectively. The average sound velocity in the air by listening method was 349 m/s and the error percentage was at 0.12 %. The velocity of sound record by the data logger at frequency was 500, 550, 600, 650 and 700 Hz respectively, while the sound speeds were 344, 354, 346, 348 and 355 m/s respectively. The percentage error was at 1.57, 1.28, 0.42, 1.00 and 1.57 %. The data logger speed was 349.4 m/s, and the error percentage was at 0.05 %. The average speed of sound waves in the air was determined by the listening and the speed of sound using a data logger compared to the theoretical speed lof soundwith a deviation of less than 1 %, which can be used as an experimental laboratory media.

Downloads

Download data is not yet available.

Article Details

Section
Research Articles

References

[1] Tapparn, J., Chaofai, M., & Khongpakdee, S. (2018). Development of Experiment Set on Light Mixing Controlled bySmartphone. In The 9th Hatyai National and International Conference, 464-472. July 20-21, 2018. Blue Ocean Hall, Hatyai Business School Building, Songkhla : Hatyai University.

[2] Chanprasert, K. (2018). Development of the Experimental Set of PHY 136: Life Science Physics on Doppler Effect. Journal of Rangsit University: Teaching & Learning, 12(1), 69-106.

[3] Díaz-Melián, V. L., Rodríguez, L. A., Pedroso-Camejo, F., Mieres, J., de Armas, Y., Batista-Leyva, A. J., & Altshuler, E. (2019). Optics Undergraduate Experiments Using Smart (and Not So Smart) Phones. Revista Cubana de Fisica, 36(1), 4-7.

[4] Noiyano, O. (2011). The Study of the Results of Regeneration Management through Development Activity Package Learning Science Influence on the Learning Achievement and the Science Movement of Students Grade 3. Bangkok: Assumption School, Primary Department.

[5] Anupongongarch, P. (2011). Development of the Experiment Set for Studying Wave Resonance in Closed End Tube. Journal of Rangsit University: Teaching & Learning, 5(1), 5-19.

[6] Nakchuay, T., Kessaratikoon, P., & Khongpakdee, S. (2018). Development of Experimental Set on Resonance of Sound Using Smartphones and Polyvinyl Chloride (PVC) Tube. Thaksin University Journal, 21(3), 183-190.

[7] Wichasilp, C., Tonrak, S., & Insongjai, S. (2017). Development of Experimental Set for Electronic Devices and DC Circuits of Mathayomsuksa 6 Students. In The 17th Graduate Studies of Northern Rajabhat University Network Conference.
2497-2505. 21 July 2017. Wangchan Reverview Hotel. Phitsanulok: Pibulsongkram Rajabhat University.

[8] Khambun, A. (2018). The Development with Projectile Experimental Set by Automatic Angle. Advanced Science Journal, 18(1), 81- 96.

[9] Selapanvilawen, V. (2009). Man Experimental Set for Correcting the Misconception of Sound Waves. Independent Study, Master of Science Degree, Chiang Mai University.

[10] The Institute for the Promotion of Teaching Science and Technology. (2008). Teacher Manual for Additional Physics. Bangkok: Office of the Welfare Promotion Commission for Teachers and Education Personnel.

[11] Blackstock, D. T. (2000). Fundamentals of Physical Acoustics. New Jersey : A Wiley–Interscience Publication.

[12] Supap, S. (2015). General Physics. Bangkok: Triple Education Co., Ltd.