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Sound and Intensity Transverse vs. Longitudinal Waves Sound Frequency

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Presentation on theme: "Sound and Intensity Transverse vs. Longitudinal Waves Sound Frequency"β€” Presentation transcript:

1 Sound and Intensity Transverse vs. Longitudinal Waves Sound Frequency
Sound Loudness Loudness and the Decibel Scale db Examples Intensity decrease with distance Other db scales

2 Transverse vs. Longitudinal Waves I
String (transverse) wave animation Air (longitudinal) wave animation Wavelength – distance between peaks at fixed time Frequency – time between repetitions at fixed position Velocity from wavelength and frequency 𝑣=π‘“πœ†

3 Transverse vs. Longitudinal Waves II
Transverse vs. longitudinal waves on slinky Transverse Longitudinal

4 Transverse vs. Longitudinal Waves III
Sound - Pressure wave vs. velocity wave

5 Waves on string vs waves in air
Both have Wavelength – distance between peaks at fixed time Frequency – rate of repetitions at fixed position (like your ear) Wave velocity 𝑣=π‘“πœ† Differences String wave velocity varies with tension and mass/length 𝑣= 𝑇 πœ‡ Air wave velocity set at 343 m/s (at 20Β° C) * *at any temperature π‘£β‰ˆ 𝑇 π‘š 𝑠 )

6 Frequency (pitch) of Sound Waves
Human ear ~ 20 Hz to 20,000 Hz (dogs higher)

7 Loudness (volume) of Sound Waves
Human ear can hear from about 10-12 W/m2 to 100 W/m2 - about 14 orders of magnitude!

8 Intensity and decibel scale
Range of human ear Intensity – 100 watts/m2 Make scale more convenient - β€œcompress” this Try Logarithms log 10 π‘₯ =π‘₯⁑ Method 3 gives most convenient scale Definition decibel (sound) 𝛽 𝑑𝑏 =10 π‘™π‘œπ‘” 𝐼 10 βˆ’12 Method Intensity Log Log(I) 𝐼= 10 βˆ’12 β†’ 10 2 πΏπ‘œπ‘” 𝐼 = βˆ’12 β†’ +2 Log(I/10-12) πΏπ‘œπ‘” 𝐼 10 βˆ’12 = 0 β†’ 14 10 Log(I/10-12) 10 πΏπ‘œπ‘” 𝐼 10 βˆ’12 =0 β†’140

9 Example - Intensity and db scale
Auto interior sound intensity 3 x 10-5 W/m2. What is decibel level? 𝛽=10 π‘™π‘œπ‘” 3βˆ™ 10 βˆ’ βˆ’12 =10 π‘™π‘œπ‘” 3βˆ™ (use calculator) =10βˆ™7.477β‰ˆ75 𝑑𝑏 (fractional logarithms OK) The sound level for a jet plane at takeoff is 140 db. What is the intensity? 10 π‘™π‘œπ‘” 𝐼 10 βˆ’12 = β†’ π‘™π‘œπ‘” 𝐼 10 βˆ’12 =14 𝐼 10 βˆ’12 = β†’ 𝐼= 10 2 =100 π‘Š π‘š ( 10 π‘™π‘œπ‘” π‘₯ =π‘₯) Logarithm rules on textbook inside back cover

10 Example 12-4 – Loudspeaker volume
3 db Intensity difference 10 π‘™π‘œπ‘” 𝐼 βˆ’12 βˆ’10 π‘™π‘œπ‘” 𝐼 βˆ’12 = 𝛽 2 βˆ’ 𝛽 1 =3𝑑𝑏 10 π‘™π‘œπ‘” 𝐼 2 𝐼 1 = (difference/quotient rule) π‘™π‘œπ‘” 𝐼 2 𝐼 1 =0.3 𝐼 2 𝐼 1 = =2 𝐼 2 =2 𝐼 1

11 Energy spreading in spherical wave
Intensity defined 𝐼= π‘ƒπ‘œπ‘€π‘’π‘Ÿ π΄π‘Ÿπ‘’π‘Ž For wave spreading over sphere 𝐼= π‘ƒπ‘œπ‘€π‘’π‘Ÿ 4πœ‹ π‘Ÿ 2 Ratio at 2 distances 𝐼 2 𝐼 1 = 1 4πœ‹ π‘Ÿ πœ‹ π‘Ÿ 1 2 𝐼 2 𝐼 1 = π‘Ÿ π‘Ÿ 2 2 General Rule: Inverse square law

12 Intensity/Amplitude variation with distance
𝐼 2 𝐼 1 = π‘Ÿ π‘Ÿ 2 2 Amplitude 𝐼∝ 𝐴 2 𝐼 2 𝐼 1 = π‘Ÿ 1 π‘Ÿ 2 Example Earthquake power 106 W/m2 at 100 km, what is it at 400 km? 𝐼 2 = 𝐼 π‘˜π‘š π‘˜π‘š 2 = 𝐼 1

13 Example 12-5 – Airplane roar
Translate 140 db at 30 m to intensity 10 π‘™π‘œπ‘” 𝐼 βˆ’12 =140 𝐼 βˆ’12 = 𝐼 1 =100 π‘Š Scale from 30 m to 300 m using inverse square law 𝐼 2 = 𝐼 π‘Ÿ 1 π‘Ÿ =100 π‘Š =1 π‘Š Translate at 300 m back to db 𝛽=10 π‘™π‘œπ‘” βˆ’12 =120 𝑑𝑏

14 FYI - Other β€œDecibel” scales
Sound db - referenced to W. 𝛽=10 π‘™π‘œπ‘” 𝐼 10 βˆ’12 Electrical dbm - referenced to 10-3 W. 𝛽 π‘‘π‘π‘š =10 π‘™π‘œπ‘” 𝐼 10 βˆ’3 2G/3G/4G/WIFI signal strengths (WIFI > -20 dbm near router.) Comcast checks cable modem this way. db always log of power ratio to some reference power. Cellphone signal strengths


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