sound – propagation

18
ENF1104 Problem Solving for Engineers – Acoustic Project Sound – Propagation

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Sound – Propagation. Sound Levels Sound / acoustic waves are pressure waves measured in Pa The amplitude of the wave is usually called the Sound Pressure Level (SPL) The human ear can detect SPL as low as 20  Pa (hearing threshold) The human ear can withstand SPL as high as 60Pa - PowerPoint PPT Presentation

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Page 1: Sound – Propagation

ENF1104 Problem Solving for Engineers – Acoustic Project

Sound – Propagation

Page 2: Sound – Propagation

ENF1104 Problem Solving for Engineers – Acoustic Project

Sound Levels• Sound / acoustic waves are pressure waves measured in Pa• The amplitude of the wave is usually called the Sound Pressure Level (SPL)• The human ear can detect SPL as low as 20Pa (hearing threshold)• The human ear can withstand SPL as high as 60Pa• The human ear has a dynamic range of 60 / 20x10-6 = 3,000,000• The human ear perceives SPL (nearly) logarithmically:

a 10-fold increase in sound power (or intensity) is needed for a human to perceive a doubling on loudness.

• The dB is based on the hearing threshold (20Pa)• Because acoustic power (P) is proportional to acoustic pressure (p):

2

2 610log 10log 20log 20log20 10ref ref ref

P p p pdBP p p x

Page 3: Sound – Propagation

ENF1104 Problem Solving for Engineers – Acoustic Project

Sound Levels – decibels

0 10000000 20000000 30000000 40000000 50000000 60000000 700000000

20

40

60

80

100

120

140

Sound pressure [Pa]

dB

Page 4: Sound – Propagation

ENF1104 Problem Solving for Engineers – Acoustic Project

Sound Levels – decibels

0 1,000,000 2,000,000 3,000,000 4,000,0000

20

40

60

80

100

120

140

Sound pressure ratio [reference: 20 Pa]

dB

Page 5: Sound – Propagation

ENF1104 Problem Solving for Engineers – Acoustic Project

Sound Levels – decibels

10 100 1000 10000 100000 1000000 10000000 1000000000

20

40

60

80

100

120

140

Sound pressure [Pa]

dB

Page 6: Sound – Propagation

ENF1104 Problem Solving for Engineers – Acoustic Project

Sound Levels – Examples:• The measured SPL in a room is 40Pa. What is the Sound level in dB?

6

6 6

40 1020log 20log 20log 2 620 10 20 10p xdB dBx x

20log 10 20dB dB

20log 100 40dB dB

6

1806 6 6 9 320 20

20log20 10

20 10 10 20 10 10 20 10 10 20 10dB

pdBx

p x x x x x Pa

• At the launch of India’s Polar Satellite Launch Vehicle (PSLV) rocket, you measure the sound level at 170 dB. How much acoustic pressure is measured by your microphone?

• The volume of a music player is increased by 10, what is the change in dB?

• The volume of a music player is increased by 100, what is the change in dB?

Page 7: Sound – Propagation

ENF1104 Problem Solving for Engineers – Acoustic Project

Reverberation time – Example:• A rich sound is produced in a room and suddenly stopped. Calculate the

reverberation time from the recorded acoustic pressure shown below:

0 1 2 3 4 5 6 7 8 9

-0.5

0

0.5

Elapsed time [s]

Sou

nd P

ress

ure

[-]

0 1 2 3 4 5 6 7 8 9-50

0

50

100

Elapsed time [s]

Mag

nitu

de [d

B]

Page 8: Sound – Propagation

ENF1104 Problem Solving for Engineers – Acoustic Project

Reverberation time – Example:• Remember: Reverberation time = time taken for sound to decrease by 60 dB

0 1 2 3 4 5 6 7 8 9

-0.5

0

0.5

Elapsed time [s]

Sou

nd P

ress

ure

[-]

0 1 2 3 4 5 6 7 8 9-50

0

50

100

Elapsed time [s]

Mag

nitu

de [d

B]

Page 9: Sound – Propagation

ENF1104 Problem Solving for Engineers – Acoustic Project

Reverberation time – Example:• Step 1: Compute moving RMS (Root-Mean-Square)• Note: Must select window width (in seconds)

0 1 2 3 4 5 6 7 8 9

-0.5

0

0.5

Elapsed time [s]

Sou

nd P

ress

ure

[-]

0 1 2 3 4 5 6 7 8 9-50

0

50

100

Elapsed time [s]

Mag

nitu

de [d

B]

Moving RMS [Pa]

Recorded sound [Pa]

Page 10: Sound – Propagation

ENF1104 Problem Solving for Engineers – Acoustic Project

Reverberation time – Example:• Step 2: Transform moving RMS into dB and plot

Moving RMS [Pa]

Recorded sound [Pa]

0 1 2 3 4 5 6 7 8 9

-0.5

0

0.5

Elapsed time [s]

Sou

nd P

ress

ure

[-]

0 1 2 3 4 5 6 7 8 9-50

0

50

100

Elapsed time [s]

Mag

nitu

de [d

B]

Moving RMS [dB]

Page 11: Sound – Propagation

ENF1104 Problem Solving for Engineers – Acoustic Project

Reverberation time – Example:• Step 3: Zoom in dB vs time curve if necessary

Moving RMS [Pa]

Recorded sound [Pa]

0 1 2 3 4 5 6 7 8 9

-0.5

0

0.5

Elapsed time [s]

Sou

nd P

ress

ure

[-]

4 4.5 5 5.5 6 6.520

40

60

80

100

Elapsed time [s]

Mag

nitu

de [d

B]

Reverberation Time:0.82327 [s]

Moving RMS [dB]

Page 12: Sound – Propagation

ENF1104 Problem Solving for Engineers – Acoustic Project

Reverberation time – Example:• Step 4: Select range (domain) for analysis

Moving RMS [Pa]

Recorded sound [Pa]

0 1 2 3 4 5 6 7 8 9

-0.5

0

0.5

Elapsed time [s]

Sou

nd P

ress

ure

[-]

4.2 4.4 4.6 4.8 5 5.2 5.4 5.6 5.8

30

40

50

60

70

80

90

Elapsed time [s]

Mag

nitu

de [d

B]

Reverberation Time:0.82327 [s]

SelectedRange foranalysis

Page 13: Sound – Propagation

ENF1104 Problem Solving for Engineers – Acoustic Project

Reverberation time – Example:• Step 5: Compute slope of dB vs time curve (straight line of best fit)

• Step 5: Compute Reverberation Tine (RT):RT=60/slope [s]

Moving RMS [Pa]

Recorded sound [Pa]

0 1 2 3 4 5 6 7 8 9

-0.5

0

0.5

Elapsed time [s]

Sou

nd P

ress

ure

[-]

4.2 4.4 4.6 4.8 5 5.2 5.4 5.6 5.8 6

30

40

50

60

70

80

90

Elapsed time [s]

Mag

nitu

de [d

B]

Reverberation Time:0.82327 [s]

Straight line of best fit: Slope [dB/s]

Page 14: Sound – Propagation

ENF1104 Problem Solving for Engineers – Acoustic Project

Reverberation Time – Example output from analysis software:

0 1 2 3 4 5 6 7 8 9

-0.5

0

0.5

Elapsed time [s]

Sou

nd P

ress

ure

[-]

0 1 2 3 4 5 6 7 8 920

40

60

80

100

Elapsed time [s]

Mag

nitu

de [d

B]

Reverberation Time:0.82327 [s]

0 1 2 3 4 5 6 7 8 9

-0.5

0

0.5

Elapsed time [s]

Sou

nd P

ress

ure

[-]

0 1 2 3 4 5 6 7 8 920

40

60

80

100

Elapsed time [s]

Mag

nitu

de [d

B]

Reverberation Time:0.82327 [s]

Moving RMS [Pa]

Recorded sound [Pa]

Moving RMS [dB]Decay slope [dB/s]

Page 15: Sound – Propagation

ENF1104 Problem Solving for Engineers – Acoustic Project

Sound – Hearing threshold

Page 16: Sound – Propagation

ENF1104 Problem Solving for Engineers – Acoustic Project

Sound – Hearing range

Page 17: Sound – Propagation

ENF1104 Problem Solving for Engineers – Acoustic Project

Sound - Octaves• Partitioning the frequency scale is a long-standing practice based on music• The octave is base of doubling or halving the frequency• Smaller increments are used for musical instruments (eg: piano) such as 1/3 or

1/12 octave• The reverberation time of a room may vary depending on the frequency of the

sound (dependent of the type of material that absorbs sound0• Too much time / effort required to evaluate RT for small frequency bands

(increments) over very large hearing range (20 – 20,000 Hz)• For practical purposes Octave Bands are used

Page 18: Sound – Propagation

ENF1104 Problem Solving for Engineers – Acoustic Project

Sound – Octaves bands

Lower limit (Hz)

(÷2)

Centre Frequency [Hz]

Upper limit (Hz)

(x2)

44 63 88

88 125 177

177 250 354

354 500 707

707 1000 1414

1414 2000 2828

2828 4000 5657

5657 8000 11314