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246

9 Sound Pressure Levels and Octave Bands

Fig. 9.1 Frequency response for the A-, B-, and C-weighting

A-weighted sound pressure level (spectrum) can be calculated by adding the unweighted sound pressure level and A-weighted gain or loss as shown below:

Lp½dBA& ¼ Lp½dB& þ A weighting

Therefore, A-weighted spectrum is given by:

(33.8, 49.3, 72.8, 80, 47.2) dB at (125, 250, 500, 1000, 2000) Hz, respectively

(c) A-weighted SPL [dBA]:

LpT ½dBA& ¼ 10 log 10

33:8

þ 10

49:3

þ 10

72:8

80

þ 10

47:2

 

10

10

10

þ 1010

10

¼10 log ð2399 þ 85114 þ 1:9E7 þ 10:0E7 þ 52481Þ ¼ 10 log ð11:9E7Þ ¼ 80:8 ½dBA&

Therefore, the A-weighted SPL ¼ 80.8 [dBA].

9.5Homework Exercises

Exercise 9.1

The mathematical expression for a level is:

9.5 Homework Exercises

 

 

 

247

 

L ½dB& ¼ 10 log 10 Ur

 

 

 

 

U

 

Use the law of conservation of energy to show that the following formula for the

total (combined) level is valid:

 

 

 

Ltot ¼ 10 log 10

10L110½dB&

þ 10L210½dB&

þ . . .

þ 10Ln10½dB& ½dB&

Exercise 9.2

The sound pressure levels measured in the following ve octave bands are:

Center frequency fo[Hz]

250

500

1000

2000

4000

Sound pressure level Lp[dB]

90

72

82

65

50

(a)Determine the unweighted sound pressure level.

(b)Determine the A-weighted spectrum of the octave bands.

(c)Calculate the A-weighted sound pressure levels.

(d)What is the PSIL and communication voice level at 1.2 m between a speaker and a listener?

(Answers): (a) 90.7 [dB]; (b) (81.3, 68.8, 82.0, 66.2, 51.0) [dBA]; (c) 84.9 [dBA];

(d) 73 [dB], shouting.

Exercise 9.3

The sound pressure levels measured in ve of the octave bands are given below:

Center frequency fo[Hz]

125

250

500

1000

2000

Sound pressure level Lp[dB]

35

45

65

70

60

(a)Determine the unweighted sound pressure level.

(b)Determine the A-weighted spectrum of the octave bands.

(c)Calculate the A-weighted sound pressure levels.

(d)What is the PSIL and communication voice level at 1.5 m from a listener?

(Answers): (a) 71.5 [dB]; (b) (18.8, 36.3, 61.8, 70.0, 61.2) [dBA]; (b) 71.1 [dBA];

(c) 65 [dB], very loud voice.

Exercise 9.4

Given the time domain function p(t) below:

p(t) ¼ 0.02 cos (2π 500 t) + 0.04 sin (2π 1000 t)+ 0.06 cos (2π 1500 t) + 0.08 sin (2π 2000 t)[Pa]

248

9 Sound Pressure Levels and Octave Bands

(a)Determine the total (combined) sound pressure level (SPL) using:

(i)The summation of the squares of the RMS pressures.

(ii)The SPLs of all individual frequencies.

(iii)The SPL spectrum of octave bands.

(b)Determine the A-weighted sound pressure level (SPL) based on the sound level conversion table.

(Answers): (a) i-iii 71.76 [dB]; (b) 72.72 [dBA].

Exercise 9.5

Given the sound pressure function p(t):

pðtÞ ¼ 0:03 cos ð2π 400 tÞ þ 0:04 sin ð2π 400 tÞ

þ0:06 cos ð2π 1200 tÞ þ 0:08 sin ð2π 1200 tÞ þ0:09 cos ð2π 1600 tÞ þ 0:12 sin ð2π 1600 tÞ½Pa&

(a)Calculate the unweighted sound pressure level.

(b)Calculate the A-weighted sound pressure level.

(c)Calculate the preferred speech interference level (PSIL).

(d)Determine the communication voice level at 0.6 m from a listener.

Hint: Combine the harmonic waves of the same frequencies into one harmonic wave function using the four equivalent forms.

(Answers): (a) 76.41[dB]; (b) 77.08[dBA]; (c) 70.14 [dB]; (d) raised voice.

Exercise 9.6

Given the sound pressure function p(t):

pðtÞ ¼ 0:05 cos ð800πtÞ þ 0:10 cos ð2400πtÞ þ 0:15 cos ð3200πtÞ½Pa&

(a)Calculate the unweighted sound pressure level.

(b)Calculate the A-weighted sound pressure level based on the sound level conversion table.

(c)Calculate the preferred speech interference level (PSIL).

(d)Determine the communication voice level at 0.6 m from a listener.

Answers): (a) 76.41[dB]; (b) 77.08[dBA]; (c) 70.14 [dB]; (d) raised voice.

9.5 Homework Exercises

249

Exercise 9.7

The sound pressure levels measured in ve of the octave bands are given below:

Center frequency fo[Hz]

125

250

500

1000

2000

Sound pressure level Lp[dB]

35

45

65

70

60

(a)Determine the unweighted total sound pressure level.

(b)Calculate the A-weighted sound pressure level.

(c)Calculate the preferred speech interference level (PSIL).

(d)Determine the communication voice level at 1 m from a listener.

(Answer): (a) 71.52 [dB]; (b) 71.08; (c) 65 [dB]; (d) raised voice.

Chapter 10

Room Acoustics and Acoustical Partitions

This chapter introduces room acoustics and acoustical partitions. Room acoustics studies the change of energy density at different locations due to the conditions of direct and reected sound. Acoustical partitions are used to reduce noise from a source.

Formulas for evaluating transmission loss (TL) and noise reduction (NR) in a room due to partition walls are formulated in this chapter.

This chapter is organized into ve sections as described below:

Section 10.1 introduces and denes three acoustic quantities: sound power (Sect. 10.1.1), acoustic intensity (Sect. 10.1.2), and energy density (Sect. 10.1.3). These acoustic quantities are used for deriving the formulas of transmission loss (TL) and noise reduction (NR). These three acoustic quantities are also commonly used in the analysis of room acoustics.

Section 10.2 introduces and denes three room quantities: absorption coefcient of surfaces (Sect. 10.2.1), room constant (Sect. 10.2.2), and reverberation time (Sect. 10.2.3). These room quantities are used in the analysis of room acoustics in the next section (Sect. 10.3).

Section 10.3 focuses on the analysis of room acoustics. A formula for calculating sound pressure level due to both direct and reverberant sound waves from a sound source is summarized below:

Q

4

 

LP ¼ Lw þ 10 log 4πr2

þ

 

 

R

where LP is the sound pressure level at a distance r from the acoustic source considering both the direct and reverberant sound waves, Lw is the sound power of the acoustic source, Q is the directivity factor of the acoustic, and R is room constant. The equation above will be derived in this section.

Section 10.4 introduces transmission loss (TL) due to acoustical partitions. A formula that relates the transmission loss (TL) to the incident sound pressure level (Lwi) and transmitted sound pressure level (Lwt) will be dened and is summarized

© The Author(s), under exclusive license to Springer Nature Switzerland AG 2021

251

H. Lin et al., Lecture Notes on Acoustics and Noise Control, https://doi.org/10.1007/978-3-030-88213-6_10