Пресс-релиз популярных книг
.
Авторы: 111 А Б В Г Д Е Ж З И Й К Л М Н О П Р С Т У Ф Х Ц Ч Ш Щ Э Ю Я
Книги: 164 А Б В Г Д Е Ж З И Й К Л М Н О П Р С Т У Ф Х Ц Ч Ш Щ Э Ю Я
На сайте 111 авторов, 92 книг, 72 статей, 5913 глав.
38.5 Psychological Effects of Noise
In this section, certain generally accepted aspects of the psychological effects of noise will be discussed
and quantified. Various indexes have been proposed that quantify the psychological effects of noise.
However, only a few of indices, loudness (sones), noise-criteria (NC) curve, and sound level, are introduced
in the following presentation.
38.5.1 Loudness Interpretation
As was discussed relating to Figure 38.2, loudness level is measured in phons, and the related quantity,
loudness, is measured in sones. A sone is defined as the loudness of a 1000 Hz pure tone with a sound
pressure level of 40 dB. On recalling the definition of loudness level, or by referring to Figure 38.2, one
notes that 40 phon have a loudness equal to 1 sone. This relationship may be simply expressed as
S ¼ 2ðLL 240Þ=10 sone ð38:1Þ
where S ¼ loudness (sones), LL ¼ loudness level (phons), or conversely
LL ¼ 33:2 log S þ 40 phon ð38:2Þ
Example 38.2
Make the following two conversions using the appropriate equation (Equation 38.1 or Equation 38.2):
(1) convert 80 phon to sone, (2) convert 100 sone to phon.
Solution
1. To convert phons to sones, use Equation 38.2:
S ¼ 2ðLL 240Þ=10 ¼ 2ð80240Þ=10 ¼ 24 ¼ 16 sone
2. To convert sones to phons, use Equation 38.2:
LL ¼ 33:2 log S þ 40 ¼ 33:2 log 100 þ 40 ¼ 66:4 þ 40 ¼ 106:4 phon
How should we determine the “total loudness” (sones), when the sound is composed of
multiple frequency components? Probably the most widely used method for establishing the loudness
of a complex noise is that developed by Stevens [2]. The method is based on the measurement of the
1-octave, 1/3-octave, or 1/2-octave band pressure levels. The measured band pressure levels are used
38-4 Vibration and Shock Handbook
© 2005 by Taylor & Francis Group, LLC
in conjunction with the equal loudness index contours shown in Figure 38.3 to determine the loudness or
loudness level by means of a simple calculation.
A step-by-step outline of the procedure is as follows:
1. Measure the band pressure levels (1-octave, 1/2-octave, or 1/3-octave) over the frequency range of
interest. Usually, the range chosen is from about 50 to 10,000 Hz.
2. Enter the center frequency and band pressure level for each band in the contour of Figure 38.3, and
determine the loudness index for each band.
3. Calculate the total loudness, St; in sones, by using
St ¼ Imð1 2 KÞ þ K
Xn
i¼1
Ii ðsoneÞ ð38:3Þ
where St ¼ the total loudness (sones), Im ¼ the largest of the loudness indices, Ii ¼ the loudness
indices, including Im, K ¼ weighting factor for the bands chosen. K ¼ 0:3 for 1-octave bands,
K ¼ 0:2 for 1/2-octave bands, K ¼ 0:15 for 1/3-octave bands.
50
10
20
30
40
50
60
70
Band pressure [dB]
80
90
100
110
120
120
100 200 500
Frequency [Hz]
1 k 2 k 5 k 10 k
0.1
0.2
0.3
0.5
0.7
1.0
1.5
2
2.5
3
4
5 6
8
10
12
15
20
30
40
50
60
80
100
150
Loudness
Index
FIGURE 38.3 Equal loudness index contour [2].
Hearing and Psychological Effects 38-5
© 2005 by Taylor & Francis Group, LLC
4. If so desired, one may calculate the loudness level in phons using Equation 38.2, or one may
convert to loudness level by means of the conversion curve of Figure 38.3.
Example 38.3
A particular complex noise was measured to yield the one-octave band pressure given in the
following table
Compute the loudness level using the procedure described before.
Solution
As a first step, the loudness indices are determined from Figure 38.3 and recorded in tabular form with
the band pressure levels. Next, we note that one-octave bands have been used. Therefore K ¼ 0:3 in
Equation 38.3, and
St ¼ Imð1 2 0:3Þ þ 0:3
X8
i¼1
Ii
From the table above, we find that Im ¼ 29.0 sone and, summing up, find
P
Ii ¼ 97:9 sone: Therefore,
St ¼ 29ð1 2 0:3Þ þ 0:3ð97:9Þ ¼ 49:67 sone
We find that the loudness, St ø 50 sone: The loudness level may now be calculated by means of Equation
38.2 as
LL ¼ 33:2 log St þ 40 ¼ 33:2 log 50 þ 40 ¼ 96:4 phon
Therefore, LL; the loudness level, is 96 phon.
38.5.2 Noise-Criteria Curves
Noise-criteria curves, which are neglected here, were established in 1957 for rating indoor noise. The
curves have been utilized as one method of rating background noise level in a room. Each curve specifies
the maximum octave-band sound pressure level for a given NC rating. If the octave band levels for a given
noise spectrum are known, the rating of that noise in terms of the NC curves is given by plotting the noise
spectrum on the set of NC curves to determine the point of highest penetration.
In 1971, some objections to the NC curves led to their modification. The new curves, which are shown
in Figure 38.4, are called the preferred noise-criteria (PNC) curves. Although these curves differ from the
NC curves, they are used in exactly the same manner.
Center Frequency
(Hz)
Band Pressure
Level (dB)
Loudness Index
(sone)
63 66 2.5
125 63 3.2
250 65 4.8
500 70 7.5
1000 73 10.6
2000 76 15.2
4000 81 25.1
8000 79 29.0
38-6 Vibration and Shock Handbook
© 2005 by Taylor & Francis Group, LLC
Example 38.4
Solution
The highest penetration is found at 500 Hz on PNC-60. Hence, the answer is PNC-60.
38.5.3 Sound Level
Sound levels are sound pressure levels that have been weighted according to a particular weighting curve.
Three weightings, A, B, and C, and associated sound levels, have been developed as a method to
subjectively evaluate the impact of noise upon the human ear, in a proper manner. The frequency
response and decibel conversions from a flat response for each of these weightings are given in Figure 38.5
and Table 38.1, respectively.
The A-weighting network is now used almost exclusively in measurements that relate directly to the
human response to noise, both from the viewpoint of hearing damage and of annoyance. Such
measurements are referred to as sound level measurements. Sound level is designated by L and the
designated unit is the dBA. Similarly, dBB and dBC are used to designate sound level weighted by B
weighting and C weighting networks, respectively.
31.5
10
20
Octave band pressure level (dB)
30
40
50
60
70
80
63 125 250 500
Octave band center frequencies (Hz)
1000 2000 4000
PNC-15
PNC-20
PNC-25
PNC-30
PNC-35
PNC-40
PNC-45
PNC-50
PNC-55
PNC-60
PNC-65
8000
The approximate
threshold of hearing
for continuous noise
FIGURE 38.4 1971 preferred noise-criteria curves.
Determine the PNC rating for the octave-band noise spectrum tabulated below.
Center frequency (Hz) 63 125 250 500 1000 2000 4000 8000
Band pressure level (dB) 65 60 60 63 55 50 45 40
Hearing and Psychological Effects 38-7
© 2005 by Taylor & Francis Group, LLC
FIGURE 38.5 Frequency response for the A, B, and C weighting networks.
TABLE 38.1 Sound Level Conversion Chart from Flat
Response to A Weighting
Frequency (Hz) A Weighting (dB)
50 2 30.2
63 2 26.2
80 2 22.5
100 2 19.1
125 2 16.1
160 2 13.4
200 2 10.9
250 2 8.6
315 2 6.6
400 2 4.8
500 2 3.2
630 2 1.9
800 2 0.8
1,000 0
1,250 þ0.6
1,600 þ1.0
2,000 þ1.2
2,500 þ1.3
3,150 þ1.2
4,000 þ1.0
5,000 þ0.5
6,300 2 0.1
8,000 2 1.1
10,000 2 2.5
12,500 2 4.3
16,000 2 6.6
38-8 Vibration and Shock Handbook
© 2005 by Taylor & Francis Group, LLC
In noise-abatement problems, it is often necessary to convert calculated a 1-octave-band or 1/3-
octave-band sound pressure level to a total sound level in dBA. Table 38.1 gives sound level conversion by
A weighting from flat response pressure.
Example 38.5
Determine the total A weight sound level, L; of the set of octave-band sound pressure levels given in
Table 38.2.
Solution
Refer Table 38.1 for the dB conversion from a flat response level, Lflat; for each of the octave bands to a
sound pressure intensity with A weighting IiA; and then the sum of IiA: Finally, the total sound level with
A weighting Ltotal;A is given by
Ltotal;A ¼ 10 log
Xn
i¼1
IiA ¼ 10 log 12:238 £ 106 ¼ 70:9 ðdBÞ
References
1. Irwin, J.D. and Graf, E.R. 1979. Industrial Noise and Vibration Control, Prentice Hall, Englewood
Cliffs, NJ.
2. American National Standard USAS S3.4-1968. 1968. Procedure for the Computation of Loudness of
Noise, America National Standards Institute, New York, NY.
TABLE 38.2 Octave-Band Sound Pressure Levels
fc (Hz) Lflat (dB) DLA (dB) LA ¼ Lflat þ DL (dB) IiA
63 74 2 26.2 47.8 0.60 £ 105
125 71 2 16.1 54.9 3.09
250 61 2 8.6 52.4 1.74
500 60 2 3.2 56.8 6.31
1000 62 0 62.0 1.585 £ 106
2000 60 1.2 61.2 1.318
4000 62 1.0 63.0 1.995
8000 69 2 1.1 67.9 6.166
Sum 12.238 £ 106
Note:
* fc: band center frequency
* Lflat: sound pressure level with flat weighting
* DLA: A-weighting level
* IiA: sound pressure intensity with A weighting.
Hearing and Psychological Effects 38-9
© 2005 by Taylor & Francis Group, LLC
Популярные книги
- Старинные занимательные задачи
- Медоносные растения
- Математика Древнего Китая
- Algebratic geometry
- Workbook in Higher Algebra
- Finite element analysis
- Пчеловодство
- Mathematics and art
- Fields and galois theory
- Black Holes
Популярные статьи
- Higher-Order Finite Element Methods
- Электровакуумные приборы
- Riemann zeta functionS
- Универсальная открытая архитектурно-строительная система зданий серии Б1.020.1-71
- Complex Analysis 2002-2003
- Пример расчета прочности елементов, стыков и узлов несущего каркаса здания
- Составы, вещества и материалы для огнезащитыметаллических консрукций и изделий
- CMOS Technology
- Рекомендации по расчету и конструированию сборных железобетонных колонн каркасов зданий серии Б1.020.1-7 с плоскими стыками ВИНСТ
- Советы старого пчеловода