Real-world attenuation of muff-type hearing protectors: The effect of spectacles

Similar documents
1 White Paper. Intelligibility.

SIA Software Company, Inc.

Introduction to Dynamic Loudspeaker Design

ENHANCEMENT OF THE TRANSMISSION LOSS OF DOUBLE PANELS BY MEANS OF ACTIVELY CONTROLLING THE CAVITY SOUND FIELD

Added sounds for quiet vehicles

Digitally controlled Active Noise Reduction with integrated Speech Communication

Acoustical Active Noise Control

Fastener Hole Crack Detection Using Adjustable Slide Probes

FFT 1 /n octave analysis wavelet

How To... Commission an Installed Sound Environment

The Naim Balanced Mode Radiator The Naim Ovator Bass Driver

Technical Guide. Installed Sound. Recommended Equalization Procedures. TA-6 Version 1.1 April, 2002

Response spectrum Time history Power Spectral Density, PSD

The New Lite-Com II For better safety and effectiveness

DESIGN OF VOICE ALARM SYSTEMS FOR TRAFFIC TUNNELS: OPTIMISATION OF SPEECH INTELLIGIBILITY

MAKE SURE TA & TI STAMPS EVERY PAGE BEFORE YOU START

XLA 3200 Line Array Loudspeakers

Technique for the Derivation of Wide Band Room Impulse Response

Reverberation time and structure loss factor

4: EXPERIMENTS WITH SOUND PULSES

THE ATTENUATION OF NOISE ENTERING BUILDINGS USING QUARTER- WAVE RESONATORS: RESULTS FROM A FULL SCALE PROTOTYPE. C.D.Field and F.R.

What you Need: Exel Acoustic Set with XL2 Analyzer M4260 Measurement Microphone Minirator MR-PRO

Application Note L26ROY

From time to time it is useful even for an expert to give a thought to the basics of sound reproduction. For instance, what the stereo is all about?

Fig 1 Microphone transducer types

Absorbers & Diffusers

When you have completed this exercise, you will be able to determine the frequency response of a

Introduction to Equalization

CHAPTER 5 PRINTED FLARED DIPOLE ANTENNA

A SYSTEM IMPLEMENTATION OF AN ACTIVE NOISE CONTROL SYSTEM COMBINED WITH PASSIVE SILENCERS FOR IMPROVED NOISE REDUCTION IN DUCTS SUMMARY INTRODUCTION

Sound Waves Practice Problems PSI AP Physics 1. (D) It cannot be determined with the given information.

Processor Setting Fundamentals -or- What Is the Crossover Point?

Generic noise criterion curves for sensitive equipment

PRIME FOCUS FEEDS FOR THE COMPACT RANGE

Validation of lateral fraction results in room acoustic measurements

AUDITORY ILLUSIONS & LAB REPORT FORM

The Design & Test of Broadband Launches up to 50 GHz on Thin & Thick Substrates

I INCH-POUND. MI L-STD December 1990 MILI T.4RYSTANDARD PHYSICAL EAR NOISE ATTENUATION TESTING. AMsc ri/.4 FSC HFAC

PanPhonics Panels in Active Control of Sound

Technical Notes Vol. 1, No Volt Distribution Systems Using JBL Industrial Series Loudspeakers

EQ s & Frequency Processing

INTRODUCTION TO ACOUSTIC PHONETICS 2 Hilary Term, week 6 22 February 2006

What applications is a cardioid subwoofer configuration appropriate for?

BIG 3 WAY SPEAKER: INTEGRATION OF BASS AND MIDRANGER DRIVERS. 3D Acoustics Research, January

EXPERIMENTAL INVESTIGATIONS OF DIFFERENT MICROPHONE INSTALLATIONS FOR ACTIVE NOISE CONTROL IN DUCTS

Active Noise Reduction Algorithm Based on NOTCH Filter and Genetic Algorithm

Chapter 5 DESIGN AND IMPLEMENTATION OF SWASTIKA-SHAPED FREQUENCY RECONFIGURABLE ANTENNA ON FR4 SUBSTRATE

NOISE REDUCTION OF A RECIPROCATING COMPRESSOR BY ADDING A RESONATOR IN SUCTION PATH OF REFRIGERANT

RD75, RD50, RD40, RD28.1 Planar magnetic transducers with true line source characteristics

Practical Limitations of Wideband Terminals

Hand Tools MEC072 SAMPLE

SECTION A Waves and Sound

FINAL REPORT. On Project Supplemental Guidance on the Application of FHWA s Traffic Noise Model (TNM) APPENDIX K Parallel Barriers

In situ assessment of the normal incidence sound absorption coefficient of asphalt mixtures with a new impedance tube

WITHIN GENERATOR APPLICATIONS

Assessing the accuracy of directional real-time noise monitoring systems

Design of a Line Array Point Source Loudspeaker System

Attenuation of low frequency underwater noise using arrays of air-filled resonators

Simulation of Cylindrical Resonator with Spiral Neck and Straight Neck to Attenuate the Low Frequency Noise of Muffler

[Q] DEFINE AUDIO AMPLIFIER. STATE ITS TYPE. DRAW ITS FREQUENCY RESPONSE CURVE.

EXPERIMENT 8: SPEED OF SOUND IN AIR

IE-35 & IE-45 RT-60 Manual October, RT 60 Manual. for the IE-35 & IE-45. Copyright 2007 Ivie Technologies Inc. Lehi, UT. Printed in U.S.A.

sound is a longitudinal, mechanical wave that travels as a series of high and low pressure variations

RF300 LARGE LOOP ANTENNA

An audio circuit collection, Part 3

7.2.8 Frequency sensitivity

Experiment-4 Study of the characteristics of the Klystron tube

The Helmholtz Resonance

THE CONVERSION OF AN ATTENUATOR TO PHASE SHIFTER AND THE CALIBRATION OF BOTH

SOUND & RECORDING 04/13 04/13. Test: Neumann KH 310. Near-field monitor NEUMANN KH310 TEST REPORTS SOUND & RECORDING 04/13

Finding the Prototype for Stereo Loudspeakers

ODEON APPLICATION NOTE Calculation of Speech Transmission Index in rooms

SECTION A Waves and Sound

Quarterly Progress and Status Report. A note on the vocal tract wall impedance

New Technique Accurately Measures Low-Frequency Distortion To <-130 dbc Levels by Xavier Ramus, Applications Engineer, Texas Instruments Incorporated


EVEN IF YOU DON T LIKE READING MANUALS PLEASE READ THIS SECTION BEFORE INSTALLING THE PIANOMIC SYSTEM

Lab 12 Microwave Optics.

Development of a reactive silencer for turbocompressors

Investigating Electromagnetic and Acoustic Properties of Loudspeakers Using Phase Sensitive Equipment

A.C. FILTER NETWORKS. Learning Objectives

A Guide to Reading Transducer Specification Sheets

Experiment 1: Instrument Familiarization (8/28/06)

Spring 2004 M2.1. Lab M2. Ultrasound: Interference, Wavelength, and Velocity

Earthworks, Inc. 37 Wilton Rd. Milford, NH , ext Printed in U.S.A.

Exercise 2: Q and Bandwidth of a Series RLC Circuit

6-channel recording/reproduction system for 3-dimensional auralization of sound fields

A CAS Forum Activity Report Looking at Hair Tension as a Design Parameter for Violin Bows

Experiment 1: Instrument Familiarization

USBPRO User Manual. Contents. Cardioid Condenser USB Microphone

IS SII BETTER THAN STI AT RECOGNISING THE EFFECTS OF POOR TONAL BALANCE ON INTELLIGIBILITY?

The Speaker Study. By: Jay Bliefnick. Acoustical Testing 1. Attn: Dr. Dominique Chéenne, Dr. Lauren Ronsse. Group Members:

Minimizing Input Filter Requirements In Military Power Supply Designs

Active Control of Energy Density in a Mock Cabin

In-Ear Monitors using VRT Transducers A market survey

(i) node [1] (ii) antinode...

Acoustical Testing I Loudspeaker Study

Airborne Sound Insulation

Sound absorption of Helmholtz resonator included a winding built-in neck extension

RF Emissions Test Report To Determine Compliance With: FCC, Part 15 Rules and Regulations

Transcription:

Real-world attenuation of muff-type hearing protectors: The effect of spectacles Frank Lemstad and Roald Kluge Sinus as, Sandvigå 24 N-7 Stavanger, Norway frank.lemstad@sinusas.no ABSTRACT A study has been carried out to investigate how much spectacles influence the attenuation of ear muffs. Measurements have been performed using broad-band stationary noise on real persons with four different safety spectacles. It is concluded that spectacles introduce a very significant reduction in the attenuation. Depending on the spectacle and person, the effect can be from moderate to severe. Particularly important is the reduction at low frequencies (1- Hz). This is due to the side bars introducing a leakage that makes the ear muff act as a kind of Helmholtz resonator with a frequency -300 Hz (depending on muff volume). However, also at 3-5 khz the opening seem to produce a resonance which for some spectacles and persons can reduce the attenuation significantly. The spectacle effect varies a lot from person to person and spectacle to spectacle. However, it is very consistent over the three different Peltor muff models tested. For optimum attenuation a good fit and thin side bars (particularly small width) is essential. Unfortunately, many safety spectacles have rather thick bars which may produce almost disastrously poor muff attenuation even with the very best muffs available. 1. INTRODUCTION It is well known from several studies that label data (obtained from laboratory measurements) of hearing protection devices (HPD) overestimate the attenuation that can be expected under real world conditions. An extensive field study by Giardino&Durkt [1] investigated a total of 7 HPDs on workers in the mining industriy. When comparing field results with laboratory data, the main observations were as follows: The average noise attenuation in the field is considerably lower The spread in the field is considerably larger (typically 4-8 db rather than the 2-3 db obtained in laboratory data) Combined, this means that some people get very low practical attenuation values. Thus, Giardino and Durkt observe that 32% of those in the study operating diesel engines had a practical noise attenuation of less than 10 dba. For 8% the reduction was less than 5 dba. BNAM4-1

The reasons for the difference between field and lab results are probably several. European Standard pren458 lists the following main factors: Poor fitting Long hair Wearing of spectacles or other PPE (Personal Protection Equipment) A particular concern, to be discussed here, is the use of spectacles, particularly safety glasses. Having rather thick frames, they tend to introduce a significant leakage which quite obviously will contribute to reduced attenuation. Despite the fact that safety glasses are mandatory in many high-noise environments, little reliable data exist on how they affect the noise attenuation of ear muffs. 2. METHOD AND EXTENT OF STUDY 2.1. Spectacles Measurements have been made on four types of spectacles (safety glasses). The spectacles are somewhat arbitrary chosen, but should present a fairly representative variation in terms of appearance and spectacle thickness. Type 1 and 2 have rather thin side bars, type 3 and 4 are thicker. Figure 1. Spectacle No. 2, Bollé Boaci (left), no. 4 Millennia 9 (right). 2.2. Muffs (hearing protector models) The tests were made on three Peltor models: 1. Peltor H9 a light-weight type 2. Peltor H520 (Optime II) a medium type 3. Peltor H540 (Optime III) heavy type, designed for maximum noise protection Only one sample (both muffs) of each protector was used. All were in very good condition (2 and 3 were actually brand new). All protectors were of the headband type, see Figure 2. BNAM4-2

Figure 2. Left: light-weight hearing protector similar to HP1. Right: HP3, the new state-of-the-art Peltor H540 2.3. Test persons Six real persons were used for the test, four males and two females. Both females had long hair. The test persons represent a fairly wide range in head shape ( narrow to round ) and size (55-61). Most test persons were familiar with using HPDs. They put the muffs on themselves without assistance from the test leader. The test persons were sitting in a chair and not moving during each measurement. 2.4. Equipment and method 1/3-octave Leq levels were measured using a Brüel&Kjær 4182 probe microphone, see figure 3. A flexible probe tube - fastened to the ear of each test person with tape - was chosen to avoid variations in positioning between measurements. The microphone has somewhat limited dynamic range. This turned out to be of importance at frequencies above -0 Hz. The dynamic limitation is probably due to the part of the tube outside the cup picking up extranous noise. For each test person, measurements were made Without HPD With HPD but no spectacle With HPD and spectacle The noise was produced using a Norsonic 811L loudspeaker in a small rather reverberant room with pink noise input. Total A-weighted level outside the cup was about 95 dba. The direct sound had an angle of incidence of about 30 degrees from ear-ear axis. BNAM4-3

Figure 3. Left: Happy author and test person with BK 4182 probe microphone, silk scarf (borrowed from the secretary!) and spectacle no. 4. Right: The BK 4182. 3. PRESENTATION OF MEASUREMENT RESULTS 3.1. Average attenuation Figure 4 presents the the average attenuation (db-average for all test persons) for HP1 and HP3. The following situations are shown: No spectacle laboratory data (large disks and no lines, octave band only) No spectacle (upper curve) Spectacle no. 1-4 The lab data presented throughout in this report is the manufacturer s stated assumed protection values (APV), which is the lab average minus one standard deviation. For our field data, however, no deduction has been made. In general, the results for protector HP2 turn out to be very similar to HP1 (although marginally better). Thus to save space, these data have for the most part been omitted. BNAM4-4

HP1 - Average attenuation, all test persons 4 35,0 3 25,0 2 15,0 1 5,0 Hz -5,0-1 2 0 0 0 2 0 None No. 1 No. 2 No. 3 No. 4 Label 45,0 HP3 - Average attenuation 4 35,0 3 25,0 2 15,0 1 5,0-5,0 2 0 0 0 2 0 None No. 1 No. 2 No. 3 No. 4 Label Figure 4. Average attenuation values for protector HP1 (top) and HP3 (bottom). BNAM4-5

3.2. Reduction in attenuation spectacle effect Figure 5 presents the average reduction in attenuation for each hearing protector and spectacle. 2,0-2,0-4,0-6,0-8,0-1 -12,0-14,0 HP1 - Relative reduction in attenuation 2 0 0 0 2 Diff 1 Diff 2 Diff 3 Diff 4 0 2,0 HP3 - Relative reduction in attenuation -2,0-4,0-6,0-8,0-1 -12,0-14,0 2 0 0 0 2 0 Diff 1 Diff 2 Diff 3 Diff 4 Figure 5. Average reduction in attenuation values due to spectacles for protector HP1 and HP3. 3.3. Spread variation between test persons There is a large spread in attenuation values between the test persons. Figure 6 shows the standard deviation obtained with hearing protector HP1 for the various spectacle alternatives. BNAM4-6

Figure 7 shows the attenuation values for each test person using HP1 and the poorly performing spectacle no. 4. 8,0 6,0 HP1 - Standard deviation, all 4,0 2,0 2 0 0 0 2 0 None No. 1 No. 2 No. 3 No. 4 Label Figure 6. Standard deviation in average attenuation values for HP1. HP1 - Spectacle no. 4 - Attenuation for each person 3 25,0 2 15,0 1 5,0-5,0-1 2 0 0 0 2 0 Frank Henning Tønnes Magnus Inger Anne Serine Hz 00 Figure 7. Attenuation for hearing protector HP1 for each person using spectacle no. 4. 3.4. System limitation attenuation without spectacle Figure 8 shows the attenuation for each test person - of HP3 without spectacle. Label data are shown for comparison. This measurement, made on the best protector (HP3), gives information about the the dynamic capability of the measurement chain as well as individual variability. BNAM4-7

4 HP3 - No spectacle - Attenuation, individual 35,0 3 25,0 2 15,0 1 5,0 2 0 0 0 2 0 Frank Henning Tønnes Magnus Inger Anne Serine Label Figure 8. Attenuation without spectacle, HP3, indicating insufficient dynamic range of measurement chain above Hz. 3.5. Effect of hair (?) male/female difference Figure 9 shows the difference in average attenuation, for each protector, between the females (2 persons) and males (4 persons). It is believed a major reason for the generally lower attenuation values of the females is long hair. If so, the hair effect is to reduce attenuation over a broad range (at least below Hz but probably even higher), as particularly evident on the HP3. Also, there is a very pronounced cutoff at 5 khz for all protectors. Difference in average attenuation, no spectacle, women-men -1,0-2,0-3,0-4,0-5,0-6,0-7,0-8,0-9,0-1 -11,0 H1 H2 H3 2 0 0 0 2 Figure 9. Difference in attenuation between females and males. BNAM4-8

3.6. Effect of head shape (?) an indication The two males with the biggest difference in attenuation were person H and M. Their results for HP3 are presented in Figure 10. In particular, the performance of spectacle 4 on M is poor. 4 HP3 - Attenuation, person "H" 35,0 3 25,0 2 15,0 1 5,0-5,0 2 0 0 0 2 0 None No. 1 No. 2 No. 3 No. 4 Label HP3 - Attenuation, person "M" 4 35,0 3 25,0 2 15,0 1 5,0-5,0-1 None No. 1 No. 2 No. 3 No. 4 Label 0 0 0 Figure 10. Attenuation for the two short-haired people with the overall best ( H, top) and worst ( M, bottom) results. BNAM4-9

4. EVALUATION AND DISCUSSION OF MEASUREMENT RESULTS 4.1. System limitation - consequences The measurement chain itself is believed to have sufficient dynamics and accuracy up to about Hz for all protectors. From -0 Hz onwards, however, the dynamic range is generally not sufficient to measure the real attenuation correctly for the better combinations of protector, spectacle and person (!). The effect of this is that the data become somewhat blurred and the full spectacle effect is not revealed. Still, interesting effects of the poorer spectacles can be observed at the higher frequency end, particularly at 4-5 khz. 4.2. Measured attenuation without spectacles The attenuation values in db at some selected frequencies are summarized in the table below. Protector Lab/field Hz 2 Hz Hz HP1 Lab (APV) Field 8 2 12 12 24 24 HP2 Lab (APV) Field 13 4 18 16 30 27 HP3 Lab (APV) Field 15 12 22 22 33 33 Without spectacles, then, the average attenuation values at 2 and Hz correspond well with laboratory data. At Hz, however, HP1 and HP2 fail to produce the promised attenuation. 4.3. Spectacle effect(s) As expected, spectacles reduce the average attenuation for all protectors. The effect varies from moderate to severe. In general spectacle no. 2 produce the best results on all persons, whereas spectacle 3 and 4 are poor. The difference plots for each protector have basically the same shape. For spectacle no. 3 and 4 there are two very obvious dips (see Figure 5) at the following frequencies: Protector Frequency 1 Frequency 2 HP1 [Hz] HP2 2 - [Hz] HP3 - [Hz] The individual variation is very large, particularly for spectacle no. 3 and 4. Standard deviations run up 6-8 db. For some combinations of spectacles and persons, a negative attenuation (i.e. amplification) is observed at - 300 Hz. Other persons retain a significant positive attenuation with all spectacles. BNAM4-10

Subtracting the standard deviation from the average attenuation (over all persons) give the attenuation values in Table 4.3. From these values, the following tentative observations are made: With spectacles, no positive attenuation can be assumed from any protector below Hz. With HP1 and HP2 there is practically no attenuation at 2 Hz with spectacles 1, 3 and 4. With spectacle no. 2, however, the attenuation is 7-8 db. Even at 4 khz spectacle 3 and 4 produce significantly poorer attenuation. Table 4.3-1. Average attenuation values for HP1 (minus one standard deviation) Spectacle Lab/field Hz 2 Hz Hz Hz None APV (Avr. SD) 1 10 20 > 20 No. 1 APV (Avr. SD) -3 0 13 > 20 No. 2 APV (Avr. SD) -2 7 17 > 20 No. 3 APV (Avr. SD) -4-4 10 13 No. 4 APV (Avr. SD) -3-4 11 12 Table 4.3-2. Average attenuation values for HP2 (minus one standard deviation) Spectacle Lab/field Hz 2 Hz Hz None APV (Avr. SD) 2 11 21 > 20 No. 1 APV (Avr. SD) -3 3 15 > 20 No. 2 APV (Avr. SD) -2 8 18 > 20 No. 3 APV (Avr. SD) -5-1 13 15 No. 4 APV (Avr. SD) -5-1 14 14 Table 4.3-3. Average attenuation values for HP3 (minus one standard deviation) Spectacle Lab/field Hz 2 Hz Hz None APV (Avr. SD) 7 18 28 > 25 No. 1 APV (Avr. SD) -2 8 20 > 25 No. 2 APV (Avr. SD) 3 13 23 > 25 No. 3 APV (Avr. SD) -5 3 18 19 No. 4 APV (Avr. SD) -4 2 17 18 The large individual variations suggest that head shape is important, particularly the area close to the ears. A round head shape is preferable and a bigger head may be better than a small. Spectacle no. 4, which shows the largest variation between persons, is very stiff and does not adapt well to different head shapes sideways. In addition to a good fit, the side bars should be thin. In particular, we believe the width to be important. The width of the spectacles used in the studty at crossover are approximately: 3 mm (no. 1), 2 mm (no. 2), 5-6 mm (no. 3) and 4 mm (no. 4).The best results are obtained with the spectacle with the narrowest bar. BNAM4-11

5. PHYSICAL EXPLANATIONS 5.1. Low-frequency dip is Helmholtz resonator Spectacles seem to significantly reduce the attenuation of ear muffs at - Hz and 3-6 khz. We believe the reduction at - Hz can be explained essentially as an Helmholtz resonator effect. The spectacle makes an opening into the otherwise enclosed muff volume. The resonance frequency of a Helmholtz resonator can be written where C 0 S f0 = 2p Vd (0.1) C 0 is the velocity of sound, S is the duct area, D is tube length and V is the cavity volume Measurements made on spectacle 4 with protector HP3 suggests 2 S = 2h (0.2) where h is the width (horizontal dimension) of the spectacle bar. The tube length d 30-40 mm. Actually, the spectacle produce two tubes, one on the upper side and one on the lower, the upper being slightly longer and thus giving a lower resonance. Each duct has an approximately triangle-shaped cross section. For spectacle 4 t his all gives f 0 220 Hz. This fits well with the measurements. The larger the muff volume, the lower the resonance frequency (other factors equal). This is also in good accordance with the measurement results, as HP1 has a resonance at 300 Hz, HP2 at 2 Hz and HP3 at about Hz. 5.2. High-frequency dip The reason for the high-frequency dip is less obvious than the low-frequency one. We suggest the 3-5 khz dip is due to a resonance related to transmission through narrow, long tubes. The effect is here only described quantitatively. In such tubes, i.e. being much longer than they are wide, and with diameter much smaller than the wavelength of sound, the air will act as a piston (moving mass). There will be an internal resonance when the wavelength is approximately twice the tube length. At this frequency, the transmission through the tube will be very efficient, hence giving a leakage. For the hearing protector seals, the tube length(s) produced by the spectacle bar will be approximately 35- mm on the upper side (and 30-40 mm on the lower side) depending on the sealing width and the crossover point. This can produce a dip in the frequency area 3.4 5.7 khz. BNAM4-12

6. CONCLUSIONS Safety spectacles have been shown to significantly reduce the typical attenuation obtained with ear-muff type hearing protectors. With spectacles having thin side bars (2-3 mm) and a generally good fit to the head, the reduction can be kept at a moderate level. However, of four spectacles tested, two performed poorly on most test persons. These types are also told to be popular. Spectacles in particular reduce the attenuation at low frequencies by introducing a leakage that create a Helmholtz resonator effect. The resonance frequency is in the -300 Hz range (depending on muff volume) but the attenuation is reduced in a much broader frequency range. At resonance, the attenuation can be negative (i.e. the muff acts as an amplifier) if the spectacle side bars are thick and/or the fitting is poor. If optimum noise protection is to be achieved in combination with safety spectacles, as much emphasis must be put on the choice of spectacles as on muffs. The spectacles should fit the individual well and have thin side bars (particularly the width is believed to be important). Further, it seems the side bars ought to curve downwards behind the ear (like normal spectacles), not be straight. Even well-fitting spectacles with thin bars will reduce the noise attenuation of ear muffs. The effect of this must be taken into consideration in hearing protection programmes so that sufficient margins are allowed. In very high-noise environments, alternatives may be to use double protection (i.e. ear plugs in addition to muffs). Helmets with integrated eye protection also exist, possibly avoiding the need for side bars crossing the muff seal altogether. 7. ACKNOWLEDGEMENTS The authors wish to thank Anne Serine Ognedal for carrying out the practical measurements and assist in the data collection. 8. REFERENCES [1] Dennis A. Giardino / George Durkt jr.: Evaluation of muff-type hearing protectors as used in a working environment, AIHA Journal (57), march 1996. BNAM4-13