06_physical_agents_1_noise_and_vibration_20140108083824 Flashcards
wavelength
The wavelength (λ) determines the pitch of the sound. Wavelength is the length of one complete cycle, and is measured in metres (m). Its relationship to the frequency and speed of sound can be expressed as: Wavelength (λ) in metres = Speed of sound (c) / Frequency (f) Long, slow waves are a low pitch (like a fog horn). Short, fast waves are a high pitch (like a whistle).
Frequency
Frequency (F) is the number of times a complete wave passes a point. It is measured in hertz (Hz), or cycles per second. The slowest, lowest sound a human can hear is approximately 20 Hz. The highest sound a human can hear is approximately 20,000 Hz (or 20 kilohertz - kHz).
period
The period (T) is the time it takes to complete one full cycle, it is proportional to the frequency - T = 1/f (seconds).
A-weighting:
Reduces the importance of lower frequencies at 500 Hz or less. The lower the frequency, the greater the A-weighted correction factor becomes (see Figure 6.4). Slightly increases the overall magnitude of the mid to high frequencies (2,000-4,000 Hz). Reduces the very high frequencies as they extend beyond normal hearing.
C-weighting:
Used principally for the evaluation of impulse noise and for hearing protection. It was originally intended to be used when measuring high sound pressure levels such as aircraft noise. C-weighted correction values show significantly less low frequency roll-off relative to the A-weighted correction values.
The strength or loudness of a sound is determined by
the amplitude or height of the sound waves. Tall waves are loud; short waves are quiet.
Amplitude is a convenient measure of the magnitude of the sound and can be related to its intensity and loudness and ultimately the effect it has on the human ear. There are various options for determining the amplitude: 3
The peak value does not relate closely to the subjective impression of the sound. An average value may be more appropriate but due to the symmetrical shape of the pressure wave positive sides of the wave ‘cancel out’ the negative and the resultant ‘average’ is zero. The measure which best takes into account the magnitude of the sound pressure fluctuations, but not the direction, is the root-mean square (or RMS) sound pressure.
Sound power (PWL)
Sound power is the total sound energy generated by the source per unit of time expressed in units of watts (W). The sound power of a source output is constant, regardless of its location although, as will be shown, the sound intensity and sound pressure will change as a function of the environment in which it is located.
Sound intensity
Sound intensity is sound power per unit area (W/m2). It is a vector quantity, i.e. is specified by direction. Note: Sound intensity is proportional to sound pressure squared.
Sound pressure (SPL)
The sound pressure level (SPL) is the variation of pressure superimposed on the atmospheric pressure. Sound pressure is expressed as force per unit area, and the preferred unit is the Pascal (Pa) (or Newton per square meter N/m2). When measured in sound pressure the hearing scale runs from 20μPa (20 × 10−6Pa) at the threshold of hearing to 200 Pa (200 000 000 μPa) at the threshold of pain. Note: compared to static air pressure (101.325 kPa – often approximated to 105 Pa) these variations are very small. Sound pressure is the ‘effect’ of a disturbance (what is heard). The actual ‘cause’ of the disturbance, and the resulting reaction effect, is due to the sound power. The sound pressure equates to the sound power plus a constant (k) which is dependent upon the acoustics of the environment, the directivity of the sound and the distance from the source.
Rules of the decibel scale 2
10dB expresses a 10 times increase in sound intensity but, to the subjective listener, seems about twice as loud, i.e. it would take ten violins to sound twice as loud as one violin. 3dB expresses a doubling in sound intensity (i.e. If one machine gave a sound pressure level of 75 dB two identical machines would give a reading of 78 dB) although this would give rise to a just noticeable change.
LEPd
daily personal noise exposure
Leq
To determine the average dose received over a given time, an integrated sound level meter balances out the peaks and troughs to calculate a single figure that would give the equivalent dose over that time. This equivalent level is known as an Leq
Noise exposure levels equivalent to 80dB(A)LEPd (the lower exposure action value – see Table 6.5), can be calculated using the ‘rule of three’.
80dB(A) over 8 hours is the same noise dose as 83dB(A) over 4 hours. Double the noise level (increase by 3dB) over half the time gives the same dose.
For sound to travel through the ear, four different types of energy are required:
Acoustical energy or sound waves set the tympanic membrane into vibration synchronous to the sound pressure compression and rarefaction cycles. Mechanical energy as the vibration is transmitted by the movement of the eardrum and the ossicular chain. A travelling wave, through the scala tympani as the oval window is pushed in, by the piston-like motion of the stapes footplate. Biochemical energy that sends an electrical signal along the cochlear nerve to the auditory cortex for interpretation as sound.
Health effects of noise Hearing loss may be
conductive, sensorineural, or mixed
Conductive hearing loss
Conductive hearing loss occurs when the sound pathway is blocked in the outer and/or middle ear, reducing the vibration that reaches the inner ear. Conductive hearing loss is diagnosed when bone conduction hearing thresholds are better than air conduction thresholds.
Sensorineural hearing loss
Sensory hearing loss is specific to the cochlea and neural hearing loss is due to pathology within the auditory nerve and/or central auditory pathway. The term sensorineural hearing loss is used to cover both a specific diagnosis is difficult without sophisticated diagnostic equipment. Sensorineural hearing loss is less likely to be medically treatable and more likely to be permanent than conductive hearing loss. Sensorineural hearing loss can be caused by medications or environmental exposure to certain chemicals. More relevant examples of sensorineural hearing loss are: Prebyacusis – or age-related hearing loss (ARHL) Noise-induced hearing loss (NIHL).
A temporary threshold shift (TTS) is
a hearing loss which shows some recovery within 24-48 hours after the noise exposure stops. The more intense (louder/longer) the exposure, the longer the expected recovery period would be.
permanent threshold shift (PTS)
Hearing loss which persists more than 30 days after the noise exposure is considered to be permanent threshold shift (PTS) and recovery is unlikely.
Where the health surveillance identifies hearing damage the employer shall ensure that the employee is examined by a doctor. If the doctor considers that the damage is likely to be the result of exposure to noise, the employer shall:
a) ensure that a suitably qualified person informs the employee b) review the risk assessment c) review control measures d) consider assigning the employee to alternative work where there is no risk from further noise exposure e) ensure continued health surveillance and a health for any other employee who has been similarly exposed.
Interpreting the audiogram
Frequency (Hz) is plotted from low to high pitch along the x axis (horizontal). Intensity (dB HL) is plotted from soft to loud along the y axis (vertical). Air conducting thresholds are indicated by an ‘X’ for the left ear and an ‘O’ for the right ear. Noise induced hearing loss typically presents with a classic ‘notch’ at around 4kHz.
Test Probable noise level A risk assessment will be needed if the noise is like this for more than:
The noise is intrusive but normal conversation is possible 80dB 6 hours You have to shout to talk to someone 2 m away 85dB 2 hours You have to shout to talk to someone 1 m away 90dB 45 minutes