Signals, systems, acoustics and the ear. Week 1. Laboratory session: Measuring thresholds

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Transcription:

Signals, systems, acoustics and the ear Week 1 Laboratory session: Measuring thresholds

What s the most commonly used piece of electronic equipment in the audiological clinic? The Audiometer

And what is its purpose? To determine the lowest intensity sounds that people can hear (for pure tones as a function of their frequency)

The minimalist audiometer needs An oscillator to generate an electrical sinusoidal wave at the desired frequencies A calibrated volume control to adjust the intensity of the sound A headphone to convert the electrical wave to an acoustic one, so it can be presented to the listener

The minimal audiometer change amplitude (2 ways) change frequency

What comes out of the oscillator? Electrical wave (to be graphed as a waveform) A graph of the instantaneous value of the voltage (or current), across time Crucial for every waveform x-axis is always time (s, ms, μs) y-axis always a linear instantaneous amplitude measure (V, mv, μv) But oscillators usually give a very special waveform, a sinusoid, also known as a pure tone (at least in reference to sounds)

An electrical sinusoidal waveform from an oscillator displacement (mm) voltage (V) 1.5 1 0.5 0-0.5-1 -1.5 0 0.002 0.004 0.006 0.008 0.01 time (s) 2 ms 4 ms 6 ms 8 ms 10 ms time

Transducing an electrical wave to an acoustic one We cannot hear an electrical wave directly, so need to convert it by feeding to the headphones which transduce the variations in the electrical wave to a mechanical wave the changes in voltage cause the headphone diaphragm to vibrate, which makes the sound

Just like a miniature loudspeaker http://electronics.howstuffworks.com/speaker5.htm

Movement of the headphone diaphragm displacement (mm) displacement (mm) 1.5 1 0.5 0-0.5-1 -1.5 0 0.002 0.004 0.006 0.008 0.01 time (s)

Sound pressure fluctuations in the air pressure (pascals Pa) displacement (mm) 1.5 1 0.5 0-0.5-1 -1.5 0 0.002 0.004 0.006 0.008 0.01 time (s) Look at the units on the y-axis

Today s laboratory: Measure thresholds with a simple audiometer

Measuring thresholds I Set oscillator to desired frequency and attenuator to 0 (maximum level) Present a tone for about 1 s by pressing the button The patient indicates having heard the tone by raising a finger

Measuring thresholds II If heard, decrease level by 10 db (2 clicks clockwise) If not heard, increase level by 5 db (1 click counter-clockwise) Present tone Repeat steps above to find lowest level at which the patient hears the tone on 2 of 2, 3 or 4 tries on the ascent (at least 50%) Do all the frequencies specified

Adjust frequency with these buttons and dial Observe! Do not touch these buttons

Adjust level with this dial Observe! What do you need to know in order to know what threshold a person has (in db SPL)?

Things you need to know Keep the data from any lab you do. You will need some of it to do your exercise sets. Today: 4 set-ups available in sound-proof rooms (work in pairs ) Once you have your thresholds as attenuation values, come back to the lab (do not do your calculations in the cubicles). Ensure you write down the calibrated values from the particular set of equipment you used. Do the lab Explore signals while you are not doing audiometry. We will do the calculations later.

Laboratory session: Measuring thresholds Part 2

db SPL examples: a reminder Threshold of Hearing (20 µpa) 20 log 10 (20 µpa/20 µpa) = 20 log 10 (1) = 20 0 = 0 db SPL Threshold of Pain (200 Pa) 20 log 10 (200 Pa/20 µpa) = 20 log 10 (10000000) = 20 7 = 140 db SPL An inaudible sound (2 µpa) 20 log 10 (2 µpa /20 µpa) = 20 log 10 (0.1) = 20-1 = -20 db SPL

db SPL: working backwards db SPL Pa If threshold of hearing for a 125 Hz sinusoid is 30 db SPL, how many Pa is this? 30 db SPL = 20 log 10 (θ µpa/20 µpa) 30/20 = log 10 (θ µpa /20 µpa) Note: 10 log10 (θ) = θ e.g., 10 log10 (100) = 10 log10 (102 ) = 10 2 = 100 10 30/20 = (θ µpa /20 µpa) 20 x 10 30/20 = θ 20 x 10 30/20 = 20 x 10 1.5 = 20 x 31.62 = 632.5 µpa More generally λ db SPL = 20 log 10 (θ µpa /20 µpa) λ /20 = log 10 (θ µpa /20 µpa) 10 λ/20 = (θ µpa /20 µpa) 20 x 10 λ/20 = θ µpa

Measuring hearing loss Poorer hearing leads to higher thresholds Someone with a hearing loss would have higher thresholds Here, for example, the loss is small at low frequencies and great at high (a typical pattern) We re interested in differences to normal thresholds

Displaying a threshold curve in a clinically relevant way the audiogram For clinical purposes, it s easier to judge deviations from normality. Use db Hearing Level (HL) instead of db SPL To calculate a person s Hearing Level... Find the absolute threshold in db SPL. Subtract the normal value of the absolute threshold (again in db SPL)... And plot increasing positive values downward (higher thresholds = more hearing loss = points further down the page).

Example audiograms normal hearing impaired hearing db HL = actual threshold (db SPL) normal threshold (db SPL) From the China Rehabilitation Research Center for Deaf Children, Beijing.

Constructing an audiogram (converting db SPL to db HL) 250 Hz 500 Hz 1 khz 2 khz 4 khz 8 khz patient SPL 30 38 42 60 73 92 normal SPL 20 10 8 4 0 20 patient HL 10 28 34 56 73 72 db HL

db SPL vs. db HL for sinusoids db SPL = 20 x log 10 (p/20 µpa) the same reference level for every frequency db HL = 20 x log 10 (p/θ µpa) where θ µpa is the normal absolute threshold for that particular frequency so reference level typically is different for every frequency

An example of db HL Normal threshold of hearing at 125 Hz = 632.5 µpa) Suppose someone s threshold is 356 µpa, then 20 log 10 (356 µpa/632.5 µpa) = -5 db HL So db HL just has a different reference level than db SPL But also note 20 log 10 ( 356 µpa /20 µpa) = 25 db SPL 20 log 10 ( 632.5 µpa /20 µpa) = 30 db SPL So, you can also obtain db HL by subtracting the normal threshold from the obtained one: 25 db SPL - 30 db SPL = -5 db HL

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