Week 2 Systems (& a bit more about db)

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AUDL Signals & Systems for Speech & Hearing Reminder: signals as waveforms A graph of the instantaneousvalue of amplitude over time x-axis is always time (s, ms, µs) y-axis always a linear instantaneousamplitude measure (Pa, mpa, µpa, V, m) Week Systems (& a bit more about db) http://www.phon.ucl.ac.uk/courses/spsci/sigsys with links to related material displacement (mm) Pressure (Pa).5.5 -.5 - -.5..4.6.8. time (s) Waveforms are of two major types: periodic and aperiodic Waveforms are of two major types: periodic and aperiodic Periodic waveforms Consist of a basic unit or cycle that repeats in time typically have a strong pitch and also come in two types Aperiodic waveforms do not repeat and also come in two types (but the distinction is not so important as for periodic waves) simple (= sinusoid) complex transient continuous (can be random).8.6.4..5..5. -. -.4.8.6.4..5..5. -. -.4.8.6.4..5..5. -. -.4.8.6.4..5..5. -. -.4 -.6 -.6 -.6 -.6 -.8 - Time (Seconds) -.8 - Time (Seconds) 3 -.8 - Time (Seconds) -.8 - Time (Seconds) 4

A variety of waveforms What is a system? Something which performs an operation on, or transformation of, a signal Concentrate on systems with one input and one output Many useful examples in hearing and speech science.5.5.5.5 amplitude (V).5 5 5 5 3 -.5 - -.5 - input x amplifier output amplitude (V).5 5 5 5 3 -.5 - -.5-5 -.5 time (ms) -.5 time (ms) 6 System = vocal tract input = sound from vibrating vocal folds output = sound emanating from the mouth A microphone (a special name for this kind of system?) hard heed who d output = electrical wave (variations in voltage) Different vocal tract shapes make different vowel sounds from the same input sound 7 input = sound wave (variations in pressure) 8

In-The-Ear Hearing Aid input = sound wave (variations in pressure) Compare sounds as received by a microphone at a position corresponding to the centre of the listener s head, to that at the entrance to ear canal System = head + pinna output = sound wave (modified in some way) 9 Compare sounds at entrance to and at bottom of ear canal System = body + head + pinna + ear canal System = ear canal input = sound from a particular place in space output = sound at the eardrum

System = middle ear Compare movement of ear drum to the movement of the stapes 3 The problem We want to be able to predict what a system will do to a wide variety of signals, without having to try each one. For example, speech from different people through a hearing aid No solution for all possible systems. It is possible for a group of very special systems, known as linear time-invariant (LTI) systems. Amazing fact: For an LTI system, you only need to know what the system does to sine waves in order to predict the effect it will have on anysignal. Linearity = homogeneity + additivity 4 Linearity in a system: Homogeneity Homogeneity for a particular pair of input and output signals, any change in the size of the input signal is matched by the same change in the size of the output If inp(t) outp(t) Then k inp(t) k outp(t) In other words Doubling the size of the input signal doubles the size of the output signal Halving the size of the input signal halves the size of the output signal Nothing is implied about the relationship between the input and output waveforms! 5 A typical test of homogeneity Present a sinewave of a particular frequency to a system (but it can be anyfixed sound) Measure the level of the output signal as you vary the level of the input signal Plot the level of the output signal on the y-axis and the level of the input signal on the x-axis input/output function If the input/output function is a straight line going through the origin (,), that behaviour is consistent with homogeneity Any other kind of curve means the system is not homogeneous and hence, cannot be linear. Would our perfect x amplifier be homogeneous? 6

An input/output function for a x amplifier Homogeneity in the cat middle ear Guinan & Peak: middle ear in cat voltage out.8.6.4..8.6.4...4.6.8 stapes movement (µm rms) 4 3 34 db SPL! 5 5 pressure at ear drum (Pa rms) voltage in 7 Would homogeneity hold at high levels? 8 Laser Doppler Velocimetry of the human eardrum 9 Dalhoff et al. (7) PNAS 4, 546-55

Basilar membrane motion to two sinusoids of different frequency Laser Doppler Velocimetry on the basilar membrane Homogeneity in the monkey inner ear? http://www.wadalab.mech.tohoku.ac.jp/bmldv-e.html 3 basilar membrane movement (µm).5..5..5 Rhode: basilar membrane in monkey...3.4.5 pressure at ear drum (Pa) 4

Adding Waveforms Linearity Part II: Additivity But first, what does it mean to add two waves? 4 Hz ½ V -. Time (s) Hz V 5 -. Time (s) 6 Adding Waveforms Linearity in a system: Additivity sinusoids complex waveform -. Time (s).5 Additivity (principle of superposition) The output of a system to two input signals added together, is the same as the separate output signals for each of the inputs on their own, added together. In other words, signals don t interact. In simple equations: If inp (t) outp (t) & inp (t) outp (t) Then inp (t)+ inp (t) outp (t) + outp (t) -.5. Time (s) 7 8

Additivity: A simple example.5.5 Requirement 3: Time-invariance.5.5 5 5 5 3.5.5.5 + 5 5 5 3 +.5.5.5 5 5 5 3.5.5.5 5 5 5 3.5 For a particular pair of input and output signals, delaying the input signal by a particular amount also delays the output signal by the same amount. The system s behavior does not change in time.5.5.5.5 5 5 5 3 5 5 5 3 9 3.5.5.5 Time invariance: A simple example 5 5 5 3.5.5.5.5.5.5 5 5 5 3.5.5.5 Next week: We show how an LTI system can be completely characterised by its response to sinusoids 5 5 5 3 5 5 5 3 3 3

Today s laboratory: Measure thresholds with a simple audiometer A little more about db 33 db SPL examples: a reminder Threshold of Hearing ( µpa) log ( µpa/ µpa) = log () = = db SPL Threshold of Pain ( Pa) log ( Pa/ µpa) = log () = 7 = 4 db SPL An inaudible sound ( µpa) log ( µpa/ µpa) = log (.) = - = - db SPL 34 db SPL: working backwards db SPL Pa If threshold of hearing for a 5 Hz sinusoid is 3 db SPL, how many Pa is this? 3 db SPL = log (θµpa/ µpa) 3/ = log (θµpa/ µpa) Note: log (θ) = θ e.g., log () = log ( ) = = 3/ = (θµpa/ µpa) x 3/ = θ x 3/ = x.5 = x 3.6 = 63.5 µpa More generally λdb SPL = log (θµpa/ µpa) λ/ = log (θµpa/ µpa) λ/ = (θµpa/ µpa) x λ/ = θµpa 35 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 differencesto normal thresholds

Displaying a threshold curve in a clinically relevant way the audiogram Example audiograms 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). 37 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) 5 Hz 5 Hz khz khz 4 khz 8 khz patient SPL 3 38 4 6 73 9 normal SPL 8 4 patient HL 8 34 56 73 7 db HL db SPL vs. db HL for sinusoids db SPL = x log (p/ µpa) the same reference level for every frequency db HL = x log (p/θµpa) where θµpa is the normal absolute threshold for that particular frequency so reference level typically is different for every frequency 39 4

An example of db HL Normal threshold of hearing at 5 Hz = 63.5 µpa) Suppose someone s threshold is 356 µpa, then log (356 µpa/63.5 µpa) = -5 db HL So db HL just has a different reference level than db SPL But also note log ( 356 µpa/ µpa) = 5 db SPL log ( 63.5 µpa/ µpa) = 3 db SPL So, you can also obtain db HL by subtracting the normal threshold from the obtained one: 5 db SPL -3 db SPL = -5 db HL 4 Today s laboratory: Measure thresholds with a simple audiometer 4 Measuring thresholds I Set oscillator to desired frequency and attenuator to (maximum level) Present a tone for about s by pressing the button The patient indicates having heard the tone by raising a finger Measuring thresholds II If heard, decrease level by db ( clicks clockwise) If not heard, increase level by 5 db ( click counter-clockwise) Present tone Repeat steps above to find lowest level at which the patient hears the tone on of, 3 or 4 tries on the ascent (at least 5%) Do all the frequencies specified 43 44

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)? 45 46 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: 6 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. Finish Explore signals (lab sheet from last week) while you are not doing the lab. 47