| Term 
 | Definition 
 
        | Propagation of a PRESSURE WAVE (not molecule) in space and time through a medium with compressible molecules |  | 
        |  | 
        
        | Term 
 
        | How do elasticity and mass effect displacement? |  | Definition 
 
        | elastic objects increasingly oppose displacement the further they move from their resting position F=kx
 
 object with mass increasingly oppose acceleration the further they move from their resting position (due to inertia)
 P=mv
 (p-momentum, m-mass, v-velocity)
 |  | 
        |  | 
        
        | Term 
 
        | What two terms are used to describe areas of high and low pressure in the air? |  | Definition 
 
        | Compression: areas of high pressure in the air (peaks of waves) 
 Rarefaction: areas of low pressure in the air (troughs of waves)
 |  | 
        |  | 
        
        | Term 
 
        | How do our ears work similarly to microphones? |  | Definition 
 
        | They both respond to pressure changes, which is mechanical energy and then convert that into electrical energy |  | 
        |  | 
        
        | Term 
 
        | What are the characteristics of Simple Harmonic Motion? |  | Definition 
 
        | Pure tones result from SHM---plot is sinusoidal 
 Periodic
 
 Period is constant-each cycle takes the same amount of time
 
 Frequency is constant
 
 ex: tuning forks and pendulums
 |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | The height of a wave, measured as the peak deviation from the center 
 Always measure from 0
 ex: if peak is at 2 and trough is at -2, the amplitude is 2
 not 4
 
 Decreases over time due to damping
 |  | 
        |  | 
        
        | Term 
 
        | Angular Frequency (ω) VS. ordinary frequency (f) |  | Definition 
 
        | Angular: the number of radians measured per second =2πf
 Ordinary: the number of cycles per second
 
 1 cycle=2π
 |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | the time it takes for a particle on a medium to make one complete vibrational cycle 
 Measured by the distance (in sec) from one wave top to the next (make sure time is on the x-axis)
 |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | Where in its cycle the oscillation begins 
 When the phase is not 0, the entire waveform appears to be shifted in time by φ/ω
 *negative value=delay <-----double check
 
 When calculating, set φ/ω equal to the time between the peak of each wave
 |  | 
        |  | 
        
        | Term 
 
        | Simple Harmonic motion of tuning fork |  | Definition 
 
        | Input force required 
 elasticity generates restoring force, pulls prongs back to resting postion
 
 prongs move beyond resting position due to inertial forces
 
 prongs move back to resting position due to restoring force
 
 1 COMPLETE CYCLE
 
 overshoots and builds restoring force, brings back to resting etc.
 |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | In air: 343 m/s 
 Doesn't depend on properties of sound but on the substance its traveling through
 -travels faster in liquids
 |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | λ = c/f Distance covered by a high pressure region and its succeeding low pressure region
 
 Distance on the x-axis NOT time
 
 High frequency=short wavelength
 |  | 
        |  | 
        
        | Term 
 
        | Longitudinal vs. Transverse waves |  | Definition 
 
        | Longitudinal: waves pile up in the same direction they are moving ex: sound waves
 
 Transverse: waves pile up in different direction from the direction they are moving in
 ex: light waves and water waves
 |  | 
        |  | 
        
        | Term 
 
        | 
What does the spectrum look like for this waveform? 
[image]
   |  | Definition 
 | 
        |  | 
        
        | Term 
 
        | What are the two types of interference associated with sound waves? |  | Definition 
 
        | Destructive interference: addition of waves that are out of phase--->creates cancellation of sound 
 Constructive interference: addition of waves that are in phase--->creates a wave with a higher amplitude
 |  | 
        |  | 
        
        | Term 
 
        | Do complex tones consist of one or more than one frequency? |  | Definition 
 
        | Complex tones involve vibration at MORE than one frequency 
 ex:addition of 2 pure tones of different frequency
 |  | 
        |  | 
        
        | Term 
 
        | What are the types of complex tones? |  | Definition 
 
        | periodic: contain pure tones of different frequencies ex: sign wave
 
 aperiodic: contain random vibrations that don't repeat in time
 
 mixed: periodic+aperiodic
 ex: sound of speech
 |  | 
        |  | 
        
        | Term 
 
        | What is the relationship between harmonics and the length of the vibrating segment? |  | Definition 
 
        | higher harmonics reflect shorter vibrating segments within the vibrating body ex: H2 represents vibration along 1/2 the body
 H3 represents vibration along 1/3 the body
 |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | In periodic sounds: based on H1 (F0) ex: sound composed of 600+900 Hz tone yields
 perception of a 300 Hz tone
 
 In aperiodic sounds: reflects center of frequency band OR
 frequency with the highest amplitude
 
 Units: mels, 1000 mels=1000Hz
 |  | 
        |  | 
        
        | Term 
 
        | Relationships between an octave, semitone, and Cent |  | Definition 
 
        | Octave: the interval between a frequency and another with half or double the original frequency ex: if 1st frequency=100 Hz, then second must equal
 200 Hz to be an octave
 
 Semitone (ST): a "half step" in a 12 note scale
 ex: moving from b flat to b
 
 Cent: 1% of a ST
 ex: 2 ST=200 cents
 
 12 ST MAKEUP 1 OCTAVE
 |  | 
        |  | 
        
        | Term 
 
        | Graphical relationship between frequency and pitch |  | Definition 
 
        | Freq on x-axis, pitch on y-axis---linear to 1000mels and then become logarithmic 
 Same for amplitude and perceived loudness (sone scale)
 shows that doubling loudness requires more than
 double intensity
 |  | 
        |  | 
        
        | Term 
 
        | What is sound pressure's relationship with distance? |  | Definition 
 
        | Sound pressure falls inversely proportional to the distance ex: if distance is doubled, sound pressure is reduced by
 a factor of 2--->equals sound level change of -6dB
 |  | 
        |  | 
        
        | Term 
 
        | Calculating change in dB SPL |  | Definition 
 
        | Change in dB= 20log (pressure of interest/some referenced pressure) some referenced pressure becomes P1
 use pressure of interest in terms of P1
 |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | Occurs when a system is able to store and easily transfer energy between 2 or more different storage modes |  | 
        |  | 
        
        | Term 
 
        | Stiffness VS Mass in mechanical resonance |  | Definition 
 
        | Stiffness=the amount of force required to displace the object some distance increases in stiffness=increases in natural frequency
 
 Mass=inertia-->opposes being accelerated and decelerated (slows things down)
 increases in mass=decrease in natural frequency
 
 fr=(1/2π) x (K/M)^1/2
 |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | Acoustic mass=column of air in resonator wider neck=smaller mass
 longer neck=larger mass
 
 Acoustic Spring=bowl of air
 larger bowl=less stiffness, since air molecules
 have more room to spread out
 |  | 
        |  | 
        
        | Term 
 
        | Sharp tuning vs Broad tuning |  | Definition 
 
        | Sharp: responds to small range of frequencies vibrations persist for a long time (light damping)
 ex: tuning fork, crystal glass
 
 Broad: system responds to a larger range of frequencies
 vibration dies out quickly (heavy damping)
 ex: sound in air, phone earpiece, vocal tract
 |  | 
        |  | 
        
        | Term 
 
        | Formula of acoustic tube open at both ends |  | Definition 
 
        | fr=n x (c/2L)-->fr=resonant freq., c=speed of sound, L=length of tube 
 Lowest resonant frequency=1/2 wavelength
 
 SO: at the open end we want the pressure to be 0, which lines up with the open end of tube (on right) at 1/2 a wavelength
 |  | 
        |  | 
        
        | Term 
 
        | What is the pressure at the open end of a tube |  | Definition 
 
        | pressure=0 or Patm because there are no constraints so air molecules are not confined to a small space 
 velocity is inversely related to pressure
 |  | 
        |  | 
        
        | Term 
 
        | Formula of acoustic tube with one end closed |  | Definition 
 
        | fr=(2n-1)x(c/4L) 
 Lowest resonant frequency=1/4 wavelength
 BECAUSE: at the closed end, pressure peaks due to the constraint (which leads to confinement of air molecules) and this peak falls at the 1/4 mark on wavelength
 |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | A device or process that removes from a signal some frequencies and not others ex: Helmholtz filter (blowing across water bottle, it
 chooses which frequency it wants to resonate)
 
 input signa (x)l x filter (T)=output signal (y)---->convolving
 |  | 
        |  | 
        
        | Term 
 
        | What number of frequencies do Helmholtz filters resonate Vs. tube filters? |  | Definition 
 
        | Helmholtz resonates 1 frequency 
 Tube resonates multiple frequencies
 |  | 
        |  | 
        
        | Term 
 
        | Power-source-filter Model |  | Definition 
 
        | Power=lungs creating the air stream 
 Vibrating vocal folds create the SOURCE
 
 Vocal tract FILTERs input source to create output of speech
 (source and filter are usually independent of on another)
 |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | range of frequencies between the two 3-dB-down points on either side of the peak energy half-power=3 dB down
 
 wider bandwidths=greater damping
 |  | 
        |  | 
        
        | Term 
 
        | What are the two paths an airstream can take when generating speech? |  | Definition 
 
        | 1. air can travel to the oscillator (vocal folds) which creates a period sound signal that is formulated into speech by the resonator (vocal tract) 
 2. air travels through the noise generator (oral constriction or occlusion), creating an aperiodic sound signal that is formulated into speech by the resonator (vocal tract)
 |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | Visceral pleura: thin airtight membrane covering the LUNGS 
 Parietal pleura: covers inner surface of CHEST WALL
 
 both are lubricated with a lubricating film
 holds pleura together and allows sliding movement
 ex: 1 balloon inflated inside a water balloon
 |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | Muscles forcefully expand the volume of chest cavity 
 Increases in volume of chest cavity creates increase in the size of the attached pleural cavity, decreasing the pressure of the fluid inside it
 
 The lungs must now expand in order to reestablish the equilibrium between pressure within pleural cavity and pressure of air inside lungs
 
 Expansion of lungs causes air from the outside to flow in until the pressures are equalized
 |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | When the temperature is constant, the pressure (p) and the volume (V) of a gas are inversely related MEANING: as pressure increases volume decreases and vice versa
 |  | 
        |  | 
        
        | Term 
 
        | What are the 3 types of passive forces in respiration? |  | Definition 
 
        | The natural recoil of muscles, cartilages, ligaments and lung tissue 
 Surface tension of alveoli and between pleura
 
 Pull of gravity
 |  | 
        |  | 
        
        | Term 
 
        | What effect do passive forces have on inspiration and expiration? |  | Definition 
 
        | if apparatus has more air than at rest, it recoils toward a smaller size----EXPIRATION 
 if apparatus has less air than at rest, it recoils toward a larger size----INSPIRATION
 
 the greater the difference from rest, the larger the passive force
 |  | 
        |  | 
        
        | Term 
 
        | What structures controls the active forces of respiration and what is the outcome of these actions? |  | Definition 
 
        | Medulla innervates diaphragm, which lowers and flattens, via the phrenic nerve, causing chest expansions which causes lung expansion 
 Medulla innervates intercostal muscles, causing them to contract, via the thoracic nerves. This causes the ribs to lift up which also causes chest and lung expansion
 |  | 
        |  | 
        
        | Term 
 
        | Muscles involved in the active forces of respiration |  | Definition 
 
        | Inhalation: external intercostals (superficial)& interchondral internal intercostals (deep) 
 Exhalation: interosseous internal intercostals (deep)
 
 Abdominal muscles involved: rectus abdominis, external/internal obliques, transverse abdominis
 |  | 
        |  | 
        
        | Term 
 
        | Two-part chest wall model |  | Definition 
 
        | When the volume/contents of abdomen stay the same: if you move your diaphragm up, chest moves out and
 abdomen moves in
 
 if you move your diaphragm down, chest moves in and
 abdomen is pushed out
 |  | 
        |  | 
        
        | Term 
 
        | Exchanged air volume terms |  | Definition 
 
        | tidal volume: small squigglies on graph---amount of air exchanged during type cycle of quiet breathing
 
 Vital capacity: maximum amount of air a person can expel from the lungs after a maximum inhalation
 
 Resting/relaxation volume: respiratory system is at about 40% of vital capacity when relaxed and upright--produced entirely through passive force
 
 Inspiratory reserve volume (IRV): max volume of air inspired from peak of tidal volume
 
 Expiratory Reserve Volume (ERV): max volume of air expired from trough of tidal volume
 
 Inspiratory Capacity: resting level to maximum inspiration
 
 Total lung capacity= vital capactity+resting/residual volume
 |  | 
        |  | 
        
        | Term 
 
        | In addition to the diaphragm and intercostals, what muscles may augment expansion of the chest and lungs? |  | Definition 
 
        | sternocleidomastoid scalenus
 subclavius
 pectoralis major & minor
 
 serratus anterior
 
 levatores costarum
 serratus posterior superior
 latissimus dorsi
 |  | 
        |  | 
        
        | Term 
 
        | What are the accessory muscles of inspiration |  | Definition 
 
        | Trapezius serratus posterior superior
 levator costarum brevis
 levator costarum longis
 |  | 
        |  | 
        
        | Term 
 
        | What are the accessory muscles of expiration? |  | Definition 
 
        | latissimus dorsi 
 serratus posterior inferior
 |  | 
        |  | 
        
        | Term 
 
        | Quiet breathing cycle VS speech breathing cycle |  | Definition 
 
        | Quiet: 40% of time spent on inspiration 60% of time spent on expiration
 
 Speech: 10% of time spent on inspiration
 90% of time spent on expiration
 |  | 
        |  | 
        
        | Term 
 
        | Volumes of air expended in tidal breathing, conversational speech, and loud speech |  | Definition 
 
        | tidal: inhale to 50% VC exhale to 40% VC---relaxation volume
 
 conversational: inhale to 60% VC
 exhale to 35% VC
 
 loud speech: inhale to 80% VC
 exhale to 35% VC or lower (because we use
 more of our inspiratory reserve to produce loud speech)
 |  | 
        |  | 
        
        | Term 
 
        | For the graph showing that muscular pressure is required to achieve targeted alveolar pressure: |  | Definition 
 
        | At large lung volumes: a negative (inspiratory) muscular pressure is required to counteract the high positive (expiratory) relaxation pressure 
 at mid-lung volume: slight positive muscular pressure is required to achieve targeted alveolar pressure
 
 at small lung volume (near end of utterance) :increasingly greater positive muscular pressure is required
 |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | measures respiratory pressure 
 pressure will move column of liquid (water or mercury) a certain distance and that distance will be measured to determine air pressure
 |  | 
        |  | 
        
        | Term 
 
        | Ways to measure air pressure: |  | Definition 
 
        | Direct assessment of subglottal pressure-invasive: tracheal puncture
 esophageal balloon
 
 Indirect assessment-less invasive
 pharyngeal pressure--pass tube through nose
 intraoral pressure--pass a sensor around teeth
 |  | 
        |  | 
        
        | Term 
 
        | How do you decided whether to use a spirometer or a pneumotachograph? |  | Definition 
 
        | spirometer: measures airflow during NONspeech tasks 
 pneumotachograph: measures flow during speech, usually collected via face mask
 |  | 
        |  | 
        
        | Term 
 
        | Calibration of a pneumograph |  | Definition 
 
        | Measure the rib cage and abdominals during two known volumes can attain these measurements through inspiring and
 expiring a known volume of air from a calibrated bag
 OR
 
 Measure the rib cage and abdominals several times throughout an isovolume maneuver
 must stay at isovolume by valsava or shutting the mouth
 |  | 
        |  | 
        
        | Term 
 
        | How does a c-spine unjust effect speech breathing? |  | Definition 
 
        | Speaks at large lung volumes to compensate for expiratory muscle impairment 
 Uses larger lung volumes to increase loudness
 
 abnormal chest wall behavior due to loss of ab function
 
 abdominal binders will help clients because it will give a little more muscle force
 |  | 
        |  | 
        
        | Term 
 
        | Deviances in speech breathing in the Deaf |  | Definition 
 
        | inappropriate pauses and durations 
 Dip below 35% VC
 
 Do not use higher lung volumes to create louder sounds
 |  | 
        |  | 
        
        | Term 
 
        | Positive effects of behavioral modification toward  higher lung volume initiation levels for expiratory limbs |  | Definition 
 
        | longer utterance strings between inspiratory refills 
 more natural phrasing
 
 higher relaxation forces available at higher lung volumes
 
 possible voice quality improvement, leading to articulatory improvement
 |  | 
        |  | 
        
        | Term 
 
        | What are the primary modes of speech communication after a laryngectomy? |  | Definition 
 
        | Electrolarynx: mechanical vibration at the neck/mouth completely replaces the source---taps against throat 
 Esophageal:patient sucks air into esophagus and releases it to excite remaining pharyngeal tissues--burping
 
 Tracheo-esophageal speech: one way valve is surgically implanted connecting the stoma to esophagus. When stoma is obstructed air can be directed from lungs to esophagus to excite remaining tissues
 |  | 
        |  | 
        
        | Term 
 
        | Extrinsic laryngeal muscles |  | Definition 
 
        | Have one attachment to the larynx and one elsewhere 
 Suprahyoid muscles are located above the larynx and have ability to pull larynx superiorly---shortening vocal tract
 
 Infrahyoid muscles are located below the larynx and have ability to pull it inferiorly---elongating vocal tract
 |  | 
        |  | 
        
        | Term 
 
        | Components of myoelastic aerodynamic theory |  | Definition 
 
        | myo=muscle 
 elastic=vocal fold's tension varied by muscle and tissue elasticity
 
 aerodynamic: vocal fold vibration as a result of aerodynamic forces
 |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | phonation requires that subglottal pressure exceeds pressure above vocal folds by a threshold value vocal folds closed, air pressure below increases
 pressure becomes enough to blow apart folds
 
 Bernoulli effect: (1/2)ρv^2 + p=constant
 velocity of air through constricted glottis is faster
 than that in the vocal tract--creates a lower glottal
 pressure, sucking vocal folds closed again
 |  | 
        |  | 
        
        | Term 
 
        | What are the 6 parameters of voice control? |  | Definition 
 
        | Loudness Pitch
 Tightness (breathy to pressed)
 Register(whistle, falsetto, fry)
 Sonority (dull to ringing)
 Roughness
 |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | More mass=lower F0 Longer (with mass)=lower F0
 Longer (less mass)=higher F0
 More tension=higher F0-->from lengthening of folds
 
 Infrahyoid muscles:lower F0
 Suprahyoid muscles:raise F0
 Sternohyoid, sternothyroid,omohyoid muscles=lower F0
 by lowering larynx to reduce tension
 Geniohyoid, mylohyoid, digastric, stylohyoid=raise F0
 by rasing larynx to increase tension
 |  | 
        |  | 
        
        | Term 
 
        | Posterior cricoarytenoid muscle (PCA) |  | Definition 
 
        | Intrinsic laryngeal muscle 
 originates on cricoid lamina moving up and to sides to insert on upper and back surfaces of arytenoid cartilage
 
 Contraction:rocks arytenoid cartilage away from midline
 ABDUCTION
 |  | 
        |  | 
        
        | Term 
 
        | Lateral cricoarytenoid muscle (LCA) |  | Definition 
 
        | Intrinsic laryngeal muscle 
 Originates from upper rim of cricoid cartilage moving up and back to insert on front surface of arytenoid cartilage
 
 Contraction: rocks arytenoid cartilage toward the midline
 ADDUCTION
 |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | combined with vocal ligament to become vocal cord |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | Intrinsic laryngeal muscle 
 Originiates outer front/side of cricoid cartilage and inserts on thyroid cartilage
 3 components: pars:rectus, oblique, media
 
 Contraction: forward sliding of thyroid cartilage and backward sliding of cricoid cartilage
 |  | 
        |  | 
        
        | Term 
 
        | Interarytenoid (arytenoid) muscle |  | Definition 
 
        | Intrinsic laryngeal muscle 
 Originates on one arytenoid cartilage and inserts on back surface of another arytenoid cartilage
 
 Contraction: pulls arytenoid cartilages toward one another either through an upward inward and back sliding movement or through tipping action
 Also pulls epiglottis back and down to cover opening
 into larynx
 |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | The percentage of time in each cycle in which the vocal folds are open 
 T0/T---T0=time measured between beginning to end of
 wave(length of time air is flowing-folds open)
 T=time measured between end of first wave to end
 of second wave(total duration of each vibrational
 cycle)
 |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | Portion of time in each cycle where the folds are moving outward divided by the time where the folds are moving inward: Tp/Tn 
 Explains how far from symmetric the waveform bump is
 |  | 
        |  | 
        
        | Term 
 | Definition 
 
        | Brassy timbre: large skewing quotient or a small open quotient (jagged waveform) more high frequencies
 Smaller spectral slope-stronger high
 frequencies
 
 Fluty timbre: higher open quotient and low skewing quotient (smoother curve)
 gradual changes in airflow
 Larger spectral slope-more rapid decrease of
 amplitudes as we move to higher frequencies
 Stronger low frequencies
 |  | 
        |  | 
        
        | Term 
 
        | What does timbre or vocal quality depend on? |  | Definition 
 
        | Differences in: pitch
 vocal fold closure
 vocal fold vibration initiation and irregularities
 |  | 
        |  |