Ville Pulkki, Matti Karjalainen — Communication Acoustics- An Introduction to Speech, Audio and Psychoacoustics

Yield

846 of 2862 paragraphs kept (29.6%). Target for mining: 30%–50% — ⚠️ BELOW target.

Pre-Assessment

Ville Pulkki and Matti Karjalainen are both highly credible acoustics researchers; Pulkki is a professor at Aalto University known for spatial audio (Vector Base Amplitude Panning, VBAP) and Karjalainen was a pioneering professor of audio signal processing at Aalto (Helsinki University of Technology) before his passing in 2010, with decades of work in speech acoustics, loudspeaker design, and psychoacoustics. The book is a 2015 Wiley textbook, so it’s reasonably current for fundamentals, though research in some areas (e.g., immersive audio) has advanced since.

The likely yield given a mining stance for “applications of acoustic communication” is predominantly structured concepts/frameworks: the book is organized to link physical acoustics, speech production/perception, audio technology, and psychoacoustics into an applied framework. Expect fewer raw facts you’ll need to memorize and more usable conceptual maps connecting theory to application domains (speech coding, loudspeaker/room acoustics, hearing aids, spatial audio). The authors’ applied-research backgrounds make this a strong source for technology-oriented applications rather than speculation. Expect moderately dense technical content — mining will likely mean skimming chapter structures and targeted extraction of application-relevant sections (speech, psychoacoustics, audio systems) rather than reading linearly.

Reading Goal

Prioritizing: Causal Relationships (Understanding applications requires seeing how acoustic signals cause behaviors/outcomes), Factual Claims (Needs concrete facts about who uses acoustic communication and how), Connection Points (Mapping acoustics to diverse application domains (tech, biology, medicine) is exactly the goal), Definitional Content (Needs clear definitions of acoustic communication concepts to build understanding) De-prioritizing: Contrarian or Surprising Claims (Applications focus is pragmatic; surprises less central but notable), Inspiration and Speculation (Future possibilities useful but secondary to understanding existing applications)

Thesis

Sound quality judgments depend on listener context and expectations · ch. 68

Argument

  1. Sound technology work needs acoustics, perception, and signal processing jointly. — ch. 0
  2. Hearing serves both environmental orientation and communication since early animal evolution — ch. 0
  3. Echolocating bats build image-like environmental representations from reflected chirps — ch. 0
  4. Sound storage digitized fully but human ears force analog endpoints — ch. 0
  5. Sound cannot persist in time because it leaves no physical trace — ch. 0
  6. Digital audio’s rise made auditory perception knowledge essential to engineers — ch. 0
  7. Noise is defined by annoyance, disturbance, or hearing harm rather than loudness alone — ch. 0
  8. Vision dominates audition except where visual events are absent or ambushed — ch. 0
  9. Voice has become a natural interface for human-machine communication — ch. 0
  10. Voice-based computer interfaces required granting machines language processing and world knowledge — ch. 0
  11. Noise is defined as sound that annoys, disturbs, or risks hearing damage — ch. 0
  12. Sensory efficiency has driven animal evolution and survival — ch. 0
  13. Natural and engineered systems organize as vertical control hierarchies — ch. 1
  14. Engineering perspectives increasingly serve computational modelling of auditory perception. — ch. 1
  15. Internal models of reality must trade completeness for tractability. — ch. 1
  16. Research advances only through sustained iteration across abstraction levels — ch. 1
  17. Machines lead humans in logic tasks but lag in pattern recognition. — ch. 1
  18. Pythagoras established the inverse relation between pitch and string length — ch. 1
  19. Communication acoustics joins basic research and engineering toward shared goals — ch. 1
  20. Multidisciplinary problems cannot be mastered within a single knowledge domain — ch. 1
  21. Computational modelling is merging experimentation and theory into one method — ch. 1
  22. Computer simulation dramatically expanded modeling’s power over physical models — ch. 1
  23. The human auditory system is the hardest link in the communication chain. — ch. 1
  24. Very general theories guide thinking but resist direct application to specific cases — ch. 1
  25. Abstracting away details and concretizing them frame scientific research as one cycle — ch. 1
  26. Systems are analyzed through complementary structure and function concepts — ch. 1
  27. Evolution produced language and engineering, but machines still lag in pattern recognition — ch. 1
  28. Physical, biological, and engineered systems share describable general properties — ch. 1
  29. Heterarchies distribute control for versatility while data become information through observation — ch. 1
  30. A system’s output depends on its remembered history — ch. 1
  31. Heterarchical, distributed control can outperform strict hierarchy under changing conditions. — ch. 1
  32. Similar-looking phenomena across domains still need domain-specific scientific concepts. — ch. 1
  33. The human auditory system is communication acoustics’ hardest link to model — ch. 1
  34. Audio and speech technology design should be grounded in perceptual mechanisms — ch. 1
  35. A mass on a spring forms the simplest vibrating system — ch. 2
  36. Sound as physical event and sound as auditory perception are distinct — ch. 2
  37. Most sound arises from vibrating mechanical objects in a medium — ch. 2
  38. Sound’s physical force is negligible yet its informational effects matter greatly. — ch. 2
  39. Room reflections shape how well speech communicates across a space. — ch. 5
  40. Resonance can be engineered to strengthen sound or damped to prevent malfunction — ch. 5
  41. Helmholtz resonance shapes violin bodies, speaker designs, and car cabin noise — ch. 5
  42. Bending stiffness makes bar vibrations dispersive and inharmonic. — ch. 5
  43. Impedance discontinuities split an arriving wave into reflected and transmitted parts — ch. 5
  44. Solids support shear forces and thus transversal waves, unlike fluids. — ch. 5
  45. Relative motion between a sound source and listener shifts perceived pitch — ch. 5
  46. Noise barriers only effectively block high-frequency traffic sound, not low frequencies — ch. 5
  47. Sound intensity is a vector describing the directional flow of sound energy. — ch. 5
  48. Sound pressure is tiny pressure deviation, and human hearing spans a specific Pa range — ch. 5
  49. Sound diffraction arises when a wavefront’s edge acts as a secondary source — ch. 5
  50. Tube end conditions determine which harmonic partials an instrument produces — ch. 5
  51. Rigid-wall tube terminations fully reflect waves while open ends reflect with phase inversion. — ch. 5
  52. Any wave can be decomposed into two counter-travelling component waves. — ch. 5
  53. Coherent sounds interfere by amplitude while incoherent sounds sum by power. — ch. 5
  54. Opposing waves do not annihilate because their energy just shifts form. — ch. 5
  55. Stiffness makes transversal waves dispersive and their modal tones inharmonic — ch. 5
  56. Compressible air in a volume forms a mechanical spring for resonance — ch. 5
  57. A vibrating string has infinitely many resonant frequencies — ch. 5
  58. Resonance can amplify desired sound or cause harmful machine vibration — ch. 5
  59. The Helmholtz resonator models confined air as a spring with an air-mass plug — ch. 5
  60. Vibration generates acoustic waves while sound radiation drains vibration energy — ch. 5
  61. Coupled masses vibrate either along or perpendicular to spring direction — ch. 5
  62. Opposing traveling waves of the same frequency create standing waves with nodes. — ch. 5
  63. Coupled oscillators produce complex resonances shared by instruments, voices, and rooms — ch. 5
  64. Any discontinuity in a medium reflects an incident wavefront — ch. 5
  65. Coherent sound addition yields double the amplitude gain of incoherent addition — ch. 5
  66. The absorption coefficient measures the fraction of incident sound energy absorbed. — ch. 5
  67. Any vibration decomposes into weighted sums of a system’s modal oscillations — ch. 5
  68. Phase alignment determines whether sounds sum by amplitude or by power — ch. 5
  69. Tube termination conditions determine which harmonics a wind instrument produces — ch. 5
  70. Early reflections boost perceived loudness while loud late reverberation degrades intelligibility — ch. 6
  71. In steady state, reverberant sound level is uniform throughout a room. — ch. 7
  72. Sound from a source falls 6 dB per distance doubling until reverberation takes over — ch. 7
  73. Room sound decay is exponential, appearing linear on a dB scale — ch. 7
  74. Hard-walled rooms behave as three-dimensional resonators with many audible modal frequencies — ch. 8
  75. Beyond the reverberation distance, loudness stays constant while reverberance increases. — ch. 8
  76. A concert hall’s acoustic field has billions of vibrational degrees of freedom. — ch. 9
  77. Room reflections can be modelled as sources in mirrored rooms — ch. 9
  78. Geometric acoustics fails on diffraction at low frequencies in complex rooms — ch. 9
  79. Element-based acoustics methods grow computationally costly at higher frequencies — ch. 9
  80. Modal density scales with spatial dimension, from flat in 1D to squared in 3D. — ch. 9
  81. Ray-tracing and image-source methods fail on low-frequency diffraction at corners — ch. 9
  82. Room acoustics can be simulated by statistically tracing sound rays until their energy decays — ch. 9
  83. Above a critical frequency, room acoustics become statistically tractable as diffuse fields. — ch. 9
  84. Non-linear acoustics governs high-pressure waves like shocks and cavitation — ch. 9
  85. Converting continuous sound to digital requires time sampling then numeric quantization — ch. 10
  86. Time-frequency transforms make signal processing and interpretation easier — ch. 10
  87. Loudspeakers at high power and low frequencies become highly nonlinear. — ch. 10
  88. Any continuous signal decomposes into sinusoidal partials and convolution simplifies in frequency domain — ch. 10
  89. The Fourier transform measures how a signal matches each sinusoid pair — ch. 10
  90. The Fourier transform trades costly time-domain convolution for simple frequency-domain multiplication — ch. 10
  91. Physically realizable systems cannot respond to future input values — ch. 10
  92. A sound signal is the registered time-varying vibration of a medium — ch. 10
  93. Computer-displayed continuous-looking curves are actually stored sample sequences — ch. 10
  94. Non-linear and time-variant systems generate frequency components absent from the input — ch. 10
  95. Human hearing resists linear time-invariant modeling except at the periphery — ch. 10
  96. LTI systems cannot create new frequency components from their input signals — ch. 10
  97. Frequency-domain analysis mirrors how the human ear processes sound — ch. 11
  98. Signal cropping is equivalent to applying a rectangular window — ch. 11
  99. The ear’s analysis resembles Fourier frequency decomposition of sound — ch. 11
  100. Group delay of modulation is the phase representation most relevant to hearing — ch. 11
  101. The auditory system largely ignores signal phase, driving spectral analysis conventions — ch. 11
  102. Undersampled signals alias because high-frequency components mirror below the Nyquist frequency — ch. 13
  103. Standard audio sampling rates range up from 8kHz speech to 192kHz ultra-high fidelity — ch. 13
  104. Autocorrelation reveals a signal’s fundamental periodicity through periodic peaks. — ch. 13
  105. Wavelet and constant-Q transforms trade time and frequency resolution non-uniformly — ch. 13
  106. Filter banks split broadband signals into sub-bands much like cochlear hearing does — ch. 13
  107. Short-time Fourier analysis converts signals into spectrograms via windowed transforms — ch. 13
  108. Digital signal processing is inherently band-limited by reconstruction filters — ch. 13
  109. Each added quantization bit yields 6dB SNR improvement — ch. 13
  110. Filter banks drive equalization, audio coding, and spatial reproduction — ch. 13
  111. LP inverse filtering flattens signals into spectrally whitened residuals — ch. 14
  112. Any band-limited linear time-invariant system can be implemented as a digital filter — ch. 14
  113. Autocorrelation is the dominant method for linear prediction analysis — ch. 14
  114. Linear prediction models signals as all-pole IIR systems predicting samples from prior ones — ch. 14
  115. Air absorption and room acoustics can be modeled as low-pass and arbitrary filters — ch. 14
  116. Feedback (IIR) filters can become unstable, while feedforward (FIR) filters cannot — ch. 14
  117. Speech recognition picks the model maximizing the probability of observed features — ch. 15
  118. Adaptive filtering changes filter coefficients over time in response to signals. — ch. 15
  119. The similarity between artificial and biological neural networks is only superficial. — ch. 15
  120. Linear prediction order scales with sample rate to capture speech formants. — ch. 15
  121. Real-world signals change over time, so fixed filters need adaptation — ch. 15
  122. Electret microphones trap charge in material so no external voltage is needed — ch. 16
  123. Condenser microphones dominate modern audio because they convert sound to electrical signals efficiently. — ch. 16
  124. A microphone’s sensing principle determines whether its pickup pattern is omnidirectional, dipolar, or cardioid — ch. 16
  125. Perfect sound reproduction tolerates arbitrary signal delay when reproducing recordings. — ch. 16
  126. Room impulse response measurements cannot be made with true perfect impulses from practical sources. — ch. 16
  127. Slight response deviations go unnoticed without an audible reference — ch. 16
  128. Enclosures prevent acoustic short-circuiting that silences low frequencies — ch. 16
  129. Most audio reproduction chain components are now perceptually flawless — ch. 16
  130. Ideal audio reproduction permits gain change and pure delay without degrading quality — ch. 16
  131. Electrostatic transduction, the condenser microphone’s inverse, delivers the highest headphone and speaker quality. — ch. 16
  132. Loudspeakers and room acoustics remain the weak link in audio quality — ch. 16
  133. A good microphone needs flat response from 20 Hz to 20 kHz. — ch. 16
  134. Reverberant rooms make loudspeaker directivity important for sound quality — ch. 16
  135. Sound reinforcement permits only milliseconds of delay while recorded reproduction tolerates seconds — ch. 16
  136. The condenser microphone and its electret variant dominate modern microphone technology — ch. 16
  137. Closed headphones gain isolation but become sensitive to leakage effects. — ch. 16
  138. Headphones come in intra-aural, supraaural, and circumaural form factors. — ch. 16
  139. Headphone cushion leakage degrades low-frequency response but spares mid and high frequencies. — ch. 16
  140. Only part of loudspeaker input power becomes sound energy — ch. 16
  141. The technically precise term for frequency response is magnitude response — ch. 16
  142. Perfect sound reproduction requires an LTI system with unity transfer function — ch. 16
  143. Loudspeaker-room interactions remain the weak link in audio reproduction chains — ch. 16
  144. Real loudspeakers show flat magnitude response only below 800 Hz with a midrange dip — ch. 16
  145. Headphone cushion leaks alter only the low-frequency transfer to the eardrum — ch. 16
  146. Reverberant rooms favor directional loudspeakers to control sound colouration — ch. 16
  147. A plus or minus 5 dB loudspeaker deviation goes unnoticed without a direct reference — ch. 16
  148. Headphones originated as noise isolation for radio operators — ch. 16
  149. Noise is defined by its disturbing effect relative to a desired signal — ch. 17
  150. Objective measures based on hearing models substitute for tedious listening tests of distortion. — ch. 17
  151. Signal processing can compensate for loudspeaker and headphone imperfections. — ch. 17
  152. Equalizing a loudspeaker response can worsen off-axis sound quality. — ch. 17
  153. Equalizers invert measured system impulse responses to flatten magnitude response — ch. 17
  154. Even ideal equalization degrades off-axis response and can amplify distortion and noise — ch. 17
  155. Total harmonic distortion measures all components a fundamental generates, including non-harmonic ones. — ch. 17
  156. Nonlinear equalization methods remain underdeveloped in audio engineering — ch. 18
  157. Linear audio distortion is easy to equalize while non-linear distortion resists compensation — ch. 18
  158. Average speaking fundamental frequency is 120 Hz for men and 200 Hz for women — ch. 19
  159. A full speech communication chain spans brain, vocal organs, channel, and hearing. — ch. 19
  160. The glottal waveform can be estimated indirectly through inverse modeling of microphone recordings — ch. 19
  161. Vowels keep the vocal tract open and vary little by context, unlike consonants — ch. 19
  162. Phonetic information concentrates either in a phone’s steady core or its transition boundary — ch. 19
  163. Unvoiced speech arises from turbulence at constrictions or sudden pressure releases — ch. 19
  164. Speech segments are classified by abstract classes, concrete sounds, and transition units — ch. 19
  165. All vowel distinctions reduce to tongue position, openness, and lip rounding — ch. 19
  166. Consonants differ from vowels in intensity, context-dependence, and articulation constriction — ch. 19
  167. Languages differ widely in vowel category counts, from two to over ten. — ch. 19
  168. Phonation types differ by glottal airflow and spectrum shape — ch. 19
  169. The International Phonetic Alphabet attempts a universal notation for every speech sound — ch. 19
  170. Voiced speech originates from airflow through the vibrating vocal folds across the glottis — ch. 19
  171. Speech is a continuous flow that still requires discrete units to be understood — ch. 19
  172. Speech sound generation was mechanically modeled as early as the 18th century — ch. 19
  173. Speakers shift glottal closure timing to control the spectral brightness of their voice. — ch. 19
  174. Speech is uniquely human among species’ communication abilities. — ch. 19
  175. Articulation shapes the voice by filtering glottal sound through the vocal tract — ch. 19
  176. Speech is the original form of linguistic communication, predating writing. — ch. 19
  177. Languages range from two to over ten vowel categories — ch. 19
  178. Computerized speech handling required simplified phonetic notations tailored per language — ch. 19
  179. Vocal tract length differs by sex and its resonances form speech formants. — ch. 19
  180. The vocal apparatus functions as a pressure source driving a resonant filter system — ch. 20
  181. Speech production maps onto a three-stage cascaded electrical circuit analogy — ch. 20
  182. In tonal languages like Chinese, pitch changes alter the phoneme itself — ch. 20
  183. Vocal tract acoustics reduce to a cross-sectional area function along one axis — ch. 20
  184. Voiced and unvoiced speech differ in whether source is glottal oscillation or frication noise — ch. 20
  185. Consonant classes are produced by distinct vocal tract closure configurations — ch. 20
  186. Languages vary in whether timing or syllable quantity carries meaning — ch. 20
  187. Acoustic reflections arise at any change in tube cross-sectional area — ch. 20
  188. Speech production reduces to lungs as compressor driving a glottal oscillator through resonating tracts — ch. 20
  189. Speakers vary pitch to signal emotion, questions, and focus. — ch. 20
  190. Prosody denotes speech features not tied to segmental structure — ch. 20
  191. Speakers use pitch variation to signal statements versus questions — ch. 20
  192. Glottal closing generates most vocal-tract excitatory energy. — ch. 20
  193. The glottal waveform’s closing phase is abrupt and carries most excitatory energy. — ch. 20
  194. Plosive consonants begin with silence then a burst when the tract opens. — ch. 20
  195. Mathematical source-filter models of speech enable practical synthesis and coding algorithms — ch. 20
  196. The vocal tract can be simulated as a cascade of acoustic transmission line segments — ch. 21
  197. High-pitched soprano singing is unintelligible because harmonics are too sparse for formants — ch. 21
  198. Formant tracking to harmonics boosts loudness, not intelligibility, in soprano singing — ch. 21
  199. Overtone singing selects harmonics with sharp vocal-tract resonances to create melodies — ch. 21
  200. Sopranos retune formants to match harmonics to boost loudness, not intelligibility — ch. 21
  201. Articulatory synthesis models speech dynamics but is too complex for practical synthesizers — ch. 21
  202. A unified source-filter model describes human and synthetic voice alike — ch. 21
  203. Singing and speech differ systematically in pitch control, spectrum, vibrato, and range — ch. 21
  204. Any phone of a language can be synthesized with 4-5 parallel formant filters — ch. 21
  205. Instruments spanning multiple sound-generation classes force contested classification — ch. 22
  206. Music and speech are utility sounds distinguished by their primary role — ch. 22
  207. Instrument sounds are endlessly varied yet fall into families sharing generation principles — ch. 22
  208. A single amplitude envelope misses that harmonics decay and modulate at different rates — ch. 24
  209. Musical instrument sounds divide into attack, decay, sustain, and release phases — ch. 24
  210. Hearing is highly sensitive to temporal changes in sound — ch. 24
  211. Resonators color spectral and temporal content of transmitted sound. — ch. 24
  212. Most real instruments are nonlinear and resist simple filter-cascade modelling — ch. 24
  213. Resonance frequencies produce longer build-up and decay than off-resonance — ch. 24
  214. Fretted instruments set pitch by vibrating string length — ch. 24
  215. Piano hammers rebound and strike strings multiple times per note — ch. 24
  216. Idiophone and most membranophone pitch cannot be controlled by the player — ch. 24
  217. Plucked strings vibrate autonomously after excitation, simplifying their modelling. — ch. 24
  218. Bowed string motion is a stick-slip effect producing a sawtooth wave — ch. 24
  219. Speech tracts lack coupling that brass instruments synchronize with. — ch. 24
  220. Musical instruments couple excitation to resonances; human speech does not — ch. 24
  221. Aerophone design tunes resonance modes so the instrument becomes musically usable — ch. 24
  222. FM synthesis generates harmonic spectra when the modulating frequency equals the carrier frequency — ch. 25
  223. Placing all string damping at terminations yields efficient digital synthesis — ch. 25
  224. Natural background sounds are synthesized statistically for virtual environments — ch. 25
  225. Continuous-excitation instruments like flutes attack slowly while impulse-excited ones do not — ch. 25
  226. A guitar body’s effect can be simulated by convolution with its measured impulse response — ch. 25
  227. Computational models can synthesize natural ambient sounds like footsteps and thunder — ch. 25
  228. Hearing is a staged chain from air capture through mechanical conduction to neural processing — ch. 26
  229. The human auditory system evolved specifically for spoken-language analysis — ch. 26
  230. Human hearing diverged from other mammals mainly via speech analysis — ch. 26
  231. Auditory nerve responses can be experimentally recorded by microelectrodes. — ch. 27
  232. The ear emits measurable echoes requiring active neural involvement — ch. 27
  233. Loud sounds spread cochlear activation broadly and respond faster than soft sounds — ch. 27
  234. Stronger tones in the cochlea actively mask neighboring weaker tones via two-tone suppression. — ch. 27
  235. Cochlear pitch mapping exploits the mass of vibrating liquid varying with route length — ch. 27
  236. Two tones presented together generate an audible combination (difference) tone not physically present. — ch. 27
  237. Pinna asymmetry creates front-back and elevation cues for directional hearing. — ch. 27
  238. Single auditory nerve fibres encode only a narrow 20-40 dB dynamic range. — ch. 27
  239. Head shading creates interaural level differences used for sound localization — ch. 27
  240. The cochlea’s sharp frequency selectivity needs an unexplained second filter. — ch. 27
  241. The Eustachian tube pressure-balances the middle ear against altitude changes — ch. 27
  242. The middle ear evolved as an impedance transformer to bridge air-water sound energy loss — ch. 27
  243. Middle-ear impedance matching boosts pressure transfer roughly 30-fold — ch. 27
  244. The ear canal acts as a quarter-wavelength resonator amplifying 3-4 kHz by 10 dB — ch. 27
  245. Single auditory neurons encode only a narrow 20-40 dB dynamic range — ch. 27
  246. A competing tone at another frequency suppresses a cochlea channel’s response — ch. 27
  247. Hair cells actively amplify cochlear vibration rather than only sensing it — ch. 27
  248. Cubic difference tones reveal nonlinear cochlear mechanics even at low sound levels — ch. 27
  249. The auditory periphery is non-linear and cannot be captured by one transfer function. — ch. 27
  250. Ion concentration differences across the basilar membrane create an electric potential. — ch. 27
  251. The cochlear nucleus functions like a preamplifier and initial spectral analyzer — ch. 28
  252. Acoustic engineering usually needs only cochlear models, not higher nuclei — ch. 28
  253. Population coding across many neurons achieves precise and robust auditory processing — ch. 28
  254. Auditory models link acoustic stimulus features to perceived attributes computationally. — ch. 28
  255. Auditory nerve phase locking degrades above 1500 Hz and is weak above 4 kHz — ch. 28
  256. Loudness above 60 dB is encoded by cross-frequency spread, not single-neuron rate — ch. 28
  257. fMRI identifies active brain regions well but is noisy and time-slow for auditory study. — ch. 28
  258. Single neuron auditory responses are mapped through controlled stimulus repetition — ch. 28
  259. Computational auditory models serve knowledge, audio-quality measurement, and diagnostics — ch. 28
  260. Bottom-up neuron-by-neuron auditory modelling is computationally and knowledge-wise infeasible. — ch. 28
  261. The superior colliculus is the only mammalian brain nucleus with a topographical auditory map — ch. 28
  262. Single-neuron auditory responses are mapped invasively in animals only — ch. 28
  263. Speech remains understandable at high levels because timing carries formant info — ch. 28
  264. Humans cannot reliably report auditory attributes on absolute internal scales. — ch. 29
  265. Constant stimuli remains gold standard but is too slow for routine use — ch. 29
  266. Simple stimuli fail to represent how hearing processes real complex sounds — ch. 29
  267. Tracking audiometry maps hearing thresholds but ignores response bias — ch. 29
  268. Trained listeners improve test sensitivity but misrepresent general audience opinion — ch. 29
  269. Psychophysical scales are built by adjusting sounds to match reference ratios — ch. 29
  270. Listener personality biases reported auditory thresholds across subjects — ch. 29
  271. Valid psychoacoustic listening tests require blind conditions and carefully worded tasks. — ch. 29
  272. Game-like testing yields less biased hearing-aid results in children than formal tasks. — ch. 29
  273. Introspection alone cannot serve as accepted scientific auditory observation — ch. 29
  274. Thresholds and auditory scales link physical sound attributes to perceived auditory events — ch. 29
  275. Psychoacoustics developed largely through communication technology challenges — ch. 29
  276. Thresholds can be measured by tracing stimulus change until perception flips — ch. 29
  277. Psychoacoustics studies higher auditory functions where physiology is unknown — ch. 29
  278. Relative magnitude judgments can be anchored into absolute psychophysical scales — ch. 29
  279. Psychophysical functions map continuous physical sound scales onto varied perceptual scales. — ch. 29
  280. Perceived-loudness matching often needs separate listening tests to achieve — ch. 29
  281. Constant-stims method maps full psychophysical functions rather than single thresholds — ch. 29
  282. Signal detection theory originated in WWII radar plane detection — ch. 29
  283. Trained listener panels trade real-world representativeness for analytic test resolution — ch. 29
  284. Vision dominates hearing in localization, identification, and size judgment — ch. 29
  285. Forced-choice guessing floors push threshold criterion above 50 percent detection — ch. 29
  286. Paired comparison against anchors reduces bias in absolute judgments — ch. 29
  287. Uncontrolled loudness differences confound audio quality listening-test results — ch. 29
  288. Perceptual thresholds blur because listener internal noise varies by personality — ch. 29
  289. Anechoic chambers misrepresent how loudspeakers sound in normal rooms — ch. 29
  290. Test method means the logic selecting sound attributes across successive tasks — ch. 29
  291. Auditory perception must be studied indirectly through measurable external reactions. — ch. 29
  292. Auditory experimentation resembles measuring an unreliable device against an unpredictable system — ch. 29
  293. Ascending and descending stimulus runs are averaged to derive perceptual thresholds — ch. 29
  294. Mean Opinion Score scales standardize audio-quality evaluation on a 1-to-5 range — ch. 29
  295. Perceived loudness depends on frequency content and duration, not just sound pressure level — ch. 29
  296. Adjustment steps sized near the JND prevent subjects overestimating imperceptible changes — ch. 29
  297. The method of limits is inherently prone to response bias — ch. 29
  298. Analysis of variance tests whether any independent variable affects a dependent variable. — ch. 30
  299. Perceptual structure analysis indirectly recovers individual feature-usage in auditory perception. — ch. 30
  300. Repertory grid technique lets each subject generate their own descriptive dimensions via triadic comparisons. — ch. 30
  301. Audio codec testing requires methods that reveal unknown perceptual attributes — ch. 30
  302. Multidimensional scaling maps perceived sound dissimilarities without labeling the perceptual dimensions — ch. 30
  303. Consensus-based sensory panels risk leader bias but training can counter it — ch. 30
  304. Free sorting adds post-hoc verbal labels that enable interpreting perceptual dimensions. — ch. 30
  305. Adaptive staircase procedures trade efficiency and bias avoidance against convergence risk — ch. 30
  306. Verbal elicitation dominates sensory science via consensus or individual vocabularies — ch. 30
  307. Descriptive sensory analysis maps perceived sound differences onto an N-dimensional attribute space — ch. 30
  308. Careful listening tests validly reveal how acoustic attributes become auditory attributes. — ch. 30
  309. Sound attributes are independent variables manipulated to elicit dependent responses. — ch. 30
  310. Sensory scales can be calibrated for equal intensity across different attributes — ch. 30
  311. Paired comparison lets flash profiling skip time-consuming attribute training. — ch. 30
  312. Subjective listening tests map manipulated acoustic variables to measured responses. — ch. 30
  313. Listening-test statistics must inform experimental design from the outset — ch. 30
  314. Generalized procrustes analysis aligns different subjects’ attribute ratings into common dimensions. — ch. 30
  315. Assessors can use their own vocabulary instead of agreeing on descriptors — ch. 30
  316. Pointing gestures can localize sound sensations where words fall short — ch. 30
  317. The cochlea splits sound into narrowband signals that the brain processes individually — ch. 31
  318. The hearing threshold is measured from sounds reaching the subject’s binaural position. — ch. 31
  319. Sound audibility depends on both its level and its frequency — ch. 31
  320. Practical speech communication uses only a small slice of hearing’s full range — ch. 31
  321. Human hearing is most sensitive to sounds around 3-4 kHz. — ch. 31
  322. Typical one-metre speech at 60-70 dB is optimally tuned for auditory communication — ch. 31
  323. Uniform masking noise must drop 3 dB per octave above 500 Hz. — ch. 31
  324. Hearing’s lower limit is the minimum audible field; upper is pain — ch. 31
  325. The phon scale defines loudness relative to equal-loudness matches at 1 kHz — ch. 31
  326. Loudness is measured subjectively against 1 kHz reference tones — ch. 31
  327. One sound can mask another even when their spectra do not overlap. — ch. 31
  328. A-weighted decibels are a rough practical approximation of perceived loudness — ch. 31
  329. Spectral masking by loud sounds is exploited to design lossy audio codecs. — ch. 31
  330. Tone-on-tone masking can be detected through beating and combination tones alone — ch. 32
  331. Coherent amplitude modulation across frequency bands may drive auditory source grouping. — ch. 32
  332. Backward masking is a weak and unreliable effect appearing mainly in novice listeners. — ch. 32
  333. Forward masking suppresses sounds for 150-200 ms after masker offset even at high levels. — ch. 32
  334. Hearing groups frequency bands by shared envelope modulation, reducing masking — ch. 32
  335. Complex real-world maskers are less effective than simple energetic ones predict — ch. 32
  336. Sounds mask both preceding and following sounds but forward masking dominates. — ch. 32
  337. Forward masking decays within roughly 200 ms after sound offset — ch. 34
  338. Each inner hair cell responds best to one frequency plus a widening critical band — ch. 34
  339. Loudness stays constant below critical bandwidth then grows beyond it — ch. 34
  340. Psychoacoustic tuning curves directly reflect cochlear mechanical processing. — ch. 34
  341. Hearing segregates sounds by frequency unless they fall within a critical band — ch. 34
  342. Longer masker sounds produce stronger forward masking — ch. 34
  343. Wider bandwidth increases perceived loudness at equal sound pressure — ch. 35
  344. The Bark scale is linear below 500 Hz and logarithmic above it. — ch. 36
  345. Human spectral analysis resolution runs about 10–15 percent of center frequency — ch. 36
  346. A 10-15 percent bandwidth window serves spectral analysis for audio tech — ch. 36
  347. Notched-masker tests prevent off-frequency listening to measure filter width — ch. 36
  348. Auditory bands from the same source are summed to compute total loudness — ch. 36
  349. The ear’s 120-dB and 20 Hz-20 kHz working range exceeds man-made devices — ch. 37
  350. Pitch discrimination is best near 500 Hz and degrades at both extremes — ch. 38
  351. Pitch is the perceptual property ordering sounds from low to high — ch. 38
  352. Pitch cues convey identity, intonation, and emotion beyond mere speech content — ch. 38
  353. Pitch is not uniquely tied to a single physical frequency — ch. 38
  354. Narrowband noise can carry clearer pitch than some periodic signals — ch. 38
  355. Frequency JND is best around 500 Hz at about 0.3 percent — ch. 38
  356. Musical pitch perception spans roughly 30 Hz to 4 kHz. — ch. 38
  357. Pitch perception requires a tone lasting at least two signal periods — ch. 39
  358. Listeners perceive the fundamental frequency even when its lowest partials are absent — ch. 40
  359. Western orchestral tuning pitch has risen historically for a brighter sound — ch. 40
  360. A set of harmonically related partials shifted together still changes perceived pitch. — ch. 40
  361. Inharmonic sounds like bells can produce multiple simultaneous pitches — ch. 40
  362. The mel scale was derived by asking listeners to double perceived pitch — ch. 40
  363. Outdoor wall and ground reflections produce repetition pitch in real settings. — ch. 40
  364. Place theory cannot fully explain how pitch is extracted from components — ch. 40
  365. Louder signals need disproportionately more dB to double perceived loudness — ch. 40
  366. The phon defines loudness level equal to dB SPL at 1 kHz — ch. 40
  367. Masking noise raises the loudness threshold and fades audible tones — ch. 40
  368. Pitch perception involves both spectral and temporal representations of sound — ch. 40
  369. Summing a signal with its delayed copy creates perceived pitch. — ch. 40
  370. Loudness perception sums auditory bands and signals distance by comparison — ch. 40
  371. Absolute pitch is roughly ten times more precise than trained relative pitch. — ch. 40
  372. Humans perceive a fundamental frequency even when it is absent from the signal — ch. 40
  373. Doubling perceived loudness requires a 10 dB increase. — ch. 40
  374. Human hearing excels at comparative judgments but fails at absolute ones. — ch. 40
  375. Amplitude modulation of noise creates pitch with a flat spectrum — ch. 40
  376. Loudness is perceptual while intensity is physical and must be distinguished — ch. 40
  377. Frequency modulation detection depends on both carrier and modulation frequency. — ch. 40
  378. Place and timing theories fail to explain some complex pitch perception phenomena — ch. 40
  379. Noise with a sharp spectral peak is perceived as pitched. — ch. 40
  380. Doubling perceived pitch of a 2-kHz tone requires about a 15-kHz frequency jump — ch. 40
  381. Perceived loudness can be measured by iterative ratio-matching across subjects — ch. 40
  382. Shifting harmonic partials upward raises perceived pitch despite unchanged envelope modulation — ch. 40
  383. Auditory loudness doubles with every 10 dB increase in sinusoid level — ch. 41
  384. Frequency spread in the cochlea is asymmetric with steeper low-frequency slopes — ch. 41
  385. The basilar membrane’s fixed-spread frequency resolution shrinks relative bandwidth as frequency rises — ch. 41
  386. Perceived loudness of concurrent tones hinges on frequency separation via three distinct mechanisms — ch. 41
  387. Humans detect level changes of about 1 dB at moderate volumes — ch. 41
  388. AM tones change perceived frequency spread, giving extra detection cues that noise lacks. — ch. 41
  389. Amplitude-modulation detection improves with tone level but is level-independent for noise. — ch. 41
  390. Amplitude-modulation detection becomes easier once modulation spreads the spectrum beyond one critical band — ch. 42
  391. Hearing forms loudness by integrating sound energy over about 100-200 ms — ch. 42
  392. Short sounds decay in perceived loudness faster than long sounds. — ch. 43
  393. Time-varying sound loudness is set by integrated loudness peaks, not moment-to-moment level — ch. 43
  394. Human hearing can in principle distinguish astronomically many timbres. — ch. 43
  395. Humans can match durations of silence to sounds of similar length. — ch. 43
  396. Temporal masking makes silence following a sound seem shorter — ch. 43
  397. Timbre distinguishes sounds sharing pitch, loudness, and duration. — ch. 43
  398. A sound’s onset transients largely determine instrument identity — ch. 43
  399. Brief silences are perceptually longer than their physical duration. — ch. 43
  400. Perceived sharpness is stable across subjects and rises with spectral centre of gravity — ch. 44
  401. Hearing repackages one-dimensional sound signals into multidimensional time-frequency objects — ch. 44
  402. Sound level has only a weak effect on perceived sharpness — ch. 44
  403. Fluctuation strength is standardized against a 4 Hz amplitude-modulated reference tone — ch. 45
  404. Modulation frequency determines whether sound is heard as fluctuation, roughness, or multiple tones — ch. 45
  405. Slow sound-level changes are heard as fluctuation and fast ones as roughness — ch. 45
  406. Amplitude-modulated loudness directly increases perceived fluctuation strength — ch. 47
  407. Fast amplitude modulations within a critical band produce roughness perception — ch. 47
  408. Just intonation leaves many intervals audibly mistuned like the D-A fifth — ch. 47
  409. Reversing a signal’s polarity changes its perceived bass level — ch. 47
  410. Auditory cortex specifically attenuates responses to frequently repeated sounds — ch. 47
  411. Arbitrary-sound roughness is estimable by summing per-critical-band contributions — ch. 47
  412. Western major scales consist of five whole tones and two semitones in fixed arrangement — ch. 47
  413. The brain organizes simultaneous sound events into separate auditory streams via auditory scene analysis. — ch. 47
  414. Impulsiveness is estimated from level statistics rather than directly measured — ch. 47
  415. Individual notes are assigned to exactly one auditory stream, altering perceived rhythm. — ch. 47
  416. Interval dissonance increases with position higher in the harmonic series — ch. 47
  417. Gestalt grouping principles apply to hearing as well as vision — ch. 47
  418. Psychoacoustic tonality measures tone-character, distinct from musical tonality terms — ch. 47
  419. Rhythm derives from natural body repetitions like heartbeat and walking. — ch. 47
  420. Noise is masked more easily by tonal parts than tones are masked by noise — ch. 47
  421. Auditory cortex adaptation decreases response to frequent sounds, shaping perception — ch. 47
  422. No single standard method measures perceived tonality accurately — ch. 47
  423. Auditory spatial information alone allows orientation in one’s surroundings. — ch. 47
  424. Simple integer frequency ratios between notes produce the greatest measured consonance — ch. 47
  425. Machine hearing mirrors human perception by comparing feature vectors against known patterns — ch. 47
  426. Synchronized phase harmonics produce a ‘buzzy’ sharpness perceptible without room reflections — ch. 47
  427. Headphone group delay alters audibility of phase-spectrum effects — ch. 47
  428. Reversing the phase of a single harmonic can drastically change its perceived loudness — ch. 47
  429. Hearing perceives synchronized neural firing across critical bands as buzzy timbre — ch. 47
  430. No tuning system can make all diatonic intervals have simple ratios — ch. 47
  431. Room reverberation can render phase-sensitive signals perceptually phase-insensitive — ch. 47
  432. Musical eras are distinguished by their systematic handling of sensory dissonance — ch. 47
  433. One second of exposure triggers neural spectral adaptation in hearing — ch. 47
  434. Peak dissonance between two tones occurs at a quarter critical band separation — ch. 47
  435. Impulsive transients grab attention by signaling state changes in physical objects — ch. 47
  436. Group delay affects perceived quality only when it varies with frequency — ch. 47
  437. Two close sine tones produce amplitude beats at their frequency difference — ch. 47
  438. Perception is a brain interpretation that need not use all sensory detail — ch. 47
  439. Humans can isolate a single speaker amid competing voices and noise — ch. 47
  440. No tuning system can make all diatonic scale intervals perfectly consonant — ch. 47
  441. Whether spectral adaptation dynamics are purely peripheral remains experimentally unresolved — ch. 47
  442. Reverberation destroys the phase information that could encode meaning — ch. 47
  443. Simultaneous cochlear neuron firing across frequencies produces buzzy timbre — ch. 47
  444. Group delay perception thresholds depend strongly on signal content and context — ch. 47
  445. Auditory perception runs parallel bottom-up and top-down processes — ch. 47
  446. A single note can sound rough only below roughly 100 Hz fundamental — ch. 47
  447. Perceptual hearing properties map onto objective signal analysis quantities — ch. 47
  448. Musical notation is a lossy code requiring stylistic knowledge to realize — ch. 47
  449. Humans are perceptually tuned to amplitude and frequency modulations across specific rate bands — ch. 48
  450. Roughness between note partials determines perceived musical dissonance — ch. 48
  451. Perceived musical dissonance reduces to roughness from beating partials. — ch. 48
  452. HRTF definition normalizes ear responses by the head’s absence — ch. 49
  453. Mannequin heads with ear microphones capture realistic spatial audio for recording — ch. 49
  454. The outer ear’s resonant cavities enable elevation perception where other cues fail — ch. 49
  455. Head, torso, and shoulder acoustics shape the localization cues reaching each ear. — ch. 49
  456. Echoes and reverberation convey room geometry and surface properties to listeners — ch. 49
  457. Sound localization evolved in nocturnal mammals and remains vital for prey and predator. — ch. 49
  458. Spatial hearing is calibrated through learning to each listener’s head and pinna geometry — ch. 49
  459. Spatial hearing is described in three distinct coordinate systems with different strengths. — ch. 49
  460. Head-related transfer functions are measured with in-ear microphones in anechoic chambers — ch. 49
  461. A dedicated cone-of-confusion coordinate system describes hard-to-discriminate sound directions. — ch. 49
  462. The ear sits 8 cm off-center, so source-ear distance changes with azimuth — ch. 50
  463. ITD spans 0-700 microseconds across azimuth independent of frequency — ch. 52
  464. Interaural level differences and time shifts trade off to control lateralization — ch. 52
  465. The head shadows and reflects sound to create level differences between the ears. — ch. 52
  466. Human sound localization is remarkably accurate given it processes only two ear signals. — ch. 52
  467. Auditory spatial perception emerges from weighted combination of localization cues — ch. 52
  468. Humans can detect interaural timing differences as small as ten to twenty microseconds — ch. 52
  469. Shoulder reflections create a distinguishable 1-ms delay in head-related impulse responses — ch. 52
  470. Shoulder reflection delays versus direct sound vary inversely with source elevation — ch. 52
  471. Low interaural coherence makes sound events seem diffuse and surrounding — ch. 53
  472. A stationary tone’s frequency alone can shift perceived elevation in the median plane. — ch. 53
  473. Low-frequency interaural level differences cue source distance and signal coherence. — ch. 53
  474. Humans perceive interaural level differences at frequencies where plane waves produce none — ch. 53
  475. Cone of confusion makes time and level cues ambiguous for elevation — ch. 53
  476. The auditory system continually relearns to decode pinna-imposed spectral cues. — ch. 53
  477. The ear achieves spatial hearing through signal analysis rather than directional receptors — ch. 54
  478. Spectral-cue adaptation in hearing requires visible sound sources as a reference — ch. 54
  479. Synchronized visual motion captures perceived sound direction within 30 degrees — ch. 54
  480. Single-ear listeners can still localize sound sources but with degraded accuracy — ch. 54
  481. Sound width perception depends on signal type, not physical source size — ch. 54
  482. Humans adapt to a room’s spatial cues through learning over hundreds of trials — ch. 54
  483. Two identical sounds within 30–40 ms are fused into one located auditory event. — ch. 54
  484. Delayed identical sounds merge spatially until delays exceed 30-40 ms — ch. 54
  485. Dynamic auditory cues can override clear visual evidence of source location — ch. 54
  486. Evolution shaped localization to favor broadband transient sounds like movement — ch. 54
  487. Neural refractory periods after strong onsets disable directional hearing for delayed sounds — ch. 54
  488. The precedence effect suppresses spatial identity of reflections, not their audibility — ch. 54
  489. Sound localization blur is smallest in front and largest at the sides — ch. 54
  490. Sound localization fuses independent sensory evidence into one coherent percept — ch. 54
  491. Headphone audio internalizes because static binaural cues signal an inside-the-head source — ch. 54
  492. Dynamic binaural head-movement cues override conflicting visual evidence of source location — ch. 54
  493. Binaural listening yields a 5-7 dB intelligibility advantage over monaural — ch. 54
  494. Speech elements near masked threshold carry intelligibility only under binaural listening. — ch. 54
  495. Binaural listening yields only 5–7 dB advantage over monaural spatially-separated sources — ch. 54
  496. Separate sensory modalities fuse into one coherent perception unless cues conflict — ch. 54
  497. Anti-phase signals vs diotic noise yield 18 dB binaural detection advantage around 200-300 Hz — ch. 55
  498. Hearing evolved as an omnidirectional alarm system complementing directional vision — ch. 55
  499. Instantaneous interaural level differences improve intelligibility beyond better-ear listening alone — ch. 55
  500. The auditory system cancels room coloration to recover source signals — ch. 55
  501. Perceived auditory distance has an acoustic horizon under 10 meters — ch. 55
  502. Binaural listening gives 0 to 8 dB advantage in multi-talker conditions — ch. 55
  503. Listeners perceptually subtract room coloration from source signals, called binaural decolouration. — ch. 55
  504. More reverberation relative to direct sound makes listeners judge a source as farther away. — ch. 55
  505. Perceived auditory distance follows a compressive power function of actual distance — ch. 56
  506. Auditory models that extract distance cues from ear signals remain an open research direction — ch. 56
  507. Reverberator pre-delay controls perceived source distance independently of loudness ratio — ch. 56
  508. The auditory system compensates for room acoustics to recover the original source signal — ch. 56
  509. Exaggerated interaural level differences signal that a sound source is near — ch. 56
  510. Auditory distance localization error varies dramatically across studies. — ch. 56
  511. DFT-based psychoacoustic models derive an auditory excitation spectrum on the ERB scale — ch. 57
  512. Frequency masking is modelled as convolution with a spreading function — ch. 57
  513. Real-time auditory models enable speech recognition, sound reproduction, and hearing aids — ch. 57
  514. A complete mathematical model of the entire auditory system will never exist — ch. 57
  515. Auditory spectra smooth harmonic detail while preserving formant structure — ch. 57
  516. Hearing sensitivity to frequency can be emulated by filtering and weighting short-time power spectra — ch. 57
  517. Computational auditory modelling began only in the 1960s — ch. 57
  518. Psychoacoustic models explain experimental results without addressing physiology — ch. 57
  519. Hearing acts as a spectral analyser extracting quantifiable perceptual metrics from sound — ch. 57
  520. Gammatone filter banks model human auditory filtering using measured nerve responses — ch. 60
  521. Combining DRNL paths produces a double impulse that loses temporal fine structure — ch. 60
  522. Middle ear acts as a band-pass filter attenuating 6 dB per octave — ch. 60
  523. Gammatone filters fail on level-dependence and fast-onset sounds — ch. 60
  524. Filter bank models outperform DFT in mimicking auditory temporal resolution — ch. 60
  525. Pitch perception can be modeled by autocorrelation across auditory filter bands — ch. 61
  526. Adaptation, temporal integration, and post-masking can be simulated by one combined feedback element. — ch. 61
  527. Hair-cell adaptation to sound arises from neurotransmitter pool depletion and recycling dynamics — ch. 61
  528. Neurotransmitter loss in the synaptic cleft produces auditory adaptation. — ch. 61
  529. The cochlear amplifier requires nonlinear, level-dependent elements to model. — ch. 61
  530. Different hearing tasks exploit different model time constants. — ch. 61
  531. A single auditory nerve fibre’s firing is unpredictable and noisy — ch. 61
  532. Auditory nerve adaptation operates like automatic gain control. — ch. 61
  533. Functional and physiological modeling approaches divide along intended use. — ch. 61
  534. Clean auditory sensation emerges only from pooling many noisy nerve fibres — ch. 61
  535. A single feedback process yields complementary onset-emphasis and loudness-integration outputs. — ch. 61
  536. Cochlear modelling faces a tradeoff between spatial accuracy and computational cost — ch. 61
  537. Loudness models need 100-200 ms time constants to capture temporal integration and post-masking. — ch. 61
  538. Auditory adaptation acts like high-pass filtering that emphasizes stimulus onsets. — ch. 61
  539. Pitch perception is encoded by the timing of neural firing in the cochlea — ch. 61
  540. Cascade AGC loops compress steady signals logarithmically while amplifying onsets. — ch. 61
  541. Robust spatial hearing despite reverberation has driven decades of binaural modeling research. — ch. 62
  542. Jeffress coincidence detection explains how neurons encode interaural time differences. — ch. 62
  543. Autocorrelation models explain pitch and can separate concurrent vowel sounds differing in fundamental frequency — ch. 62
  544. Two competing loudness models predict time-variant loudness by peak tracking or frame averaging — ch. 62
  545. Interaural time differences are computed by cross-correlating the two ear signals — ch. 62
  546. The IACC maximum value estimates interaural coherence between the two ear signals — ch. 62
  547. Count-comparison and coincidence-detection models imply different brain receptive-field architectures for direction coding. — ch. 63
  548. Neural networks trained on single-subject data can accurately model human elevation localization — ch. 63
  549. Equalization-cancellation subtracts masker signals to reveal hidden targets — ch. 63
  550. Cross-correlation sidelobes near 1 kHz stem from interaural phase ambiguities — ch. 63
  551. High-frequency auditory analysis preserves only the temporal envelope of signals — ch. 63
  552. Binaural unmasking can be modelled as equalizing then subtracting two ear signals — ch. 63
  553. Auditory modelling accuracy trades off sharply against computational cost — ch. 63
  554. Two brain models differ on whether localization uses narrow or wide receptive fields — ch. 63
  555. Close-miked mono reproduction stays clear because the room barely affects the signal — ch. 64
  556. Visual color affects perceived loudness of the same sound — ch. 64
  557. Spaced mics sound warm and ambient because incoherent signals exceed loudspeaker angle. — ch. 64
  558. Audio quality improvements mask video defects, but video quality does not mask audio defects. — ch. 64
  559. The ORTF technique blends coincident and spaced microphone characteristics — ch. 64
  560. Required audio fidelity scales with the application’s communicative demands — ch. 64
  561. First-order Ambisonics reproduction is restricted to three loudspeakers — ch. 64
  562. Authentic sound reproduction is judged by perceptual identity, not signal fidelity — ch. 64
  563. The listening experience intended by engineers is what gets conveyed, not raw sound — ch. 64
  564. Human hearing adapts to different room acoustics to preserve timbre perception — ch. 64
  565. Cinema has historically pioneered new audio reproduction formats before home use. — ch. 64
  566. Three-dimensional VBAP extends pair panning to position sources on loudspeaker triangles — ch. 64
  567. Sound reproduction’s unifying trait is its endpoint in the human listener — ch. 64
  568. Sound within one critical band is perceived as a single source — ch. 64
  569. Stereophonic two-channel reproduction became widespread after the two-channel record format arrived. — ch. 64
  570. Cinema 5.1 surround sound originated in 1976 and reached homes in the late 1990s. — ch. 64
  571. Audio engineering is the production of meaningful sound signals across media. — ch. 64
  572. Loudspeaker signals can be computed as virtual microphone signals with first-order directional patterns. — ch. 64
  573. Panning between non-symmetric loudspeaker pairs distorts perceived spatial width. — ch. 64
  574. Human audio-visual synchronicity tolerance is asymmetric because sound naturally lags light. — ch. 64
  575. Mono reproduction exaggerates recording-room coloration that stereo cancels — ch. 64
  576. Object-based audio decouples soundtracks from specific loudspeaker layouts — ch. 64
  577. Tactile vibration raises perceived loudness and lowers preferred bass levels — ch. 64
  578. Tactile frequency discrimination is crude, often off by an octave — ch. 64
  579. Quadraphonic sound failed due to delivery problems and too few speakers. — ch. 64
  580. Directional coincident microphones suppress room reverberation, killing sense of space — ch. 64
  581. Recorded audio is engineered for plausibility, not faithful reproduction of reality — ch. 64
  582. Listening room specifications exist to make psychoacoustic test results comparable across sites — ch. 64
  583. Spherical harmonics act as basis functions for building any microphone pattern — ch. 64
  584. Audio production divides into recording, mixing, mastering, and live sound stages — ch. 64
  585. Instrument directionality shapes the captured spectrum depending on mic placement — ch. 64
  586. Auditory-tactile systems improve music reproduction quality and enable tactile feedback. — ch. 64
  587. Spot miking captures each instrument with its own near microphone for independent channels — ch. 64
  588. Standard Ambisonics microphones use four capsules to capture omnidirectional and three-dipole signals. — ch. 64
  589. VBAP predicts perceived source azimuth accurately but not personal elevation — ch. 64
  590. Physical accuracy of a sound field does not predict perceived accuracy — ch. 64
  591. Surround recordings pair spaced mics one-to-one with each loudspeaker — ch. 64
  592. Gain ratios alone cause loudness shifts; sum-of-squares normalization prevents them — ch. 64
  593. Tactile-audio desynchrony is as critical as audiovisual desynchrony — ch. 64
  594. The Blumlein XY pair captures reverberance fully but causes phase artefacts from side sound. — ch. 64
  595. Room reverberation suppresses the comb-filter colouring of amplitude panning — ch. 64
  596. Amplitude panning creates auditory objects with no real physical source — ch. 64
  597. Room acoustics smear directional perception and mask recorded reverberation — ch. 64
  598. No single ideal listening room acoustic exists because humans adapt to room differences — ch. 64
  599. DirAC divides captured sound into diffuse and non-diffuse streams — ch. 64
  600. DirAC reproduction quality depends on one dominant source per frequency band — ch. 64
  601. FFT block convolution trades speed for double-block latency in reverbs — ch. 65
  602. Headphone and loudspeaker playback of stereo differ yet yield similar spatial order. — ch. 65
  603. Stereo loudspeakers create directional illusion through summed phase shifts mimicking time delays — ch. 65
  604. Nonlinear spatial analysis distributes measured impulse responses across loudspeaker arrangements — ch. 65
  605. Uncorrelated noise from surround speakers creates enveloping source perception. — ch. 65
  606. Crosstalk-cancelled playback yields externalized sound only in the frontal hemisphere — ch. 65
  607. Each person’s unique pinna and head shape undermines binaural recordings for other listeners — ch. 65
  608. Regularization trades inversion accuracy against loudspeaker dynamic-range demands — ch. 65
  609. Sound field control can deliver different audio to different zones of a room. — ch. 65
  610. Computed room impulse responses often sound unnatural in the late reverberant tail — ch. 65
  611. Microphone directivity shapes how reverberant a convolved signal sounds — ch. 65
  612. Shoulder reflections imprint identifiable arcs on measured head-related impulse responses. — ch. 65
  613. Headphone binaural reproduction fails without dynamic head-movement cues — ch. 65
  614. Binaural audio reproduces ear canal signals from real or virtual scenarios. — ch. 65
  615. Interaural level differences only emerge at frequencies above roughly 400 Hz. — ch. 65
  616. Wave field synthesis is nearly always generated synthetically, not from real recordings. — ch. 65
  617. DIY in-ear binaural recording yields convincing spatial reproduction — ch. 65
  618. Sound source location is encoded in waveform distortions between the ears — ch. 65
  619. HRTFs can virtualize multi-channel loudspeaker layouts on headphones. — ch. 65
  620. Head-tracked HRTF filtering restores realistic external sound localization — ch. 65
  621. Inverted-polarity (antiphasic) stereo signals cancel lows and smear image — ch. 65
  622. Compression, limiting, and expansion attenuate or boost audio differently by amplitude. — ch. 65
  623. Phase-based localization sensing has a hard frequency ceiling near 1.6 kHz — ch. 65
  624. Wave field synthesis needs loudspeakers spaced at most half a wavelength apart. — ch. 65
  625. Time-frequency modulation and amplitude modulation are distinct operations — ch. 66
  626. MDCT exploits inter-frame aliasing cancellation to achieve critical sampling — ch. 66
  627. Frequency-domain processing enables efficient audio coding for monophonic and multichannel signals — ch. 66
  628. Non-redundant time-frequency transforms introduce aliasing artifacts when signals are modified in the frequency domain. — ch. 66
  629. MDCT excels for coding but lacks robustness to time-frequency domain edits — ch. 66
  630. Stereo signals can be processed for headphones to recreate natural binaural sound fields — ch. 66
  631. Each STFT sample represents a circularly continuous tone — ch. 66
  632. Modifying STFT bins creates edge transients that synthesis windows imperfectly suppress — ch. 66
  633. Modifying frame gains in overlap-add processing reveals previously cancelled aliasing artifacts as audible distortion. — ch. 66
  634. The ear’s 1-2 ms time resolution makes monaural temporal cues unusable for localization. — ch. 66
  635. Decorrelators degrade audio quality on transient-rich signals like applause. — ch. 66
  636. Time–frequency audio processing exploits the ear’s own spectral analysis structure — ch. 66
  637. Decorrelation enables creating independent channels while preserving perceptual quality. — ch. 66
  638. Audio analysis bands can follow perceptual scales while processing stays on full-resolution QMF bands. — ch. 66
  639. Head and pinna scattering imprint direction-dependent spectral notches onto the ear signal. — ch. 66
  640. Human spatial resolution limits make stereo-to-multichannel upmixing perceptually plausible. — ch. 66
  641. Spatial audio is synthesized by controlling band energies and inter-channel interdependencies. — ch. 66
  642. Downsampled filter banks enable efficient DSP implementations like FFT for DFT. — ch. 66
  643. Fixed-width filter bands mismatch hearing’s finer low-frequency resolution — ch. 66
  644. Audio coders prefer critically sampled filter banks for minimal data transmission. — ch. 66
  645. Modern synthetic voices learn from single-speaker speech databases rather than hand-crafted phonetic rules. — ch. 67
  646. Synthetic speech dates to late-18th-century acoustic-mechanical machines — ch. 67
  647. Speech coding is the most mature speech technology because it needs no databases. — ch. 67
  648. Auditory elevation calibration requires visual confirmation of sound sources — ch. 67
  649. Data-based speech synthesis splits into sample-reassembly and parameter-model approaches. — ch. 67
  650. Logarithmic quantization suits speech but distorts music beyond tolerance — ch. 67
  651. Rule-based speech synthesis survives only where computational power is scarce. — ch. 67
  652. The hardest part of speech-to-speech translation is language processing, not signal processing. — ch. 67
  653. Wideband speech coding spans 50 Hz to 7000 Hz for brighter fuller quality — ch. 67
  654. Bandwidth extension and error concealment are speech-enhancement techniques for missing or narrow data. — ch. 67
  655. Source-filter parametric synthesis enables voice modification that unit-selection cannot. — ch. 67
  656. Mobile phone codecs adapt their bit rate across eight levels to optimize call quality — ch. 67
  657. The 1930s vocoder pioneered reducing speech to slowly-varying parameters to cut bandwidth — ch. 67
  658. Language knowledge beyond acoustics is required for automatic speech recognition. — ch. 67
  659. The telephone band of 300-3400 Hz remains the standard compromise for speech intelligibility. — ch. 67
  660. Head movements resolve front-back ambiguity by creating direction-specific binaural cue changes — ch. 67
  661. Spatial hearing is worst near 1.7 kHz where head wavelength matches. — ch. 67
  662. Speech synthesis selects units by minimizing target and concatenation costs. — ch. 67
  663. Humans localize single sources well but fail at source distributions — ch. 67
  664. Speech coding is fundamentally a quality-versus-bitrate optimization tradeoff. — ch. 67
  665. Human speech evolved as a robust channel tolerant to high background noise — ch. 67
  666. High-quality synthesized speech requires tens of hours of manually-segmented recorded speech. — ch. 67
  667. Speech recognition shifted from time warping and shallow nets to HMMs then deep networks — ch. 67
  668. Synthesis and recognition demand language knowledge databases that coding does not. — ch. 67
  669. Reverberation low-pass filters speech modulation while noise raises its floor — ch. 68
  670. PAQM estimates audible quality degradation by comparing specific loudness across critical bands. — ch. 68
  671. Squaring the pressure signal makes noise and reverberation measurable on a common scale — ch. 68
  672. Spatial audio synthesis quality is measurable against a real-source reference. — ch. 68
  673. Auditory-model quality metrics fail on acoustically captured signals — ch. 68
  674. Binaural auditory models cannot yet explain human perception of complex spatial audio — ch. 68
  675. Perceptual auditory models will eventually replace traditional audio metrics — ch. 68
  676. Musical instrument design evolved as early product sound quality experimentation — ch. 68
  677. Hearing damage begins after long exposure above 85 dB — ch. 68
  678. Noise engineering now targets annoyance and quality, not just hearing loss — ch. 68
  679. The transmission channel changes from acoustic path to electrical system in device-mediated speech. — ch. 68
  680. Quality and impairment are measured with distinct MOS variants. — ch. 68
  681. Sound quality means judged preferability, not category membership — ch. 68
  682. The public’s subjective opinion is the final truth on sound quality — ch. 68
  683. Unlike the eye, the ear has no primary directional sensitivity — ch. 68
  684. Timbral quality dominates perceived sound quality over spatial reproduction — ch. 68
  685. Digital audio coding made perceptual modeling central to audio engineering — ch. 68
  686. Commercial telephone bandwidth standards derive from interwar human listening tests — ch. 68
  687. MUSHRA only yields reliable results when sample differences are easily perceptible — ch. 68
  688. Human auditory memory cannot compare sounds separated by more than a few seconds — ch. 68
  689. Audio quality bottlenecks shifted from storage to transducers — ch. 68
  690. Computational sound quality models are trained on subjective listening data — ch. 68
  691. Binaural intelligibility level difference measures speech unmasking benefit — ch. 68
  692. Comparative MOS ratings allow a test sound to score above the reference. — ch. 68
  693. Human auditory adaptation neutralizes room acoustics but not device imperfections — ch. 68
  694. PEAQ uses a trained neural-network cognitive model to predict human MOS ratings. — ch. 68
  695. Objective sound quality models have limited domains of validity and cannot replace subjective testing — ch. 68
  696. Sound quality cannot be assessed except through psychophysical experiments with human subjects — ch. 68
  697. Multi-stimulus quality tests fail when samples vary in several perceptual dimensions at once — ch. 68
  698. Speech transmission quality hinges on undistorted information transfer — ch. 68
  699. Speech intelligibility measures the proportion of correctly identified transmitted messages — ch. 68
  700. Beyond intelligibility, telephony must preserve speaker recognizability — ch. 68
  701. Speech intelligibility in public spaces is a regulated engineering requirement — ch. 68
  702. MTF measurement uses amplitude-modulated noise bands across 0.63 to 12.5 Hz — ch. 69
  703. Speech intelligibility metrics can be predicted from impulse response and noise — ch. 69
  704. Speech intelligibility estimates compress 98 MTF values into one index — ch. 69
  705. Reverberation time maps directly onto equivalent signal-to-noise ratio — ch. 70
  706. All sound quality judgments derive from properties of the human auditory system. — ch. 71
  707. Telecom device sound quality depends on network, room, and feedback conditions jointly — ch. 71
  708. Concert hall acoustics shape the music composed for them — ch. 71
  709. PESQ works as a signal-difference device rather than a true auditory model — ch. 71
  710. Annoyance and disturbance refer to distinct degrees of noise harm — ch. 71
  711. STI reliability is judged against its 0.15 category step size — ch. 71
  712. Every sounding product is continuously evaluated for sound quality — ch. 71
  713. Consumer devices are engineered to sound masculine and powerful, not merely quiet. — ch. 71
  714. Concert hall quality is codified into standardized subjective attribute vocabularies — ch. 71
  715. Industry relies on objective methods because exhaustive listening tests are impractical — ch. 71
  716. EQUEST injects temporal masking knowledge into echo annoyance estimation — ch. 71
  717. Echo delay thresholds produce distinct perceptual and speaking effects — ch. 71
  718. Noise suppression algorithms can degrade speech quality in non-stationary noise — ch. 71
  719. The first objective speech quality measure failed on mobile-network timing variations — ch. 71
  720. Standardized concert hall acoustics metrics have known technical limitations compared to human perception — ch. 71
  721. Entering a car generates designed auditory-tactile impressions of finishing quality — ch. 71
  722. Sound perception is shaped by the listener’s expectations and context of use — ch. 71
  723. Computational simulation is the best method to model the auditory system’s function — ch. 71
  724. Speech intelligibility harms open-plan office quality, unlike in auditoria — ch. 71
  725. Speech redundancy masks up to 30 percent consonant loss in auditoriums — ch. 71
  726. MFCCs remain the dominant feature representation for speech recognition systems — ch. 71
  727. Any sound can function as noise depending on the listener — ch. 71
  728. Objective models of subjective annoyance remain limited to specific noise types — ch. 71
  729. Auditory spectrum computation begins with FFT then emulates hearing sensitivity via filtering and weighting. — ch. 71
  730. VoIP call delays exceed those of regular mobile calls — ch. 71
  731. Speech quality can be predicted algorithmically using signals that mimic human auditory processing. — ch. 71
  732. Sharpness, roughness, and narrowband temporal components increase noise annoyance — ch. 71
  733. Excitation spread across frequency bands is modelled as convolution with a level-dependent spreading function. — ch. 71
  734. Reverberation time is the key design variable separating concert hall types — ch. 71
  735. Speech intelligibility alone cannot capture loss of speaker identity in codecs — ch. 71
  736. Spatially broad sound sources should alter their perceived extent with listener distance — ch. 72
  737. MIR metadata is largely assigned by expert listeners, motivating automation as music creation accelerates — ch. 72
  738. Computational auditory scene analysis targets human-level performance without imitating the ear — ch. 72
  739. Music databases need automatic high-level content querying beyond raw audio signals. — ch. 72
  740. Sound design in interfaces is an extension of product sound quality — ch. 72
  741. Interactive game audio requires dynamic rendering systems beyond traditional linear production. — ch. 72
  742. Auditory displays deliver computer information to humans through sonification and earcons — ch. 72
  743. Virtual sound source distance is limited by reproduction technology, not perception — ch. 72
  744. Music information retrieval serves both casual listeners and music professionals needing structured database queries — ch. 72
  745. Sonic interaction design studies sound perception in active embodied contexts rather than passive listening — ch. 72
  746. Image-source room acoustics modelling becomes computationally costly in interactive VR — ch. 72
  747. CASA aims to extract all perceivable information from ear canal signals. — ch. 72
  748. Virtual audio engines render sounds based on avatar position, not just a fixed mix. — ch. 72
  749. Blind source separation becomes very difficult when sources exceed microphones — ch. 72
  750. Interactive rendering differs from reproduction because user actions alter the sound. — ch. 72
  751. Source directivity is usually omitted from virtual audio for computational reasons — ch. 72
  752. Speech intelligibility is the standard criterion for hearing function — ch. 73
  753. Sensation level expresses tone level relative to one individual’s own threshold — ch. 73
  754. Untreated hearing loss in children was once misdiagnosed as intellectual disability — ch. 73
  755. Substantial hearing loss reduces ability to react to sonic warnings — ch. 73
  756. PLP coefficients describe speech spectral features compactly and speaker-independently — ch. 73
  757. Microprocessor electronics made cochlear implants possible — ch. 73
  758. Hearing impairment degrades sensitivity, discrimination, and can cause hyperacusis or tinnitus — ch. 73
  759. The 0 dB HL audiometric zero varies across frequency by design — ch. 73
  760. Excess noise damages cochlear hair cells through several distinct mechanisms — ch. 73
  761. Deaf, hard-of-hearing, and deafened denote distinct functional categories — ch. 73
  762. Outer hair cell damage compresses dynamic range, causing recruitment and distorted loudness perception — ch. 73
  763. Hearing’s temporal resolution varies from 1-2 ms depending on frequency — ch. 74
  764. Recruitment makes loudness grow faster in impaired ears than normal ears. — ch. 74
  765. Individual HRTF measurements give the most accurate external ear emulation — ch. 74
  766. Cochlear hydrodynamics can be simulated by analog electrical equivalent circuits — ch. 75
  767. Noise damage creates a 4-kHz notch while aging affects high frequencies — ch. 75
  768. Higher-level hearing models rely on assumptions tested only against psychoacoustic data — ch. 75
  769. Outer hair cell damage destroys the cocktail party effect — ch. 75
  770. Hearing loss varies independently across different frequency ranges — ch. 75
  771. Adaptation, temporal integration, and post-masking can be simulated in a single auditory element. — ch. 75
  772. Basilar membrane models range from transmission-line equivalent circuits to finite element methods — ch. 75
  773. Brief unprotected noise exposure during otherwise protected periods raises hearing loss risk — ch. 76
  774. Even moderate 70 dB sound causes temporary hearing threshold shift with hours of exposure — ch. 76
  775. Hearing aids are miniature signal-processing sound systems that must secure adequate signal-to-noise ratio — ch. 76
  776. Outer hair cell damage widens critical bands and worsens speech-in-noise — ch. 76
  777. Tinnitus can arise from unstable outer hair cell oscillation in the cochlea — ch. 76
  778. Estimated ITDs match theoretical values especially at low frequencies — ch. 76
  779. Recovery from temporary hearing shift takes roughly double the exposure time — ch. 76
  780. Eardrum and middle ear status can be measured objectively via acoustic impedance — ch. 76
  781. Adult cochlear implant success depends on prior experience with sound — ch. 76
  782. Binaural hearing aid processing preserves spatial cues that monaural processing distorts — ch. 76
  783. Outer hair cells provide active frequency-selective amplification in the cochlea — ch. 76
  784. Tinnitus is treated by masking or habituation, not cured — ch. 76
  785. Otoacoustic emissions objectively reveal auditory system functioning and defect location — ch. 76
  786. Automatic gain control compresses sound to fit impaired hearing’s reduced dynamic range. — ch. 76
  787. Pressure differences across the eardrum attenuate low-frequency sound and cause pain — ch. 76
  788. Speech audiometry tests intelligibility by varying signal level and speech pace — ch. 76
  789. Noise control should prioritize source reduction then path attenuation before personal protection — ch. 76
  790. Combining compression with a limiter reduces distortion better than a limiter alone. — ch. 76
  791. Hearing-aid users and small children require loudspeaker-based audiometry for accurate coupling — ch. 76
  792. Bone conduction through the skull shapes how one hears one’s own voice — ch. 76
  793. A healthy cochlea emits new frequencies when stimulated by two tones — ch. 76
  794. Adaptive filters cancel hearing aid whistling caused by earphone-microphone feedback — ch. 76
  795. Post-noise tinnitus and distortion signal auditory overload and hearing-loss risk — ch. 76
  796. Low-frequency attenuation depends critically on proper seal and construction — ch. 76
  797. Most modern cochlear implant patients achieve telephone conversation ability — ch. 76
  798. Single loud impulses can instantly tear the eardrum or break ossicles — ch. 76
  799. Speech processing can fail independently of general hearing ability — ch. 76
  800. Subtractive microphone designs produce cardioid and dipole patterns via port spacing and delay — ch. 76
  801. Cochlear implants bypass the conductive auditory path to stimulate nerve fibers directly — ch. 76
  802. Pure-tone audiometry measures hearing thresholds at six standard frequencies — ch. 76
  803. Beamforming combines multiple microphone signals into directive beams — ch. 76
  804. Single-channel noise reduction exploits speech’s temporal, spectral, and statistical properties — ch. 76
  805. Hearing-loss risk threshold should drop from 85 to 75 dB for full protection — ch. 76
  806. Hearing-loss risk dominates noise research because it is predictable from sound properties — ch. 76
  807. Tinnitus can originate from blood pressure changes in the ear — ch. 76
  808. Noise is the most common cause of work-related impairments — ch. 76
  809. Comparing bone- and air-conduction thresholds distinguishes conductive from sensorineural hearing loss — ch. 76
  810. Hearing impairment degrades signal-to-noise tolerance more than quiet speech perception. — ch. 76

Annotation Roundup

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