Tones (Sounds) Loudness Surface: the Weber' Law for Hearing

International Conference on Circuits and Systems (CAS 2015) Tones (Sounds) Loudness Surface: the Weber’ Law for Hearing Ovchinnikov Evgeny L Department of Medical and Biological Physics, Samara State Medical University, Samara, Russia Abstract—Purpose: Research and theoretical substantiation of In practice, the tone's loudness as a response to stimulation the hearing Weber law for sounds arbitrary frequencies and (sensation) is evaluated the decibel loudness, equating to intensities. declaratively on the standard frequency decibel intensity Objects: Results of classic psychophysical experiments of and decibel loudness, calling his phon.For arbitrary Weber, hearing Fechner model (equation) as a special case of frequencies and intensities of sound the Weber - Fechner the Weber law. law determined only experimentally and graphically is Methods: Audiometric for determining hearing acuity, displayed as the curves of equal loudness – isophon. But it biophysical for the substantiation of auditory process, methods can be shown that the differential equation represented by of mathematical analysis and computer simulation. Fechner as dЕ = k (dI/I), has a logical and a definite Results: To the analytical and graphical form is decision in the entire range of sound frequencies substantiated and submitted the hearing Weber law for arbitrary frequencies and intensities of sounds. permissible (comfortable) intensity. Experiments show that the auditory perception of a Keywords-sound (tones) loudness; loudness surface; weber’ sound, greater or smaller standard frequency, but the same law for hearing; sounds of arbitrary frequencies and intensities. loudness as the standard sound requires an increase in the intensity of the sound on the new frequency at this level. I. INTRODUCTION First let us identify the causes of this phenomenon – a Person's perception of sound energy (intensity I or nature of tones (sounds) of equal loudness. pressure P) in hearing physiology and psychophysics is B. Nature of tones (sounds) equal loudness estimated as loudness E sense and is installed by Weber – Fechner law [1, 2]. The law regulates the parity "the relative Initially, let us clarify the physical, biophysical, physiological and psychophysical meaning of the quantity sound intensity I (sound pressure Δp) with respect to the -12 2. Inf threshold intensity Io = Ioc = 10 J/(m s) (threshold sound and substantiate the possibility of its calculation. This . -5 pressure Δpoc = 2 10 Pa), .as relative strength of the Inc stimulus, and its subjective sense – tones loudness E. "This is the ratio of sounds intensities of equal loudness on n- means that the tones loudness is a psychoacoustic correlate level loudness: two sound of an arbitrary f and standard fc of hearing perception of the sound energy (sound intensity, frequency of the n-level loudness are of equal loudness sound pressure). (produce the same sense of loudness) when performed the * * Mathematical Fechner substantiation of the law for equation E nf = E nc in the receptor section of an inner ear. hearing on Weber experiments does not give a full and final The equality of loudness tones interprets an answer of equal decision and, of course, does not establish a functional link number n of sensors that are excited by stimulation, between the force and sense of irritation in the hearing manifesting itself in subjectivity of sensations. But, perception of the sound energy of arbitrary parameters. according to Weber, this equality is an objective for the quantitative ratios of energy conversion in the receptor II. STUDY RESULTS section. * * A. Problems in hearing psychophysics Sounds with intensities I nf and I nc (respectively, with * * energies W nf and W nc) will have equal loudness if they Weber – Fechner law defined in integral form only for * * will have the same irritating effect on receptors: I nf = I nc, the standard frequency fc = 1 kHz as a declarative (conditionally accepted) relations I* or, equivalently nf = 1. Introducing morphologic and * I Δp Inc Е, phon = 10 log , dB = 20 log , dB. (1) I Δp functional parameters of the cochlear duct and using the о о definition of the wave intensity, expressing its connection In the general solution of the differential equation dЕ = with energy W, we obtain k (dI/I) as the Weber – Fechner in integral form Е = 10 log(I/Io), the unit values on the right side is the decibel (dB). © 2015. The authors - Published by Atlantis Press 259 * * clearance) and the physical characteristics of sound I* W* S t nf = nf c c . (2) (velocity of dispersed waves in liquids of the cochlea). I* W* S* t* nc nc f f C. Nature of tones (sounds) equal loudness * * Here S c and S f – areas of basilar membrane which are Note that the sound intensity (pressure) set by its occupies receptors, excited by waves of an arbitrary f and definition in the environment. Entering on eardrum of the standard fc frequencies, that are proportional to the square relative energy of waves of arbitrary frequency Wnf, divided of the distance between the receptors Λs and Λf. by the energy of waves standard frequency Wns, is equal to Coordinates of the receptors distribution ℓ(N) [3, 4] along W I the relative intensity of these waves nf = nf , since the the basilar membrane of a length L , sensing a frequency o Wnc Inc f(N) at the maximum frequency of the perceived ear fmo = energy falls on one and the same surface – on the eardrum 20 kHz, are satisfied to acoustic-wave hearing model [5] ℓ(f) (S = const) and the duration of the passage of the wave f ed lg2 distance from the inlet to the external auditory canal it can . fmo = Lo 2 , where the frequency f, being a function of be considered the sme because of the small sound velocity numbers N of excited receptors on ratio f(N) = fmo dispersion of in air. 1 Nmo −2 Nmo This conversion takes place under the law of lg lg conservation and transformation of energy. The law, in the 2lg + f(NN a ) . 2lg + f(NN a ) 10 , gives ℓ(N) = Lo 2 . W W* Then the distances between adjacent receptors Λ(f) may be form nf = nf , leads to the relation * calculated from the obvious equation Λ(N) = ℓ(N+1)–ℓ(N) Wnc Wnc (Figure 1a). In the same ratio t* and t* is duration of passing waves W I Λ v c f nf = nf = f c = G(f). (4) of compared frequencies clearance h between vestibular and W I Λ v tectorial membrane (transfer of energy). This value (in the nc nc c f axial duct profile) is not experimentally determined. We can This means that a sense of sound at a frequency assume that clearance is constant over the entire length of different from the standard requires great energy, which is the cochlear duct (with the possible exception of small areas caused by an significant increase distances between at ends it). The result is greatly simplified by assuming that receptors Λf with varying frequency. Perhaps this is due to the lumen is inversely proportional to the distances between the greater volume of intra-labyrinth liquid above receptors, t* v which must vibrate for a physiological sensation of sound. c vh cc Λf f the receptors. Then = = , where vf and The value G(f) acquires a meaning of the t* vh Λ v f ff c c psychophysical frequency equivalent for the sounds of equal loudness (Figure 1c). Note two it features. For the vc – velocity waves of arbitrary f and standard fc frequencies, obeying dispersion in inner ear liquids equivalent we note two comments. The first comment is according acoustic-wave hearing model [5] and satisfying states that the absolute increment of the relative level of f/flog(2 ) intensity of sound with respect to the n-level for tones of + 21 mo equal loudness is the absolute increment of psychophysical the relation v(f) = ⋅ vmo , where vmo = 2 ⎛ I ⎞ ΔI 1600 m/s – the sound velocity in the perilymph with the equivalent: Δ⎜ nf ⎟ = nf = ΔG(f), that leads to the ⎜ I ⎟ I highest perceived by ear frequency fmo (Figure 1b). Finally, ⎝ nc ⎠ nc we obtain relation ΔInf = Inc ΔG(f). Last equality implies second comment - about the relative increment of the sound W* Λ v intensity in frequency by n-level, which is nf = f c = G(f). (3) * Λ v Wnc c f ⎛ ΔI ⎞ ΔI I ΔG ⎜ ⎟ = nf = nc ΔG = . Thus ratio of the energy of sound waves of arbitrary and ⎝ I ⎠n Inf Inf G standard frequencies for tones equal loudness in the inner ear directly proportional to the ratio of the distance between Now back to the Weber law for the rationale of sound the receptors and inversely proportional to the relative perception of arbitrary frequency and intensity. velocities of the partial waves in fluids of the inner ear. According to Weber, the increment of perception of Dimensionless quantity G (f) defines the ratio of the tones loudness ΔЕ is proportional to the increment of the energies of tones equal loudness: it shows how many times relative intensity of the sound (ΔI/I), i.e. ΔЕ = k(ΔI/I). But one of them must be larger than the other for sensations of increment of sound intensity ΔI is reflected by variations as tones of equal loudness, and can serve as a criterion of in energy (intensity level) ΔIL, and in frequency ΔIf, and tones equal loudness, but varying pitch. Its special feature is generally represents the sum to determine through parameters of inner ear (the distances between the auditory receptors and the endolymphatic duct 260 Еnf = Еmo, and Emo = Enc (for tones of equal loudness) and log(Imo/Ioc)= Lmo = Emo (for declarative agreement) and Inc log log(Inc/Ioc) = Lnc = L, leads to the fact that Еnc = Ioc a b c Imo k f k f k f lg + lg Gmo = Lmo + lg Gmo, = (L – Ioc elg elg elg 1 Lmo) , and E = L + (Lnc – Lmo) or Glg mo I ⎛ I I ⎞ d Е = log + ⎜log − log mo ⎟ Glog = ⎜ ⎟ Ioc ⎝ Ioc Ioc ⎠ Glog mo Figure 1.

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