Titlebook: Sound in the Time Domain; Mikio Tohyama Book 2018 Springer Nature Singapore Pte Ltd. 2018 Binaural Listening.Chaotic Reverberation Sound.I

NATTY

Transfer Functions and Sequences in the Time Domain,eristics by introducing the notion of poles and zeros of a complex function. Phase responses are crucial in establishing the time delay sequences representing the impulse responses. Accumulated phase functions (continuous phase functions of the angular frequency) are defined by integration of the gr

附錄

OTTER

絕緣

Wave Equation and Its General Solution in the Time Domain,ne-dimensional wave equation or plane waves may be formulated from point of view of the linear system theory using the convolution of the impulse responses and virtual sources converted from the initial excitation. These plane wave solutions may be extended to spherically symmetric waves following t

interior

作嘔

Reverberation in Rooms,for the sound energy and amplitude distributions in a room indicating that the sound field is no longer uniform. Reverberation decay curves and modulation transfer functions can be derived from the impulse responses at observation points in a room assuming white noise as a source signal. Reverberati

FICE

Signal Dynamics and Sound Source Distance,reas reverberation sounds convey the sound-path information in a room. The energy ratio of the two components is a function of the distance between the source and receiving positions, and it is an important parameter in establishing auditory events in room acoustics. This chapter develops the charac

Ophthalmologist

緩解

1860-4862 intuitively understandable description of various acoustic t.This book addresses the nature of sound, focusing on the characteristics of sound waves in the context of time structures. This time domain approach provides an informative and intuitively understandable description of various acoustic top

使激動(dòng)

Time and Frequency Responses of Spherical Source,ing both the magnitude and phase of the transfer function. The Fourier transform of the impedance function renders the transient response of the source to an impulsive excitation in the time domain. The impulse response of a loudspeaker system may be interpreted as a representation of radiation impedance functions in the time domain.