Analysis and Synthesis of Expressive Guitar Performance

Total Page:16

File Type:pdf, Size:1020Kb

Analysis and Synthesis of Expressive Guitar Performance Analysis and Synthesis of Expressive Guitar Performance AThesis Submitted to the Faculty of Drexel University by Raymond Vincent Migneco in partial fulfillment of the requirements for the degree of Doctor of Philosophy May 2012 c Copyright 2012 Raymond Vincent Migneco. All Rights Reserved. ii Table of Contents ListofTables........................................... vi ListofFigures .......................................... vii Abstract.............................................. xi 1 INTRODUCTION ..................................... 1 1.1 Contributions........................................ 3 1.2 Overview .......................................... 4 2 COMPUTATIONAL GUITAR MODELING . 6 2.1 SoundModelingandSynthesisTechniques. 6 2.1.1 WavetableSynthesis .................................. 6 2.1.2 FMSynthesis...................................... 7 2.1.3 AdditiveSynthesis ................................... 8 2.1.4 Source-FilterModeling................................. 8 2.1.5 PhysicalModeling ................................... 9 2.2 Summary and Model Recommendation . 10 2.3 SynthesisApplications ................................... 12 2.3.1 SynthesisEngines ................................... 12 2.3.2 Description and Transmission . 12 2.3.3 New Music Interfaces . 13 3 PHYSICALLY INSPIRED GUITAR MODELING . 14 3.1 Overview .......................................... 14 3.2 WaveguideModeling .................................... 14 3.2.1 Solution for the Ideal, Plucked-String . 15 3.2.2 Digital Implementation of the Wave Solution . 15 3.2.3 Lossy Waveguide Model . 17 3.2.4 Waveguide Boundary Conditions . 18 iii 3.2.5 ExtensionstotheWaveguideModel . 20 3.3 Analysis and Synthesis Using Source-Filter Approximations . 21 3.3.1 Relation to the Karplus-Strong Model . 22 3.3.2 Plucked String Synthesis as a Source-Filter Interaction . 22 3.3.3 SDL Components . 23 3.3.4 Excitation and Body Modeling via Commuted Synthesis . 25 3.3.5 SDL Loop Filter Estimation . 27 3.4 ExtensionstotheSDLModel ............................... 31 4 SOURCE-FILTERPARAMETERESTIMATION . 32 4.1 Overview .......................................... 32 4.2 Background on Expressive Guitar Modeling . 32 4.3 Excitation Analysis . 33 4.3.1 Experiment: Expressive Variation on a Single Note . 34 4.3.2 Physicality of the SDL Excitation Signal . 36 4.3.3 Parametric Excitation Model . 38 4.4 Joint Source-Filter Estimation . 38 4.4.1 Error Minimization . 38 4.4.2 Convex Optimization . 40 5 SYSTEMFORPARAMETERESTIMATION. 43 5.1 Onset Localization . 43 5.1.1 Coarse Onset Detection . 44 5.1.2 Pitch Estimation . 45 5.1.3 Pitch Synchronous Onset Detection . 46 5.1.4 Locating the Incident and Reflected Pulse . 48 5.2 Experiment1 ........................................ 49 5.2.1 Formulation . 49 5.2.2 Problem Solution . 52 5.2.3 Results ......................................... 53 5.3 Experiment2 ........................................ 58 iv 5.3.1 Formulation . 58 5.3.2 Problem Solution . 59 5.3.3 Results ......................................... 61 5.4 Discussion.......................................... 62 6 EXCITATIONMODELING ................................ 63 6.1 Overview .......................................... 63 6.2 Previous Work on Guitar Source Signal Modeling . 64 6.3 Data Collection Overview . 66 6.3.1 Approach . 67 6.4 Excitation Signal Recovery . 68 6.4.1 Pitch Estimation and Resampling . 69 6.4.2 Residual Extraction . 69 6.4.3 Spectral Bias from Plucking Point Location . 70 6.4.4 Estimating the Plucking Point Location . 71 6.4.5 Equalization: Removing the Spectral Bias . 74 6.4.6 Residual Alignment . 76 6.5 Component-based Analysis of Excitation Signals . 77 6.5.1 Analysis of Recovered Excitation Signals . 77 6.5.2 Towards an Excitation Codebook . 78 6.5.3 Application of Principal Components Analysis . 79 6.5.4 Analysis of PC Weights and Basis Vectors . 81 6.5.5 Codebook Design . 84 6.5.6 Codebook Evaluation and Synthesis . 85 6.6 Nonlinear PCA for Expressive Guitar Synthesis . 88 6.6.1 Nonlinear Dimensionality Reduction . 89 6.6.2 Application to Guitar Data . 90 6.6.3 Expressive Control Interface . 92 6.7 Discussion.......................................... 94 7 CONCLUSIONS . 95 v 7.1 ExpressiveLimitations................................... 96 7.2 Physical Limitations . 97 7.3 FutureDirections...................................... 98 Appendix A Overview of Fractional Delay Filters . 100 A.1 Overview .......................................... 100 A.2 The Ideal Fractional Delay Filter . 100 A.3 Approximation Using FIR Filters . 102 A.3.1 Delay Approximation using Lagrange Interpolation Filters . 103 A.4 Further Considerations . 104 AppendixB PitchGlideModeling .............................. 106 B.1 Overview .......................................... 106 B.2 PitchGlideModel ..................................... 107 B.3 PitchGlideMeasurement ................................. 107 B.4 Nonlinear Modeling and Data Fitting . 108 B.4.1 Nonlinear Least Squares Formulation . 108 B.4.2 FittingandResults .................................. 109 B.5 Implementation....................................... 110 Bibliography . 113 VITA ............................................... 119 vi List of Tables 2.1 Summary of sound synthesis models including their modeling domain and applicable audio signals. Adopted from Vercoe et al. [93]. 11 2.2 Evaluating the attributes of various sound modeling techniques. The boldface tags indicate the optimal evaluation for a particular category. 11 5.1 Mean and standard deviation of the SNR computed using Equation 5.11. The joint source-filter estimation approach was used to obtain parameters for synthesizing the guitar tones based on an IIR loop filter. 58 5.2 Mean and standard deviation of the SNR computed using Equation 5.11. The joint source-filter estimation approach was used to obtain parameters for synthesizing the guitar tones using a FIR loop filter with length N = 3. 61 B.1 Pitch glide parameters of Equation B.3 for plucked guitar tones for each guitar string. p, mf and f indicate strings excited with piano, mezzo-forte and forte dynamics, respectively. ......................................... 112 vii List of Figures 3.1 Traveling wave solution of an ideal string plucked at time t = t1 and its displacement at subsequent time instances t2,t3. The string’s displacement (solid) at any position is the summation of the two disturbances (dashed) at that position. 16 3.2 Waveguide model showing the discretized solution of an ideal, plucked string. The + upper (y ) and lower (y−) signal paths represent the right and left traveling distur- + bances, respectively. The string’s displacement is obtained by summing y and y− at adesiredspatialsample. .................................. 17 3.3 Waveguide model incorporating losses due to propagation at the spatial sampling instances. The dashed lines outline a section where M gain and delay blocks are consolidated using a linear time-invariant assumption. 18 3.4 Plucked-string waveguide model as it correlates to the physical layout of the guitar. Propagation losses and boundary conditions are lumped into digital filters located at the bridge and nut positions. The delay lines are initialized with the string’s initial displacement. ........................................ 20 3.5 Single delay-loop model (right) obtained by concatenating the two delay lines from a bidirectional waveguide model (left) at the nut position. Losses from the bridge and nut filters are consolidated into a single filter in the feedback loop. 22 3.6 Plucked string synthesis using the single delay-loop (SDL) model specified by S(z). C(z) and U(z) are comb filters simulating the e↵ects of the plucking point and pickup positions along the string, respectively. 24 3.7 Components for guitar synthesis including excitation, string and body filters. The excitation and body filter’s may be consolidated for commuted synthesis. 26 3.8 Overview of the loop filter design algorithm outlined in Section 3.3.5 using short-time Fourier transform analysis on the signal. 30 4.1 Top: Plucked guitar tones representing various string articulations by the guitarist on the open, 1st string (pitch E4, 329.63 Hz). Bottom: Excitation signals for the SDL modelassociatedwitheachpluckingstyle. 35 4.2 The output of a waveguide model is observed over one period of oscillation. The top figure in each subplot shows the position of the traveling acceleration waves at di↵erent time instances. The bottom plot traces out the measured acceleration at the bridge (notedbythe’x’inthetopplots)overtime. 37 5.1 Proposed system for jointly estimating the source-filter parameters for plucked guitar tones.............................................. 43 5.2 Pitch estimation using the autocorrelation function. The lag corresponding to the global maximum indicates the fundamental frequency for a signal with f0 = 330 Hz. 46 viii 5.3 Overview of residual onset localization in the plucked-string signal. (a): Coarse onset localization using a threshold based on spectral flux with a large frame size. (b): pitch-synchronous onset detection utilizing spectral flux threshold computed with a frame size proportional to the fundamental frequency of the string. (c): Plucked-string signal with onsets coarse and pitch-synchronous onsets overlayed. 47 5.4 Detail view of the “attack” portion of the plucked-tone signal in Figure 5.3. The pitch- synchronous onset is marked as well as the incident and reflected pulses from the first period of oscillation. 48 5.5 Pole-zero and magnitude plots of a string filter S(z)withf0
Recommended publications
  • The Science of String Instruments
    The Science of String Instruments Thomas D. Rossing Editor The Science of String Instruments Editor Thomas D. Rossing Stanford University Center for Computer Research in Music and Acoustics (CCRMA) Stanford, CA 94302-8180, USA [email protected] ISBN 978-1-4419-7109-8 e-ISBN 978-1-4419-7110-4 DOI 10.1007/978-1-4419-7110-4 Springer New York Dordrecht Heidelberg London # Springer Science+Business Media, LLC 2010 All rights reserved. This work may not be translated or copied in whole or in part without the written permission of the publisher (Springer Science+Business Media, LLC, 233 Spring Street, New York, NY 10013, USA), except for brief excerpts in connection with reviews or scholarly analysis. Use in connection with any form of information storage and retrieval, electronic adaptation, computer software, or by similar or dissimilar methodology now known or hereafter developed is forbidden. The use in this publication of trade names, trademarks, service marks, and similar terms, even if they are not identified as such, is not to be taken as an expression of opinion as to whether or not they are subject to proprietary rights. Printed on acid-free paper Springer is part of Springer ScienceþBusiness Media (www.springer.com) Contents 1 Introduction............................................................... 1 Thomas D. Rossing 2 Plucked Strings ........................................................... 11 Thomas D. Rossing 3 Guitars and Lutes ........................................................ 19 Thomas D. Rossing and Graham Caldersmith 4 Portuguese Guitar ........................................................ 47 Octavio Inacio 5 Banjo ...................................................................... 59 James Rae 6 Mandolin Family Instruments........................................... 77 David J. Cohen and Thomas D. Rossing 7 Psalteries and Zithers .................................................... 99 Andres Peekna and Thomas D.
    [Show full text]
  • Enter Title Here
    Integer-Based Wavetable Synthesis for Low-Computational Embedded Systems Ben Wright and Somsak Sukittanon University of Tennessee at Martin Department of Engineering Martin, TN USA [email protected], [email protected] Abstract— The evolution of digital music synthesis spans from discussed. Section B will discuss the mathematics explaining tried-and-true frequency modulation to string modeling with the components of the wavetables. Part II will examine the neural networks. This project begins from a wavetable basis. music theory used to derive the wavetables and the software The audio waveform was modeled as a superposition of formant implementation. Part III will cover the applied results. sinusoids at various frequencies relative to the fundamental frequency. Piano sounds were reverse-engineered to derive a B. Mathematics and Music Theory basis for the final formant structure, and used to create a Many periodic signals can be represented by a wavetable. The quality of reproduction hangs in a trade-off superposition of sinusoids, conventionally called Fourier between rich notes and sampling frequency. For low- series. Eigenfunction expansions, a superset of these, can computational systems, this calls for an approach that avoids represent solutions to partial differential equations (PDE) burdensome floating-point calculations. To speed up where Fourier series cannot. In these expansions, the calculations while preserving resolution, floating-point math was frequency of each wave (here called a formant) in the avoided entirely--all numbers involved are integral. The method was built into the Laser Piano. Along its 12-foot length are 24 superposition is a function of the properties of the string. This “keys,” each consisting of a laser aligned with a photoresistive is said merely to emphasize that the response of a plucked sensor connected to 8-bit MCU.
    [Show full text]
  • TINSLEY ELLIS - Around Memphis - Little Charlie Baty - Nine CD Reviews
    Blues Music Online Weekly Edition TINSLEY ELLIS - Around Memphis - Little Charlie Baty - Nine CD Reviews BLUES MUSIC ONLINE - March 18, 2020 - Issue 6 Table Of Contents 6 TINSLEY ELLIS Enjoying The Ride By Marc Lipkin - Alligator Records 10 TINSLEY ELLIS Red Clay Soul Man Originally Published January 2017 By Grant Britt 14 LITTLE CHARLIE BATY In Memoriam By Art Tipaldi - Thomas Cullen III 16 AROUND MEMPHIS Pandemic Effects 18 CD REVIEWS By Various Writers 29 Blues Music Store CDs Onsale COVER PHOTOGRAPHY © MARILYN STRINGER TOC PHOTOGRAPHY © MARILYN STRINGER TOC PHOTOGRAPHY © MARILYN STRINGER Tinsley Ellis Enjoying The Ride By Marc Lipkin - Alligator Records ver since he first hit the road 40 years shuffles, and it all sounds great.” The Chicago ago, blues-rock guitar virtuoso, soulful Sun-Times says, “It’s hard to overstate the Evocalist and prolific songwriter Tinsley raw power of his music.” Ellis has grown his worldwide audience one Ellis considers his new album, Ice scorching performance at a time. Armed with Cream In Hell, the most raw-sounding, guitar- blazing, every-note-matters guitar skills and drenched album of his career. Recorded scores of instantly memorable original songs, in Nashville and produced by Ellis and his Ellis has traveled enough miles, he says, “to longtime co-producer Kevin McKendree get to the moon and back six times.” He’s (John Hiatt, Delbert McClinton), Ice Cream released 17 previous solo albums, and has In Hell is a cathartic blast of blues-rock earned his place at the top of the blues-rock power. Though inspired by all three Kings world.
    [Show full text]
  • Harmonic Resources in 1980S Hard Rock and Heavy Metal Music
    HARMONIC RESOURCES IN 1980S HARD ROCK AND HEAVY METAL MUSIC A thesis submitted to the College of the Arts of Kent State University in partial fulfillment of the requirements for the degree of Master of Arts in Music Theory by Erin M. Vaughn December, 2015 Thesis written by Erin M. Vaughn B.M., The University of Akron, 2003 M.A., Kent State University, 2015 Approved by ____________________________________________ Richard O. Devore, Thesis Advisor ____________________________________________ Ralph Lorenz, Director, School of Music _____________________________________________ John R. Crawford-Spinelli, Dean, College of the Arts ii Table of Contents LIST OF FIGURES ............................................................................................................................... v CHAPTER I........................................................................................................................................ 1 INTRODUCTION ........................................................................................................................... 1 GOALS AND METHODS ................................................................................................................ 3 REVIEW OF RELATED LITERATURE............................................................................................... 5 CHAPTER II..................................................................................................................................... 36 ANALYSIS OF “MASTER OF PUPPETS” ......................................................................................
    [Show full text]
  • Additive Synthesis, Amplitude Modulation and Frequency Modulation
    Additive Synthesis, Amplitude Modulation and Frequency Modulation Prof Eduardo R Miranda Varèse-Gastprofessor [email protected] Electronic Music Studio TU Berlin Institute of Communications Research http://www.kgw.tu-berlin.de/ Topics: Additive Synthesis Amplitude Modulation (and Ring Modulation) Frequency Modulation Additive Synthesis • The technique assumes that any periodic waveform can be modelled as a sum sinusoids at various amplitude envelopes and time-varying frequencies. • Works by summing up individually generated sinusoids in order to form a specific sound. Additive Synthesis eg21 Additive Synthesis eg24 • A very powerful and flexible technique. • But it is difficult to control manually and is computationally expensive. • Musical timbres: composed of dozens of time-varying partials. • It requires dozens of oscillators, noise generators and envelopes to obtain convincing simulations of acoustic sounds. • The specification and control of the parameter values for these components are difficult and time consuming. • Alternative approach: tools to obtain the synthesis parameters automatically from the analysis of the spectrum of sampled sounds. Amplitude Modulation • Modulation occurs when some aspect of an audio signal (carrier) varies according to the behaviour of another signal (modulator). • AM = when a modulator drives the amplitude of a carrier. • Simple AM: uses only 2 sinewave oscillators. eg23 • Complex AM: may involve more than 2 signals; or signals other than sinewaves may be employed as carriers and/or modulators. • Two types of AM: a) Classic AM b) Ring Modulation Classic AM • The output from the modulator is added to an offset amplitude value. • If there is no modulation, then the amplitude of the carrier will be equal to the offset.
    [Show full text]
  • Guitar Best Practices Years 1, 2, 3 and 4 Nafme Council for Guitar
    Guitar Best Practices Years 1, 2, 3 and 4 Many schools today offer guitar classes and guitar ensembles as a form of music instruction. While guitar is a popular music choice for students to take, there are many teachers offering instruction where guitar is their secondary instrument. The NAfME Guitar Council collaborated and compiled lists of Guitar Best Practices for each year of study. They comprise a set of technical skills, music experiences, and music theory knowledge that guitar students should know through their scholastic career. As a Guitar Council, we have taken careful consideration to ensure that the lists are applicable to middle school and high school guitar class instruction, and may be covered through a wide variety of method books and music styles (classical, country, folk, jazz, pop). All items on the list can be performed on acoustic, classical, and/or electric guitars. NAfME Council for Guitar Education Best Practices Outline for a Year One Guitar Class YEAR ONE - At the completion of year one, students will be able to: 1. Perform using correct sitting posture and appropriate hand positions 2. Play a sixteen measure melody composed with eighth notes at a moderate tempo using alternate picking 3. Read standard music notation and play on all six strings in first position up to the fourth fret 4. Play melodies in the keys C major, a minor, G major, e minor, D major, b minor, F major and d minor 5. Play one octave scales including C major, G major, A major, D major and E major in first position 6.
    [Show full text]
  • Compound AABA Form and Style Distinction in Heavy Metal *
    Compound AABA Form and Style Distinction in Heavy Metal * Stephen S. Hudson NOTE: The examples for the (text-only) PDF version of this item are available online at: hps://www.mtosmt.org/issues/mto.21.27.1/mto.21.27.1.hudson.php KEYWORDS: Heavy Metal, Formenlehre, Form Perception, Embodied Cognition, Corpus Study, Musical Meaning, Genre ABSTRACT: This article presents a new framework for analyzing compound AABA form in heavy metal music, inspired by normative theories of form in the Formenlehre tradition. A corpus study shows that a particular riff-based version of compound AABA, with a specific style of buildup intro (Aas 2015) and other characteristic features, is normative in mainstream styles of the metal genre. Within this norm, individual artists have their own strategies (Meyer 1989) for manifesting compound AABA form. These strategies afford stylistic distinctions between bands, so that differences in form can be said to signify aesthetic posing or social positioning—a different kind of signification than the programmatic or semantic communication that has been the focus of most existing music theory research in areas like topic theory or musical semiotics. This article concludes with an exploration of how these different formal strategies embody different qualities of physical movement or feelings of motion, arguing that in making stylistic distinctions and identifying with a particular subgenre or style, we imagine that these distinct ways of moving correlate with (sub)genre rhetoric and the physical stances of imagined communities of fans (Anderson 1983, Hill 2016). Received January 2020 Volume 27, Number 1, March 2021 Copyright © 2021 Society for Music Theory “Your favorite songs all sound the same — and that’s okay .
    [Show full text]
  • The Sonification Handbook Chapter 9 Sound Synthesis for Auditory Display
    The Sonification Handbook Edited by Thomas Hermann, Andy Hunt, John G. Neuhoff Logos Publishing House, Berlin, Germany ISBN 978-3-8325-2819-5 2011, 586 pages Online: http://sonification.de/handbook Order: http://www.logos-verlag.com Reference: Hermann, T., Hunt, A., Neuhoff, J. G., editors (2011). The Sonification Handbook. Logos Publishing House, Berlin, Germany. Chapter 9 Sound Synthesis for Auditory Display Perry R. Cook This chapter covers most means for synthesizing sounds, with an emphasis on describing the parameters available for each technique, especially as they might be useful for data sonification. The techniques are covered in progression, from the least parametric (the fewest means of modifying the resulting sound from data or controllers), to the most parametric (most flexible for manipulation). Some examples are provided of using various synthesis techniques to sonify body position, desktop GUI interactions, stock data, etc. Reference: Cook, P. R. (2011). Sound synthesis for auditory display. In Hermann, T., Hunt, A., Neuhoff, J. G., editors, The Sonification Handbook, chapter 9, pages 197–235. Logos Publishing House, Berlin, Germany. Media examples: http://sonification.de/handbook/chapters/chapter9 18 Chapter 9 Sound Synthesis for Auditory Display Perry R. Cook 9.1 Introduction and Chapter Overview Applications and research in auditory display require sound synthesis and manipulation algorithms that afford careful control over the sonic results. The long legacy of research in speech, computer music, acoustics, and human audio perception has yielded a wide variety of sound analysis/processing/synthesis algorithms that the auditory display designer may use. This chapter surveys algorithms and techniques for digital sound synthesis as related to auditory display.
    [Show full text]
  • MUSIC 158 Proceeds with Techniques and Compositions of Intermediate Level for Classical Guitar
    COURSE OUTLINE : MUSIC 158 D Credit – Degree Applicable COURSE ID 001203 AUGUST 2020 COURSE DISCIPLINE : MUSIC COURSE NUMBER : 158 COURSE TITLE (FULL) : Classical Guitar III COURSE TITLE (SHORT) : Classical Guitar III CATALOG DESCRIPTION MUSIC 158 proceeds with techniques and compositions of intermediate level for classical guitar. Included for study are selected pieces from the Renaissance, Baroque, Classic and Romantic eras, as well as solo arrangements of familiar tunes. Knowledge of the entire fingerboard is further enhanced by the practice of two and three octave scales. Basic skills for transcribing music written for keyboard are introduced. CATALOG NOTES Note: This class requires the student to have a full-size guitar in playable condition. Total Lecture Units: 0.00 Total Laboratory Units: 1.00 Total Course Units: 1.00 Total Lecture Hours: 0.00 Total Laboratory Hours: 54.00 Total Laboratory Hours To Be Arranged: 0.00 Total Contact Hours: 54.00 Total Out-of-Class Hours: 0.00 Prerequisite: MUSIC 157 or equivalent. GLENDALE COMMUNITY COLLEGE --FOR COMPLETE OUTLINE OF RECORD SEE GCC WEBCMS DATABASE-- Page 1 of 4 COURSE OUTLINE : MUSIC 158 D Credit – Degree Applicable COURSE ID 001203 AUGUST 2020 ENTRY STANDARDS Subject Number Title Description Include 1 MUSIC 157 Classical Guitar II Analyze and perform music of greater Yes contrapuntal and rhythmic complexity; 2 MUSIC 157 Classical Guitar II observe and demonstrate variations in Yes volume; 3 MUSIC 157 Classical Guitar II incorporate proper techniques for slurs and Yes grace notes into music as required; 4 MUSIC 157 Classical Guitar II develop the ability to produce natural and Yes artificial harmonics; 5 MUSIC 157 Classical Guitar II extend familiarity with the fret board by Yes practicing scales in several positions; 6 MUSIC 157 Classical Guitar II construct basic triads in major and minor Yes keys and apply them to the comprehension of fretboard harmony.
    [Show full text]
  • “Apoyando” and “Tirando” Related to Its Harmonic Components and Autocorrelation Function
    Buenos Aires – 5 to 9 September, 2016 Acoustics for the 21st Century… PROCEEDINGS of the 22nd International Congress on Acoustics Music Perception: Paper ICA2016-227 Subjective preference of classical guitar strokes “apoyando” and “tirando” related to its harmonic components and autocorrelation function Joaquin Garcia(a), Shin-ichi Sato(b), Florent Masson(c) (a)Universidad Nacional de Tres de Febrero, Argentina, [email protected] (b)Universidad Nacional de Tres de Febrero, Argentina, [email protected] (c)Universidad Nacional de Tres de Febrero, Argentina, [email protected] Abstract Tone production of classical guitar performance is an essential part for musicians to transmit their sentimental and interpretative intentions. This work investigates subjective preferences of two common plucking techniques used by guitar players, apoyando (rest) and tirando (free) strokes. Six excerpts of classical guitar music with different tempos and range of frequency were performed using the two techniques and were recorded for the subjective tests. Two groups of subjects, guitar players and people who do not play guitar, were investigated to see if both groups evaluate the guitar timbre in different way or not. AB test was conducted with 50 persons for each group asking which technique is preferred and have more sound quality. Then the harmonic components and autocorrelation function (ACF) of each stroke were analysed to relate with the characteristics of the music program (tempo and frequency range) and subjective preferences. The effective duration of ACF is defined with the taue (τe) parameter. Results of the subjective test showed that harmonic content did not define preferences, but higher taue values of the ACF were correlated with a higher sound guitar quality.
    [Show full text]
  • Frequency-Domain Additive Synthesis with an Oversampled Weighted Overlap-Add Filterbank for a Portable Low-Power MIDI Synthesizer
    Audio Engineering Society Convention Paper 6202 Presented at the 117th Convention 2004 October 28–31 San Francisco, CA, USA This convention paper has been reproduced from the author's advance manuscript, without editing, corrections, or consideration by the Review Board. The AES takes no responsibility for the contents. Additional papers may be obtained by sending request and remittance to Audio Engineering Society, 60 East 42nd Street, New York, New York 10165-2520, USA; also see www.aes.org. All rights reserved. Reproduction of this paper, or any portion thereof, is not permitted without direct permission from the Journal of the Audio Engineering Society. Frequency-Domain Additive Synthesis With An Oversampled Weighted Overlap-Add Filterbank For A Portable Low-Power MIDI Synthesizer King Tam1 1 Dspfactory Ltd., Waterloo, Ontario, N2V 1K8, Canada [email protected] ABSTRACT This paper discusses a hybrid audio synthesis method employing both additive synthesis and DPCM audio playback, and the implementation of a miniature synthesizer system that accepts MIDI as an input format. Additive synthesis is performed in the frequency domain using a weighted overlap-add filterbank, providing efficiency gains compared to previously known methods. The synthesizer system is implemented on an ultra-miniature, low-power, reconfigurable application specific digital signal processing platform. This low-resource MIDI synthesizer is suitable for portable, low-power devices such as mobile telephones and other portable communication devices. Several issues related to the additive synthesis method, DPCM codec design, and system tradeoffs are discussed. implementation using the Fourier transform and inverse Fourier transform. 1. INTRODUCTION While several other synthesis methods have been Additive synthesis in musical applications has been developed, interest in additive synthesis has continued.
    [Show full text]
  • Wavetable Synthesis 101, a Fundamental Perspective
    Wavetable Synthesis 101, A Fundamental Perspective Robert Bristow-Johnson Wave Mechanics, Inc. 45 Kilburn St., Burlington VT 05401 USA [email protected] ABSTRACT: Wavetable synthesis is both simple and straightforward in implementation and sophisticated and subtle in optimization. For the case of quasi-periodic musical tones, wavetable synthesis can be as compact in data storage requirements and as general as additive synthesis but requires much less real-time computation. This paper shows this equivalence, explores some suboptimal methods of extracting wavetable data from a recorded tone, and proposes a perceptually relevant error metric and constraint when attempting to reduce the amount of stored wavetable data. 0 INTRODUCTION Wavetable music synthesis (not to be confused with common PCM sample buffer playback) is similar to simple digital sine wave generation [1] [2] but extended at least two ways. First, the waveform lookup table contains samples for not just a single period of a sine function but for a single period of a more general waveshape. Second, a mechanism exists for dynamically changing the waveshape as the musical note evolves, thus generating a quasi-periodic function in time. This mechanism can take on a few different forms, probably the simplest being linear crossfading from one wavetable to the next sequentially. More sophisticated methods are proposed by a few authors (recently Horner, et al. [3] [4]) such as mixing a set of well chosen basis wavetables each with their corresponding envelope function as in Fig. 1. The simple linear crossfading method can be thought of as a subclass of the more general basis mixing method where the envelopes are overlapping triangular pulse functions.
    [Show full text]