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Voice Leading: The Science Behind a Musical Art PDF

269 Pages·2016·2.58 MB·English
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Voice Leading The Science behind a Musical Art David Huron The MIT Press Cambridge, Massachusetts London, England © 2016 Massachusetts Institute of Technology All rights reserved. No part of this book may be reproduced in any form by any electronic or mechanical means (including photocopying, recording, or information storage and retrieval) without permission in writing from the publisher. MIT Press books may be purchased at special quantity discounts for business or sales promotional use. For information, please email [email protected] or write to Special Sales Department, The MIT Press, 1 Rogers Street, Cambridge, MA 02142. This book was set in Stone Sans and Stone Serif by Toppan Best-set Premedia Limited. Printed and bound in the United States of America. Library of Congress Cataloging-in-Publication Data Names: Huron, David Brian. Title: Voice leading : the science behind a musical art / David Huron. Description: Cambridge, MA : MIT Press, [2016] | Includes bibliographical references and index. Identifiers: LCCN 2016004808 | ISBN 9780262034852 (hardcover : alk. paper) eISBN 9780262335430 Subjects: LCSH: Harmony. | Music--Psychological aspects. | Music perception. Classification: LCC ML3836 .H87 2016 | DDC 781.4/2--dc23 LC record available at http://lccn.loc.gov/2016004808 ePub Version 1.0 Table of Contents Title page Copyright page Preface 1 Introduction 2 The Canon 3 Sources and Images 4 Principles of Image Formation 5 Auditory Masking 6 Connecting the Dots 7 Preference Rules 8 Types of Part-Writing 9 Embellishing Tones 10 The Feeling of Leading 11 Chordal-Tone Doubling 12 Direct Intervals Revisited 13 Hierarchical Streams 14 Scene Setting 15 The Cultural Connection 16 Ear Teasers 17 Conclusion Afterword Acknowledgments References Index List of Tables List of Tables Table 10.1 Probabilities of successive diatonic pitches (major mode only) List of Illustrations Figure 4.1 Changes of toneness versus pitch for complex tones from various natural and artificial sources, calculated according to the method described in Terhardt, Stoll, and Seewann (1982a, 1982b). Solid line: pitch weight for standardized electronic tones from C1 to C7. Dotted lines: toneness for recorded tones spanning the entire ranges for harp, violin, flute, trumpet, cello, and contrabassoon. Figure 5.1 Relationship between input frequency and place of maximum stimulation on the basilar membrane. Figure 5.2 Approximate size of critical bands represented using musical notation. Successive notes are separated by approximately one critical bandwidth—roughly 1 millimeter separation along the basilar membrane. Notated pitches represent pure tones rather than complex tones. Note: The internote distances plotted in this figure have been calculated according to the equivalent rectangular bandwidth-rate (ERB) scale devised by Moore and Glasberg (1983; revised Glasberg & Moore, 1990). Figure 5.3 The approximate position of the first sixteen harmonics for a single complex tone with a fundamental of C2 (roughly 65 Hz). Compare the distances between successive harmonics with the size of critical bands shown in figure 5.2. Successive lower harmonics are separated by more than a critical band and so will be individually resolved by the cochlea. Beyond the sixth harmonic, the distances separating successive partials are smaller than a critical band, so neighboring harmonics will tend to interfere with each other. Notated pitches represent pure tones rather than complex tones. Figure 5.4 Average spacing of tones for sonorities having various bass pitches from C4 to C2. Calculated from over ten thousand four-note sonorities extracted from Haydn string quartets and Bach keyboard works. Bass pitches are fixed. For each bass pitch, the average tenor, alto, and soprano pitches are plotted to the nearest semitone. (Readers should not be distracted by the specific sonorities notated; only the approximate spacing of voices is of interest.) Note the wider spacing between the lower voices for chords having a low average tessitura. Notated pitches represent complex tones rather than pure tones. Source: Huron (2001; see also Huron, 1993c). Figure 5.5 Masking effect of a 1,000 Hz pure tone with an 80 dB intensity level. Complete masking is represented by the triangular region under the masking skirt. The lower tone (950 Hz with an intensity level of 60 dB) is completely masked. The higher tone (1,050 Hz with an intensity level of 70 dB) is only partially masked. Asymmetrical spread of masking with frequency is not illustrated. After Egan and Hake (1950). Figure 5.6 Masking skirts for seven harmonics of a complex tone with a fundamental frequency of 230 Hz. Note: When masking skirts are plotted with respect to position along the basilar membrane (rather than with respect to frequency), they are symmetrical. Figure 5.7 Masking skirts for two complex tones, both containing seven harmonics with identical intensities or amplitudes. The lower tone has a fundamental of 100 Hz (dashed lines); the upper tone has a fundamental of 230 Hz (solid lines). Significant mutual masking is evident. Notice that the lower partials of the higher tone mask the upper partials of the lower tone more than the other way around. Figure 5.8 Four potential masking situations: (a) no masking, (b) moderate masking, (c) significant masking, (d) complete masking. Figure 5.9 Reported consonance for complex tones from Kaestner (1909). Figure 5.10 Comparison of sensory consonance for complex tones (line) from Kaestner (1909) with interval prevalence (bars) from a sample of music by J. S. Bach. Notice especially the discrepancies for P1 and P8. Source: Adapted from Huron (1991b). Figure 6.1 Schematic illustration of auditory induction. A faint tone (line) alternates with a series of noise bursts (blocks). Listeners report hearing the faint tone as continuing throughout the noise bursts even though the tone is physically absent. Figure 6.2 Effect of pitch separation on the sense of auditory motion. (a) Neighboring pitches evoke the perception of a single undulating line. (b) Distant pitches evoke the perception of two static beeping tones with no sense of movement between the pitches. Figure 6.3 Influence of interval size and tone duration on the perception of alternating tones. In region 1, listeners always hear one stream (small interval sizes and slow tempos). In region 2, listeners always hear two streams (large interval sizes and fast tempos). In the large region between the two boundaries listeners may hear either one or two streams depending on the context and the listener’s mental disposition. Source: After van Noorden (1975, p. 15). Figure 6.4 Frequency of occurrence of melodic intervals in notated sources for folk and popular melodies from several cultures. Interval sizes have been rounded to the nearest equally tempered semitone. Source: Huron (2001). Figure 6.5 Illustration of pitch competition. Four auditory interpretations are illustrated for the stimulus shown in example (a). Ensuing pitches commonly stream to the nearest preceding pitch, as in example (b). Other stream organizations (c–e) are less likely to be heard. Figure 6.6 Illustration of part-crossing. Listeners tend to hear the two lines as bouncing away from each other (b) rather than crossing (a). Figure 6.7 Schematic illustration of two possible perceptions of intersecting pitch trajectories. Bounced perceptions (right) are more common for stimuli consisting of discrete pitch sequences, when the timbres are identical. Figure 6.8 Illustration of rhythmic discontinuity caused by crossing parts. When passage (a) is performed, listeners have a strong tendency to hear passage (b). The upper stream becomes syncopated at the point of pitch crossover, whereas the lower stream ceases to be syncopated at the point of crossover. Figure 6.9 Two pairs of circular targets illustrating Fitts’s law. Participants were asked to alternate the point of a stylus back and forth as rapidly as possible between two targets. The minimum duration of movement between targets depends on the distance separating the targets as well as target size. The movement is more rapid between the lower pair of targets. Fitts’s law applies to all muscle motions, including the motions of the vocal muscles. Musically, the distance separating the targets can be regarded as the pitch distance between two tones, whereas the size of the targets represents pitch accuracy or intonation. Fitts’s law predicts that if the intonation remains fixed, vocalists will be unable to execute wide intervals as rapidly as small intervals. Figure 6.10 Passage from Maurice Ravel’s Bolero (three measures after rehearsal marking “8”) showing the use of parallel motion in the piccolos, horn, and celeste. The pitch co-modulation in this orchestration causes an “emergent” or virtual instrument. Figure 8.1 Onset synchrony autophase functions for a random selection of ten of Bach’s two-part keyboard Inventions (BWVs 772–786) (Huron, 1993a). Values plotted at zero degrees indicate the proportion of onset synchrony for the actual works. All other phase values indicate the proportion of onset synchrony for rearranged music, controlling for duration, rhythmic order, and meter, etc. The dips at zero degrees are consistent with the hypothesis that Bach avoided synchronous note onsets between the parts. The solid line plots an average onset synchrony function for all ten works. Figure 8.2 Three-dimensional onset synchrony autophase graphs comparing polyphonic and homophonic works: (a) three-part Sinfonia no. 1 (BWV 787) by J. S. Bach; (b) four-part hymn “Adeste Fideles.” The vertical axis indicates the onset synchrony (measured according to method 3 described in Huron, 1989a). The horizontal axes indicate measure-by-measure shifts of two of the voices with respect to the remaining voice(s). Figure 8.2a shows a marked dip at the origin (front), whereas figure 8.2b shows a marked peak at the origin (back). The horizontal axes in the two graphs have been reversed to preserve visual clarity. The graphs formally demonstrate that any realignment of the parts in Bach’s Sinfonia no. 1 would result in greater onset synchrony, whereas any realignment of the parts in “Adeste Fideles” would result in less onset synchrony. Figure 8.3 Three passages illustrating (a) synchronous movement to a nonfused interval, (b) synchronous movement to a harmonically fused interval, and (c) asynchronous preparation of a tonally fused interval. Figure 8.4 Comparison of harmonically fused intervals in chorales and fugues by J. S. Bach. Only perfect harmonic intervals are plotted (e.g., unisons, fourths, fifths, octaves, twelfths). In the more homophonic chorale repertoire, most perfect intervals are formed synchronously; that is, both notes tend to begin sounding at the same moment. But in polyphonic textures, most perfect intervals are approached with asynchronous onsets (one note sounding before the onset of the second note of the interval). The two repertoires show no differences when approaching imperfect and dissonant intervals. Figure 8.5 Voice-tracking errors while listening to polyphonic music. Black columns: average estimation errors for textural density (number of polyphonic voices). Gray columns: unrecognized single-voice entries in polyphonic listening. The data show that tracking confusions for listeners to polyphonic textures employing relatively homogeneous timbres are common when more than three voices are present. Source: Huron (1989b). Figure 8.6 Relationship between nominal number of voices or parts and mean number of estimated auditory streams in 108 polyphonic works by J. S. Bach. Plotted points indicate average values for each repertoire; vertical bars indicate data ranges. The dotted line shows a relation of unity slope, where an N-voice polyphonic work maintains an average of N auditory streams. The graph shows evidence consistent with a preferred textural density of three auditory streams. Note: Average stream density for each work was calculated according to a method described and tested experimentally in Huron (1989a, chap. 14). Figure 8.7 Illustration of the “frustrated leading tone.” In the key of C, the leading tone (B) does not resolve upward to the tonic, but instead drops down to the dominant in order to allow the tonic chord to be spelled with all three chord factors (root, third, and fifth). This not uncommon harmonization suggests that in many circumstances, musicians deem full triadic harmony to be a more important goal than optimum voice leading. Figure 8.8 Schematic illustration of Wessel’s (1979) illusion. A sequence of three rising pitches is constructed using two contrasting timbres (marked with open and closed noteheads). As the tempo of presentation increases, the perception of an ascending pitch figure is replaced by two independent streams of descending pitch, each distinguished by a unique timbre. Figure 9.1 Illustrations of various embellishing tones. Examples are drawn from Bach chorale harmonizations. Figure 9.2 Illustration of two different ways of deploying embellishing tones. In both examples (a) and (b), the pitch C is doubled between the bass and alto voices. In example (a), the passing tone is assigned to a voice that does not double a pitch class. In example (b), the passing tone is assigned to a voice that does double a pitch class. The second example is more characteristic of J. S. Bach’s musical practice and is consistent with efforts to minimize tonal fusion. Figure 9.3 Frequency of occurrence of embellishing tones in chorale harmonizations by J. S. Bach. Embellishing tones occur with nearly identical frequency in the bass, tenor, and alto voices. Relatively few embellishments are found in the soprano. Source: Huron (2007). Figure 10.1 Two interleaved melodies: the odd-numbered pitches form the melody “Frère Jacques.” The even-numbered pitches form the melody “Twinkle, Twinkle, Little Star.” Source: After Dowling (1967). Figure 10.2 The same interleaved melodies as in figure 10.1 transposed. “Frère Jacques” (odd-numbered pitches) has been transposed upward, while “Twinkle, Twinkle, Little Star” (even-numbered pitches) has been transposed downward, increasing the likelihood of hearing out the two melodies. Figure 10.3 Final two phrases of the four-part hymn “St. Flavian”: (a) normal; (b) same passage played backward. Are any part-writing rules transgressed in the backward version? Figure 10.4 Schematic illustration of scale-degree successions for major- mode melodies from Huron (2006b). The thickness of each connecting line is proportional to the probability of melodic succession. The quarter-rest symbol signifies any rest or the end of a phrase. Lines have been drawn only for transitions that occur more than 1.5 percent of the time. Figure 10.5 Schematic illustration of scale-degree successions for , ♯ , and ♯ for major-key melodies. The thickness of each connecting line is proportional to the probability of melodic succession. The quarter-rest symbol signifies any rest or the end of a phrase. Figure 10.6 Figure 10.7 Figure 12.1 Figure 12.2 Figure 13.1 Figure 13.2 Figure 13.3 Figure 13.4 Figure 13.5 Figure 13.6 Figure 14.1

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An accessible scientific explanation for the traditional rules of voice leading, including an account of why listeners find some musical textures more pleasing than others. Voice leading is the musical art of combining sounds over time. In this book, David Huron offers an accessible account of the c
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Most books are stored in the elastic cloud where traffic is expensive. For this reason, we have a limit on daily download.