Download A Geometry of Music: Harmony and Counterpoint in the by Dmitri Tymoczko PDF

By Dmitri Tymoczko

How is the Beatles' "Help!" just like Stravinsky's "Dance of the Adolescents?" How does Radiohead's "Just" relate to the improvisations of invoice Evans? and the way do Chopin's works make the most the non-Euclidean geometry of musical chords?
during this groundbreaking paintings, writer Dmitri Tymoczko describes a brand new framework for wondering song that emphasizes the commonalities between types from medieval polyphony to modern rock. Tymoczko identifies 5 simple musical positive factors that together give a contribution to the feel of tonality, and indicates how those good points recur during the historical past of Western track. within the method he sheds new mild on an age-old query: what makes tune sound good?
A Geometry of tune presents an obtainable advent to Tymoczko's progressive geometrical method of tune idea. The e-book exhibits the best way to build easy diagrams representing relationships between usual chords and scales, giving readers the instruments to translate among the musical and visible nation-states and revealing spectacular levels of constitution in differently hard-to-understand items.
Tymoczko makes use of this theoretical origin to retell the heritage of Western tune from the 11th century to the current day. Arguing that conventional histories concentration too narrowly at the "common practice" interval from 1680-1850, he proposes in its place that Western song contains a longer universal perform stretching from the overdue center a while to the current. He discusses a bunch of common items by means of quite a lot of composers, from Bach to the Beatles, Mozart to Miles Davis, and lots of in between.
A Geometry of tune is available to more than a few readers, from undergraduate tune majors to scientists and mathematicians with an curiosity in track. Defining its phrases alongside the way in which, it presupposes no distinct mathematical heritage and just a easy familiarity with Western track idea. The e-book additionally includes workouts designed to enhance and expand readers' figuring out, besides a chain of appendices that discover the technical information of this intriguing new concept.

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Additional info for A Geometry of Music: Harmony and Counterpoint in the Extended Common Practice (Oxford Studies in Music Theory)

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Suppose, on Tuesday, a typical person whistles a tune whose pitches have frequencies f, g, h,. . On Wednesday, if asked to reproduce the tune, she is likely to whistle the frequencies cf, cg, ch, . , where c is some number close to one. Musicians say that the whistler has transposed the notes, changing their fundamental frequencies so as to preserve the ratios between them. 1 Musicians do not like to work with fundamental frequencies, since ratios are awkward and division is hard; furthermore, we typically measure numerical distances using subtraction rather than division.

We do not determine the meaning of sentences by estimating the proportion of nouns to verbs, but we do respond very strongly to relatively crude global features of the musical stimulus. Does the piece use consonant or dissonant harmonies? Does it restrict itself, over moderate spans of musical time, to a small set of notes, and do these notes themselves change over larger time spans? Do melodies in general move by short distances? The answers to these questions tell us an enormous amount about how untrained listeners will respond to a piece.

Pitch. Thus IB3 Harmony and Voice Leading would be. The point A3 is a fixed point of the inversion, since it is unaltered by the reflection. ) Inversions, unlike transpositions, cannot be distinguished by their size, since for any distance x, an inversion will move some pair of pitches by that amount. Transposition and inversion can also be defined in pitch-class space. 4 shows that transposition is represented by rotation while inversion is represented by reflection: the inversion around C sends every pitch class to the point where its image would appear, if there were a pointlike mirror at C.

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