Download e-book for iPad: Acoustics of Musical Instruments by Antoine Chaigne

Download e-book for iPad: Acoustics of Musical Instruments by Antoine Chaigne

By Antoine Chaigne

ISBN-10: 1493936778

ISBN-13: 9781493936779

ISBN-10: 1493936794

ISBN-13: 9781493936793

This e-book, the 1st English-language translation of Acoustique des tools de musique, moment Edition, offers the required foundations for knowing the advanced actual phenomena thinking about musical tools. what's the functionality of the labium in a flute? Which good points of an tool let us make a transparent audible contrast among a clarinet and a trumpet? With the aid of various examples, those questions are addressed intimately. The authors concentration specifically at the major effects received within the box over the last fifteen years. Their aim is to teach that straightforward actual versions can be utilized with profit for varied purposes in sound synthesis, tool making, and sound recording. The e-book is basically addressed to graduate scholars and researchers; but it may be of curiosity for engineers, musicians, craftsmen, and tune enthusiasts who desire to find out about the fundamentals of musical acoustics.

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Example text

In linear acoustics, we can now linearize Eq. 101) to the first order, which is the Euler equation. 103) 36 A. Chaigne and J. 101) implies that the zeroth order of F is zero (because 0 is not zero): thus, F is of the first order. 101), it is seen that if the force F is irrotational, this is also the case for the velocity, and they both derive from a potential, written V and ': F D gradV and v D grad'. , along a streamline. 104) We can include the right-hand side function in the potential ', which is defined apart from a space-independent function, and we obtain a righthand side equal to zero.

Gravity is ignored. x/h R D 11 12 12 22 @x @x @y @y @x @y where h is the thickness. 8) In Eq. 8), the source term corresponds to a pressure jump across the membrane. For timpani, this pressure jump is equal to the difference between the sound pressure in the cavity and the sound pressure in the external air, in the membrane plane z D 0. More generally, the membrane may be subjected to a distribution of external forces localized or distributed on its surface. x; y; t/ (with dimension of a pressure) is due, for example, to the action of a timpani mallet or of a drum stick.

Such vibrations arise because fluctuations in length induce stress fluctuations. As a consequence, the stress becomes a function of the amplitude (and thus a function of time). This transverse–longitudinal coupling is usually neglected under the assumption of small amplitude. Nevertheless, it can be easily observed in piano strings, for example. This point will be clarified in Chap. 8. 2 Homogeneous Membranes and Strings Under Uniform Tension For a uniformly stretched membrane made of a homogeneous material, the tension tensor becomes isotropic, which can be written as D 1l, where 1l denotes the unit tensor.

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Acoustics of Musical Instruments by Antoine Chaigne

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