Download Music - A Mathematical Offering by Dave Benson PDF

By Dave Benson

Because the time of the traditional Greeks, a lot has been written concerning the relation among arithmetic and song: from concord and quantity thought, to musical styles and staff concept. Benson presents a wealth of knowledge the following to permit the trainer, the coed, or the novice to appreciate, at various degrees of technicality, the genuine interaction among those historical disciplines. the tale is lengthy in addition to extensive and contains physics, biology, psycho acoustics, the heritage of technology, and electronic expertise in addition to, in fact, arithmetic and song. beginning with the constitution of the human ear and its dating with Fourier research, the tale proceeds through the maths of musical tools to the tips of consonance and dissonance, after which to scales and temperaments. this can be a must-have ebook that allows you to learn about the tune of the spheres or electronic tune and plenty of issues in among.

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Extra resources for Music - A Mathematical Offering

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To begin to answer this question, we first ask: given a function defined by a trigonometric series, how can the coefficients an and bn be recovered? 1). This suggests that in order to find the coefficent am , we multiply f (θ) by cos(mθ) and integrate. 1). Provided we can pass the integral through the infinite sum, only one term gives a nonzero contribution. So for m > 0 we have 2π 2π cos(mθ) cos(mθ)f (θ) dθ = 0 0 2π = 12 a0 cos(mθ) dθ + 0 ∞ 1 2 a0 + ∞ (an cos(nθ) + bn sin(nθ)) dθ n=1 2π an n=1 2π cos(mθ) cos(nθ) dθ + bn 0 cos(mθ) sin(nθ) dθ 0 = πam .

Examples 1. Consider the equation y¨ + 4y˙ + 5y = 10t2 − 1. 2) 2 We look for a particular integral of the form y = at + bt + c. Differentiating, we get y˙ = 2at + b and y¨ = 2a. 2) gives 2a + 4(2at + b) + 5(at2 + bt + c) = 10t2 + t − 3. Comparing coefficients of t2 gives 5a = 10 or a = 2. Then comparing coefficients of t gives 8a + 5b = 1, so b = −3. Finally, comparing constant terms gives 2a + 4b + 5c = −3, so c = 1. So we get a particular integral of y = 2t2 − 3t + 1. 2) is given by y = 2t2 − 3t + 1 + e−2t (A′ cos t + B ′ sin t).

The above value of ω is called the resonant frequency of the system. 4) for the complementary function: √ µ2 −∆ k = − , ω= 2m m 4m2 which is already less than the value of ω for the corresponding undamped system: k ω= . m Example. Consider the forced, underdamped equation ω= y¨ + 2y˙ + 30y = 10 sin ωt. amplitude The above formula √ tells us that the amplitude of the resulting steady state √ sine wave solution is 10/ 900 − 56ω 2 + ω 4 , which has its maximum value at ω = 28. 5 5 10 angular frequency ω Without the damping term, the amplitude of the steady state solution to the equation y¨ + 30y = 10 sin ωt, √ is equal to 10/|30 − ω 2 |.

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