From Lissajous to Pas de Deux to Tattoo: The Graphic Life of a Beautiful Loop
From Lissajous to Pas de Deux to Tattoo: The Graphic Life of a Beautiful Loop
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从利萨如到双人舞再到纹身:美丽循环的图形生活
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发表时间:
2011
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通讯作者:
D. McKenna
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作者:
D. McKenna
The author re-implemented of a custom drawing technique—developed nearly 30 years ago for large pen plotter artwork—in order to redraw an aesthetically tuned, calligraphically widened, compound Lissajous figure, only to find it rendered a third time in an unusual medium for mathematical art: as a tattoo. Introduction. The history of how we draw mathematical ideas accurately by machine goes back long before our current era of ubiquitous digital computation. Prior to the 1960s, when computer programmers took their first baby steps towards creating mathematical art, perhaps the most imagination-capturing method was to play with oscillatory systems, either mechanical or later electronic. Fourier had, after all, shown in 1807 the rather startling fact that a superposition (albeit infinite) of simple trigonometric sin() and cos() functions of varying frequencies and amplitudes could be used to represent arbitrary periodic functions having nearly arbitrary shapes. The future Nobel laureate Michelson would later use an apparatus to mechanically sum and graph Fourier series.1 Using mirrors, light sources, and tuning forks, the French mathematician Lissajous built an apparatus to help him explore the output of the simple harmonic system x(t) = Ax sin(λxt+ φ) , y(t) = Ay sin(λyt) (1) (where time/angle t is measured in radians, the As are the amplitudes, the λs are the sinusoidal frequencies, and φ is a phase shift). A staple of laser light shows, these are known as two-dimensional Lissajous curves. They are visually elegant, typically closed, curves bounded in the plane by a rectangle centered at the origin, with sides 2Ax × 2Ay, where Ax and Ay are the amplitudes from equation (1). Figure 1 : Various Lissajous curves, with unit amplitudes (so they are bounded by squares, not rectangles), and using various frequency ratios. The rightmost figure also uses a phase φ 6= π/2. In the second half of the 19th century, harmonographs [1] held great fascination as a means of exploring certain compounded Lissajous figures, made more visually interesting by the effects of friction-caused Michelson also thought the machine was misbehaving due to what would later be misattributed as Gibb’s Phenomenon. Although Gibbs explained the curious discontinuity to the physics community soon after Michelson’s confusion, the phenomenon was first described by a 24-year-old Trinity math student, Henry Wilbraham, 50 years earlier than Gibbs. See [7]. Bridges 2011: Mathematics, Music, Art, Architecture, Culture