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Zigzag
Zigzag
from Wikipedia
Drawing of a zigzag

A zigzag is a pattern made up of small corners at variable angles, though constant within the zigzag, tracing a path between two parallel lines; it can be described as both jagged and fairly regular.

In geometry, this pattern is described as a skew apeirogon. From the point of view of symmetry, a regular zigzag can be generated from a simple motif like a line segment by repeated application of a glide reflection.

Although the origin of the word is unclear, its first printed appearances were in French-language books and ephemera of the late 17th century.[1]

Examples of zigzags

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A 2-metre carpenter's ruler with centimetre divisions
Road sign warning for upcoming zigzag turn.
A seismograph showing zigzag lines

See also

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References

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Bibliography

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Revisions and contributorsEdit on WikipediaRead on Wikipedia
from Grokipedia
A zigzag is a line, path, or characterized by a series of short, sharp turns or angles alternating in direction, often resembling the jagged form of or a sawtooth. This geometric motif has been employed across various domains, including , , and , to convey motion, , and symbolism since prehistoric times. The term "zigzag" originated in the late , first appearing in French as zigzag around , likely derived from the German Zickzack, evoking the onomatopoeic sound or visual repetition of angular shifts. Its earliest documented uses trace back to printed French books and , reflecting a European linguistic evolution that captured the essence of irregular, alternating lines. In ancient and prehistoric contexts, zigzag patterns adorned artifacts such as antler batons, bone daggers, and cave art, where they served protective or symbolic roles, often linked to motifs representing continuity, the cycle of life and death, or warding off harm in funerary and settlement sites across Northern during the Palaeolithic and periods. These early applications highlight the pattern's intuitive appeal, as it mimics natural phenomena like , river courses, or animal markings, making it one of the simplest yet versatile motifs in human artistic expression. In , the zigzag motif evolved into structural and decorative elements, notably as the zigzag arch—a crenellated or jagged archway—prevalent in Islamic, Byzantine, Norman, and Romanesque styles from the medieval period onward, where it added rhythmic ornamentation to doorways, friezes, and facades. The marked a peak in its popularity through the movement (circa 1910s–1930s), where the angular, geometric zigzag—termed Zigzag Moderne—defined urban , interiors, and in cities like New York and , symbolizing modernity, speed, and industrial progress through bold, repetitive lines in , furniture, and fashion. Today, zigzag patterns persist in contemporary , from textiles and to digital graphics, valued for their dynamic visual and adaptability across scales.

Etymology and Definition

Etymology

The term "zigzag" originates from French, where it was first attested in the late 17th century (around 1670), likely borrowed from a Germanic source such as Walloon ziczac or directly from German Zickzack (attested from ), with the form imitating the sound or motion of sharp, alternating turns. The word's structure is partly symbolic or onomatopoeic, as the repetition of similar syllables with varying vowels evokes the back-and-forth direction of a path, akin to the teeth of a saw or lightning bolt. The exact pre-French roots remain unclear, but it may derive from a reduplication of Middle High German zacke, meaning "point" or "nail," reflecting pointed, angular forms. This French term entered English around 1712, initially through translations of late 17th-century French texts describing angular lines or paths. By the , "zigzag" had evolved in usage to describe not only lines or routes with sharp alternations but also broader patterns in literature and technical writings, such as fortifications or decorative motifs, solidifying its role as a versatile descriptor of irregular, angular motion. This linguistic development underscores its connection to visual representations of alternating angles in geometric patterns.

Definition and Characteristics

A zigzag is a line or path composed of short, straight segments connected at acute or obtuse angles, alternating directions, creating a jagged yet regular appearance. This pattern traces a series of small corners, with the angles remaining constant within a given zigzag while allowing variation across different instances. The term derives from French zigzag, first appearing in the late as a descriptor of such erratic motion, possibly influenced by German Zickzack. Key characteristics of a zigzag include its consistent yet variable angles—often acute or right—and the alternation of direction that produces a repetitive, non-sinusoidal form. Zigzags may be regular, featuring symmetric segment lengths and uniform angles for a balanced appearance, or irregular, with differing lengths that introduce while maintaining the overall directional shift. Unlike waves, which rely on smooth, curved transitions, zigzags are defined by their sharp, angular turns, emphasizing discrete linear elements over continuous . Visually, a zigzag manifests as a sequence of V-shapes or chevron motifs, evoking the form of a row of connected Zs. This structure is highly scalable, appearing in microscopic scales such as molecular patterns or macroscopic layouts like winding mountain roads designed for gradual elevation changes.

Geometry and Mathematics

Geometric Properties

In , a zigzag is formalized as a skew apeirogon, an infinite whose vertices lie alternately on two , resulting in a non-collinear but coplanar arrangement. This structure is generated by repeatedly applying glide reflections to a along these , producing an infinite sequence of equal-length edges that alternate direction. A key property of the zigzag is its constant width, defined as the fixed distance between the bounding parallel lines, which remains invariant regardless of the position along the pattern. The total path length of the zigzag exceeds the straight-line displacement along the central direction (perpendicular to the bounding lines) by a factor determined by the angle θ\theta between consecutive segments; specifically, the length LL satisfies L=Dcos(θ/2)L = \frac{D}{\cos(\theta/2)}, where DD is the straight-line distance. For example, with θ=60\theta = 60^\circ, cos(30)=3/20.866\cos(30^\circ) = \sqrt{3}/2 \approx 0.866
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