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Concave

In , concave describes a , surface, or that bends or curves inward, such that the interior lies on the side toward which the curve bends, opposite to a shape that curves outward. This term originates from the Latin concavus, meaning "hollow," and is commonly illustrated by the inner surface of a or . Concave forms appear in various natural and artificial contexts, such as the shape of certain lenses, arches in , and biological structures like the human palate. In the study of polygons, a is a simple that is not . In , the concept extends to , where a is concave down if its is negative, meaning the lies below its lines, the decreases over the , and it forms a downward-opening like y = -x^2. Conversely, a concave up has a positive , with the lying above its and increasing , such as y = x^2. Note that can vary: in optimization and , a "" refers to one where the lies above the chords connecting any two points (satisfying f(tx + (1-t)y) \geq t f(x) + (1-t) f(y) for t \in [0,1]), equivalent to concave down in , and the negative of a . These properties are crucial for analyzing optimization problems. Beyond , concave principles apply in physics, such as in concave mirrors that converge rays to a , enabling applications in telescopes and headlights. The distinction from forms is fundamental across disciplines, influencing design in , computer graphics for rendering curved surfaces, and even for modeling utility functions.

Mathematics

Concave polygons

A is a simple in which at least one interior measures greater than 180 degrees, known as a reflex . This distinguishes it from polygons, where all interior angles are less than or equal to 180 degrees. Alternatively, a can be identified if there exists at least one pair of points on its boundary such that the connecting them lies partially outside the . Key properties of concave polygons include the presence of at least one "dent" or indentation in their , which causes the shape to fail the convexity test: not every joining two points within the remains entirely inside it. Despite this, concave polygons remain , meaning they do not intersect themselves, and the sum of their interior angles follows the standard formula for polygons: (n-2) × 180 degrees, where n is the number of sides. These shapes must have at least four sides, as triangles are inherently . Examples of concave polygons include the or shape, a with one angle creating a pointed indentation, and an L-shaped pentagon, formed by attaching two rectangles at a , resulting in a reentrant . In visualizations, the appears as a with an inward , while the L-shape resembles a , highlighting the inward angle. A fundamental result in polygon classification states that a simple polygon is concave if and only if it is not convex, meaning it lacks the property that all internal angles are non-reflex and all boundary line segments stay inside. This theorem underscores the binary nature of simple polygon types in plane geometry.

Concave functions

In mathematical analysis, a function f: D \to \mathbb{R}, where D is a convex subset of \mathbb{R}^n, is defined as concave if for all x, y \in D and all \lambda \in [0, 1], f(\lambda x + (1 - \lambda) y) \geq \lambda f(x) + (1 - \lambda) f(y). Equivalently, f is concave if and only if -f is convex. For twice continuously differentiable functions on an open interval, f is concave if its second derivative satisfies f''(x) \leq 0 for all x in the domain. Concave functions exhibit several key properties. Composition with an affine transformation g(x) = Ax + b, where A is a and b a , preserves concavity: if f is concave, then f \circ g is concave provided the domain aligns appropriately. Concavity also implies quasiconcavity, meaning the upper level sets \{x \mid f(x) \geq \alpha\} are convex for all \alpha. A fundamental property is , which states that for a f and a X with finite , f(\mathbb{E}[X]) \geq \mathbb{E}[f(X)]. This inequality was established by Johan Jensen in 1906. Examples of include linear functions f(x) = ax + b, which are both concave and . The natural logarithm f(x) = \log x for x > 0 is strictly concave, as its is negative. In , utility functions are often modeled as concave to capture diminishing . Concave functions play a central in optimization: maximizing a over a is a problem, which is computationally tractable and guarantees global optima. Related concepts include strict concavity, where the in the definition holds strictly for \lambda \in (0,1) and x \neq y, ensuring at most one maximum.

Physics

Concave mirrors

A concave mirror is a mirror that has its reflecting surface curved inward toward the incident , resembling the interior surface of a . This causes parallel rays of to converge at a after reflection, making concave mirrors converging . The f of a concave mirror is half the R, so f = \frac{R}{2}. This relationship holds under the paraxial approximation, which assumes rays are close to the principal axis and the mirror's is gentle. Ray diagrams for concave mirrors rely on three principal s to locate the : (1) a parallel to the principal reflects through the ; (2) a passing through the reflects parallel to the principal ; and (3) a passing through the center of reflects back along the same path. These s intersect to form the , providing a geometric method to predict its position and nature without equations. Image formation depends on the object's position relative to the . For objects beyond the , a real, inverted forms on the same side as the incoming , which can be onto a screen. When the object is inside the , a , upright, and magnified appears behind the mirror. The lateral m is given by m = -\frac{v}{u}, where u is the object distance and v is the image distance (using the where distances are positive for real images and objects). Concave mirrors find applications in optical instruments due to their light-converging properties. In telescopes, such as the Cassegrain design, a primary concave mirror collects and focuses distant light, with a secondary mirror redirecting it to the for observation. They are used in headlights to produce a parallel beam for illumination and in solar cookers to concentrate sunlight for heating. Historically, concave mirrors were employed in ancient times for concentrating light, as in the legendary account of using them to focus sunlight on enemy ships during the siege of Syracuse in 214 BCE. Their optical principles were formalized in the 17th century by , who constructed the first in 1668 using a concave primary mirror to avoid in lenses.

Concave lenses

A concave lens, also known as a diverging lens, is an optical component that is thinner at its center than at its edges, causing parallel rays of incident upon it to diverge after as if emanating from a focal point on the same side as the incident . This diverging arises from the inward of at least one surface, which bends rays outward relative to the principal axis. Unlike lenses, which converge , concave lenses spread it out, making them essential for applications requiring or minification. The focal length f of a concave lens is negative (f < 0), indicating its diverging nature, and is determined by the lensmaker's formula for a thin lens in air: \frac{1}{f} = (n - 1) \left( \frac{1}{R_1} - \frac{1}{R_2} \right) where n is the refractive index of the lens material, and R_1 and R_2 are the radii of curvature of the first and second surfaces, respectively, following the sign convention that R is positive for convex surfaces facing the incident light and negative for concave ones. For a typical biconcave lens with symmetric surfaces, this yields a negative f, confirming the lens's inability to form real images. In ray diagrams for concave lenses, three principal rays are commonly traced to locate the image: a ray parallel to the principal axis refracts through the lens and diverges as if originating from the on the incident side; a ray passing through the of the lens proceeds undeviated; and a ray aimed toward the on the opposite side refracts parallel to the principal axis after passing through the lens. These rays, when extended backward, intersect at the position, illustrating the lens's behavior for objects placed anywhere along the axis. For real objects, concave lenses invariably form images that are upright and diminished in size, located between the lens and its on the same side as the object. The distance is always shorter than the object distance, and no real images can be projected onto a screen due to the diverging rays. This consistent type makes concave lenses unsuitable for but ideal for correction and tasks. Concave lenses find widespread applications in vision correction, particularly in eyeglasses for (nearsightedness), where they diverge incoming light to shift the backward onto the . The power P of such lenses is given by P = 1/f (with f in meters), expressed in diopters (D), and is negative for diverging lenses—for instance, a -3.00 D corrects moderate by effectively reducing the eye's converging power. They are also used in compound microscopes as components of objective assemblies to correct aberrations and expand beam widths, and in camera systems to achieve wide-angle effects by diverging light for broader fields of view. Concave lenses for vision correction were developed in 15th-century , with records indicating their production in by the mid-1400s to address nearsightedness, building on earlier convex lenses invented around 1286. This advancement marked a significant step in optical history, enabling clearer distant vision for those with refractive errors.

Other applications

In architecture

In architecture, concave elements refer to surfaces or forms that curve inward, forming depressions or hollows that generate and visual depth, in contrast to elements that project outward. These inward curves often serve to enclose spaces, foster a sense of , and manipulate perceptions of and within built environments. Historically, concave forms appeared prominently in ancient basilicas through apses, which were semi-circular, inward-curving projections at the end of the rectangular hall, designed to accommodate judicial or ceremonial functions while enhancing spatial focus. For instance, basilicas like the in the featured such apses to create a contained area for magistrates, emphasizing and intimacy within larger public structures. In Gothic cathedrals, concave vaults, particularly fan vaults with ribs radiating in concave patterns, contributed to an illusion of greater height by drawing the eye upward through layered, curving compartments that distributed light and weight efficiently. Examples include the fan vaults at Chapel in , where the concave arrangement amplifies verticality and ethereal quality. In modern applications, architects like employed fluid concave facades to evoke organic dynamism and cultural fluidity, as seen in the in , , completed in 2012, where sweeping inward curves integrate the building with its landscape and avoid rigid geometries. These forms also support by diffusing natural light across interior surfaces, reducing glare and promoting even illumination, as concave profiles scatter incoming rays more uniformly than flat or convex ones. Structurally, inward-curving concave forms present challenges in load-bearing, as they can concentrate stresses and risk under without adequate , often necessitating tensile materials such as high-strength fabrics or thin shells to maintain stability. Engineers address these by using catenary-inspired tensile membranes that distribute forces through rather than bending, or by fabricating prefabricated shells that exploit for self-support while minimizing material use. Aesthetically, concave elements enhance spatial perception by creating intimacy in expansive public areas, drawing viewers inward to foster emotional engagement and a sense of shelter, a technique influenced by 17th-century where undulating concave surfaces generated dramatic movement and immersion. In Baroque designs, such as those by , inward curves in facades and interiors manipulated light and shadow to heighten theatricality and psychological depth, laying groundwork for later explorations in perceptual architecture.

In engineering

In engineering, concave profiles refer to curved surfaces that bend inward, often employed to optimize distribution, enhance , or facilitate precise component fitting in various structures and mechanisms. These designs help mitigate concentrations by distributing loads more uniformly across surfaces, as seen in contact geometries where curved profiles reduce peak pressures compared to flat interfaces. In applications, concave curvatures influence behavior, promoting the formation of counter-rotating vortices that can enhance or mixing in turbulent flows. In mechanical engineering, concave elements such as cams and gears are utilized to achieve smooth, controlled motion in machinery. Concave globoidal cams with swinging roller followers enable precise indexing and high-speed operations by minimizing vibrations and ensuring continuous contact during rotation. Similarly, internal gears feature concave tooth profiles that mesh with external gears to transmit power efficiently while accommodating radial adjustments for alignment. To further reduce stress concentrations in machine parts like shafts and fillets, engineers apply concave fillet radii, which lower peak stresses under bending or torsion loads; Roark's Formulas for Stress and Strain provides tabulated factors showing that increasing the fillet radius-to-shoulder height ratio can reduce stress concentration factors by up to 50% in typical configurations. Civil engineering leverages concave profiles in bridge and arch designs to manage tensile forces effectively. Suspension bridges like the Akashi Kaikyō Bridge (completed in 1998) employ parabolic cable shapes—approximating a concave upward curve under self-weight—to distribute across the main span of 1,991 meters, allowing the structure to withstand seismic and loads up to 80 m/s. This configuration transforms the bridge deck into a tension member supported by parabolic cables, optimizing material use and in long-span applications. In , concave nozzles are critical for , where bell-shaped designs expand exhaust gases efficiently to maximize . The Bell nozzle, developed in the mid-20th century, features a concave divergent section that accelerates flow supersonically while minimizing losses; its contour is optimized using the , which solves partial differential equations to align shock waves and achieve uniform exit conditions, potentially increasing by approximately 2-10% over conical nozzles. Concave mirrors also find brief application in dishes, focusing incoming radio signals onto receivers for reliable communication links. Concave designs offer advantages in by improving through reduced in curved flows and enhancing acoustics via controlled wave propagation in nozzles, but they present challenges in , as deviations in can amplify instabilities or require advanced composites integrated since the for high-temperature resilience. These profiles demand tools and finite element analysis to balance performance gains against fabrication complexities, such as molding concave composites without defects.

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