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Rose (mathematics)
Rose (mathematics)
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Roses specified by the sinusoid r = cos() for various rational numbered values of the angular frequency k = n/d.
For proper mathematical analysis, k must be expressed in irreducible form.

In mathematics, a rose or rhodonea curve is a sinusoid specified by either the cosine or sine functions with no phase angle that is plotted in polar coordinates. Rose curves or "rhodonea" were named by the Italian mathematician who studied them, Guido Grandi, between the years 1723 and 1728.[1]

General overview

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Specification

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A rose is the set of points in polar coordinates specified by the polar equation[2]

or in Cartesian coordinates using the parametric equations

Roses can also be specified using the sine function.[3] Since

.

Thus, the rose specified by r = a sin() is identical to that specified by r = a cos() rotated counter-clockwise by π/2k radians, which is one-quarter the period of either sinusoid.

Since they are specified using the cosine or sine function, roses are usually expressed as polar coordinate (rather than Cartesian coordinate) graphs of sinusoids that have angular frequency of k and an amplitude of a that determine the radial coordinate r given the polar angle θ (though when k is a rational number, a rose curve can be expressed in Cartesian coordinates since those can be specified as algebraic curves[4]).

General properties

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Artistic depiction of roses with different parameter settings

Roses are directly related to the properties of the sinusoids that specify them.

Petals

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  • Graphs of roses are composed of petals. A petal is the shape formed by the graph of a half-cycle of the sinusoid that specifies the rose. (A cycle is a portion of a sinusoid that is one period T = 2π/k long and consists of a positive half-cycle, the continuous set of points where r ≥ 0 and is T/2 = π/k long, and a negative half-cycle is the other half where r ≤ 0.)
    • The shape of each petal is same because the graphs of half-cycles have the same shape. The shape is given by the positive half-cycle with crest at (a,0) specified by r = a cos() (that is bounded by the angle interval T/4θT/4). The petal is symmetric about the polar axis. All other petals are rotations of this petal about the pole, including those for roses specified by the sine function with same values for a and k.[5]
    • Consistent with the rules for plotting points in polar coordinates, a point in a negative half-cycle cannot be plotted at its polar angle because its radial coordinate r is negative. The point is plotted by adding π radians to the polar angle with a radial coordinate |r|. Thus, positive and negative half-cycles can be coincident in the graph of a rose. In addition, roses are inscribed in the circle r = a.
    • When the period T of the sinusoid is less than or equal to 4π, the petal's shape is a single closed loop. A single loop is formed because the angle interval for a polar plot is 2π and the angular width of the half-cycle is less than or equal to 2π. When T > 4π (or |k| < 1/2) the plot of a half-cycle can be seen as spiraling out from the pole in more than one circuit around the pole until plotting reaches the inscribed circle where it spirals back to the pole, intersecting itself and forming one or more loops along the way. Consequently, each petal forms two loops when 4π < T ≤ 8π (or 1/4 ≤ |k| < 1/2), three loops when 8π < T ≤ 12π (or 1/6 ≤ |k| < 1/4), etc. Roses with only one petal with multiple loops are observed for k = 1/3, 1/5, 1/7, etc. (See the figure in the introduction section.)
    • A rose's petals will not intersect each other when the angular frequency k is a non-zero integer; otherwise, petals intersect one another.

Symmetry

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All roses display one or more forms of symmetry due to the underlying symmetric and periodic properties of sinusoids.

  • A rose specified as r = a cos() is symmetric about the polar axis (the line θ = 0) because of the identity a cos() = a cos(−) that makes the roses specified by the two polar equations coincident.
  • A rose specified as r = a sin() is symmetric about the vertical line θ = π/2 because of the identity a sin() = a sin(π) that makes the roses specified by the two polar equations coincident.
  • Only certain roses are symmetric about the pole.
  • Individual petals are symmetric about the line through the pole and the petal's peak, which reflects the symmetry of the half-cycle of the underlying sinusoid. Roses composed of a finite number of petals are, by definition, rotationally symmetric since each petal is the same shape with successive petals rotated about the same angle about the pole.

Roses with non-zero integer values of k

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The rose r = cos(4θ). Since k = 4 is an even number, the rose has 2k = 8 petals. Line segments connecting successive peaks lie on the circle r = 1 and will form an octagon. Since one peak is at (1,0) the octagon makes sketching the graph relatively easy after the half-cycle boundaries (corresponding to apothems) are drawn.
The rose specified by r = cos(7θ). Since k = 7 is an odd number, the rose has k = 7 petals. Line segments connecting successive peaks lie on the circle r = 1 and will form a heptagon. The rose is inscribed in the circle r = 1.

When k is a non-zero integer, the curve will be rose-shaped with 2k petals if k is even, and k petals when k is odd.[6] The properties of these roses are a special case of roses with angular frequencies k that are rational numbers discussed in the next section of this article.

  • The rose is inscribed in the circle r = a, corresponding to the radial coordinate of all of its peaks.
  • Because a polar coordinate plot is limited to polar angles between 0 and 2π, there are 2π/T = k cycles displayed in the graph. No additional points need be plotted because the radial coordinate at θ = 0 is the same value at θ = 2π (which are crests for two different positive half-cycles for roses specified by the cosine function).
  • When k is even (and non-zero), the rose is composed of 2k petals, one for each peak in the 2π interval of polar angles displayed. Each peak corresponds to a point lying on the circle r = a. Line segments connecting successive peaks will form a regular polygon with an even number of vertices that has its center at the pole and a radius through each peak, and likewise:
    • The roses are symmetric about the pole.
    • The roses are symmetric about each line through the pole and a peak (through the "middle" a petal) with the polar angle between the peaks of successive petals being 2π/2k = π/k radians. Thus, these roses have rotational symmetry of order 2k.
    • The roses are symmetric about each line that bisects the angle between successive peaks, which corresponds to half-cycle boundaries and the apothem of the corresponding polygon.
  • When k is odd, the rose is composed of the k petals, one for each crest (or trough) in the 2π interval of polar angles displayed. Each peak corresponds to a point lying on the circle r = a. These rose's positive and negative half-cycles are coincident, which means that in graphing them, only the positive half-cycles or only the negative half-cycles need to plotted in order to form the full curve. (Equivalently, a complete curve will be graphed by plotting any continuous interval of polar angles that is π radians long such as θ = 0 to θ = π.[7]) Line segments connecting successive peaks will form a regular polygon with an odd number of vertices, and likewise:
    • The roses are symmetric about each line through the pole and a peak (through the middle of a petal) with the polar angle between the peaks of successive petals being 2π/k radians. Thus, these roses have rotational symmetry of order k.
  • The rose’s petals do not overlap.
  • The roses can be specified by algebraic curves of order k + 1 when k is odd, and 2(k + 1) when k is even.[8]

The circle

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A rose with k = 1 is a circle that lies on the pole with a diameter that lies on the polar axis when r = a cos(θ). The circle is the curve's single petal. (See the circle being formed at the end of the next section.) In Cartesian coordinates, the equivalent cosine and sine specifications are

and

respectively.

The quadrifolium

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A rose with k = 2 is called a quadrifolium because it has 2k = 4 petals and will form a square. In Cartesian coordinates the cosine and sine specifications are

and

respectively.

The trifolium

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A rose with k = 3 is called a trifolium[9] because it has k = 3 petals and will form an equilateral triangle. The curve is also called the Paquerette de Mélibée. In Cartesian Coordinates the cosine and sine specifications are

and

respectively.[10] (See the trifolium being formed at the end of the next section.)

The octafolium

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A rose with k = 4 is called an octafolium because it has 2k = 8 petals and will form an octagon. In Cartesian Coordinates the cosine and sine specifications are

and

respectively.

The pentafolium

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A rose with k = 5 is called a pentafolium because it has k = 5 petals and will form a regular pentagon. In Cartesian Coordinates the cosine and sine specifications are

and

respectively.

The dodecafolium

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A rose with k = 6 is called a dodecafolium because it has 2k = 12 petals and will form a dodecagon. In Cartesian Coordinates the cosine and sine specifications are

and

respectively.

Total and petal areas

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The total area of a rose with polar equation of the form r = a cos() or r = a sin(), where k is a non-zero integer, is[11]

When k is even, there are 2k petals; and when k is odd, there are k petals, so the area of each petal is πa2/4k.

As a consequence, if someone wanted to play the popular game He loves me... he loves me not on a rose like above, instead of counting the petals they could calculate the area of the rose to determine the result of the game.

Roses with rational number values for k

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In general, when k is a rational number in the irreducible fraction form k = n/d, where n and d are non-zero integers, the number of petals is the denominator of the expression 1/21/2k = nd/2n.[12] This means that the number of petals is n if both n and d are odd, and 2n otherwise.[13]

  • In the case when both n and d are odd, the positive and negative half-cycles of the sinusoid are coincident. The graph of these roses are completed in any continuous interval of polar angles that is long.[14]
  • When n is even and d is odd, or visa versa, the rose will be completely graphed in a continuous polar angle interval 2 long.[15] Furthermore, the roses are symmetric about the pole for both cosine and sine specifications.[16]
    • In addition, when n is odd and d is even, roses specified by the cosine and sine polar equations with the same values of a and k are coincident. For such a pair of roses, the rose with the sine function specification is coincident with the crest of the rose with the cosine specification at on the polar axis either at θ = /2 or at θ = 3/2. (This means that roses r = a cos() and r = a sin() with non-zero integer values of k are never coincident.)
  • The rose is inscribed in the circle r = a, corresponding to the radial coordinate of all of its peaks.

The Dürer folium

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A rose with k = 1/2 is called the Dürer folium, named after the German painter and engraver Albrecht Dürer. The roses specified by r = a cos(θ/2) and r = a sin(θ/2) are coincident even though a cos(θ/2) ≠ a sin(θ/2). In Cartesian coordinates the rose is specified as[17]

The Dürer folium is also a trisectrix, a curve that can be used to trisect angles.

The limaçon trisectrix

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A rose with k = 1/3 is a limaçon trisectrix that has the property of trisectrix curves that can be used to trisect angles. The rose has a single petal with two loops. (See the animation below.)

Examples of roses r = cos() created using gears with different ratios.
The rays displayed are the polar axis and θ = π/2.
Graphing starts at θ = 2π when k is an integer, θ = 2 otherwise, and proceeds clockwise to θ = 0.
The circle, k = 1 (n = 1, d = 1). The rose is complete when θ = π is reached (half a revolution of the lighter gear).
The limaçon trisectrix, k = 1/3 (n = 1, d = 3), has one petal with two loops. The rose is complete when θ = 3π is reached (3/2 revolutions of the lighter gear).
The trifolium, k = 3 (n = 3, d = 1). The rose is complete when θ = π is reached (half a revolution of the lighter gear).
The 8 petals of the rose with k = 4/5 (n = 4, d = 5) is each, a single loop that intersect other petals. The rose is symmetric about the pole. The rose is complete at θ = 10π (five revolutions of the lighter gear).

Roses with irrational number values for k

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A rose curve specified with an irrational number for k has an infinite number of petals[18] and will never complete. For example, the sinusoid r = a cos(πθ) has a period T = 2, so, it has a petal in the polar angle interval 1/2θ1/2 with a crest on the polar axis; however there is no other polar angle in the domain of the polar equation that will plot at the coordinates (a,0). Overall, roses specified by sinusoids with angular frequencies that are irrational constants form a dense set (that is, they come arbitrarily close to specifying every point in the disk ra).

Rotations required to close the curve

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The number of rotations (or total angular range) required for a rhodonea curve to complete one full closed figure depends on the ratio k = n/d. When k is an integer, the curve closes after π radians if k is odd, and after 2π radians if k is even. When k is a rational number, the total rotation needed for the curve to close is given by /gcd(n,d) if nd is odd, and by 2dπ/gcd(n,d) otherwise. This formula determines how many radians (or loops) are required for the rose curve to complete a full pattern before repeating itself.

See also

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Notes

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Revisions and contributorsEdit on WikipediaRead on Wikipedia
from Grokipedia
In , a , also known as a rhodonea curve or multifolium, is a defined in polar coordinates that produces a flower-like resembling the petals of a . Its standard equation is r=acos(nθ)r = a \cos(n\theta) or r=asin(nθ)r = a \sin(n\theta), where a>0a > 0 determines the radial extent of the petals and nn is a positive that controls the number and arrangement of the petals. The sine version is a 90-degree of the cosine version, and both forms exhibit about the origin. For values of nn, the rose curve traces nn distinct petals if nn is odd and 2n2n petals if nn is even in the cosine form, with the sine form producing equivalent results but potentially rotated. When nn is a expressed as p/qp/q in lowest terms, the curve is algebraic, closing after a finite number of loops with degree p+qp + q if pqpq is odd or 2(p+q)2(p + q) if pqpq is even. If nn is , the curve generates infinitely many overlapping petals and does not close upon itself. The rose curve was first named "rhodonea" by Italian mathematician Guido Grandi between 1723 and 1728, a term derived from the Latin rhodoneus meaning "made of roses," reflecting its distinctive petal shape. It can also be viewed as a special case of a hypotrochoid, a roulette curve generated by a point on a small circle rolling inside a larger fixed circle. Specific instances include the trifolium (n=3n = 3) and quadrifolium (n=2n = 2), which have been studied for their symmetry and use in illustrating polar graphing techniques.

Introduction

Definition

The rose curve, also known as the rhodonea curve or multifolium, is a given by the polar equation r=acos(kθ)r = a \cos(k\theta) or r=asin(kθ)r = a \sin(k\theta), where a>0a > 0 determines the radial extent of the petals and kk is a positive that controls the number and arrangement of the petals. This produces intricate petal-like patterns in the plane, evoking the appearance of a flower. These curves are distinguished by their elegant, symmetric forms, which arise from the interplay of radial and angular components in their construction. The sine version is a 90-degree rotation of the cosine version. Rose curves are generated using sinusoidal functions in polar coordinates, yielding multi-lobed shapes that radiate from the origin. The key parameter kk serves as the , fundamentally determining the number and spatial arrangement of the petals. The entire curve is confined within a bounding of aa centered at the origin, with the petals extending outward to touch this boundary at specific points. This inscription ensures that all features of the rose remain compactly enclosed, highlighting its geometric elegance.

History

The rose curves, known initially as rhodonea curves, were first systematically studied and named by the Italian mathematician and priest Luigi Guido Grandi between 1723 and 1728. Grandi, a professor of mathematics at the University of Pisa, explored these curves in his work on geometric forms, noting their intricate, petal-like patterns that evoked the appearance of roses. He derived the name "rhodonea" from the Greek word rhodon, meaning rose, highlighting their floral resemblance. During Grandi's era, these curves gained early recognition as a specialized variant within the broader family of roulette curves, particularly as special cases of hypotrochoids generated by the rolling of circles. This connection positioned rhodonea curves alongside cycloidal forms, which were prominent in 18th-century studies of rolling motions and pedal curves. Grandi's investigations contributed to the understanding of polar representations, though his primary focus remained on their geometric aesthetics rather than practical uses. Interest in rhodonea curves persisted into the amid growing fascination with polar coordinate systems and symmetric plane curves. This period saw rhodonea integrated into broader treatises on algebraic curves, reflecting the era's emphasis on elegant mathematical visualizations.

Formulation

Polar Equation

The rose curve in polar coordinates is defined by the equations r=acos(kθ)r = a \cos(k\theta) or r=asin(kθ)r = a \sin(k\theta), where a>0a > 0 serves as the scaling factor determining the overall size and k>0k > 0 is a that governs the curve's complexity. To generate the full curve without retracing, the parameter θ\theta is traced over specific intervals depending on whether kk is an odd or even integer: for odd kk, the interval [0,π][0, \pi] suffices to complete the trace, whereas for even kk, the interval [0,2π][0, 2\pi] is necessary. During plotting, negative values of rr are typically interpreted as positive radii at angle θ+π\theta + \pi, or the absolute value r|r| is used to ensure the curve is rendered in the correct quadrants. The parameter aa represents the maximum radial distance from the origin, as cos(kθ)1|\cos(k\theta)| \leq 1 and sin(kθ)1|\sin(k\theta)| \leq 1, confining the entire within the circle of radius aa. The two forms differ in orientation: the cosine version exhibits about the polar axis (θ=0\theta = 0), while the sine version is symmetric about the line θ=π/2\theta = \pi/2, effectively rotating the cosine curve by an angle of π/(2k)\pi/(2k) radians.

Equivalent Forms

The rose curve, defined in polar coordinates as r=acos(kθ)r = a \cos(k\theta), admits a parametric representation in Cartesian coordinates given by
x(θ)=acos(kθ)cos(θ),x(\theta) = a \cos(k\theta) \cos(\theta),
y(θ)=acos(kθ)sin(θ).y(\theta) = a \cos(k\theta) \sin(\theta). This form facilitates analysis in rectangular coordinates, where θ\theta serves as the ranging appropriately to trace the curve.
For the sine-based polar form r=asin(kθ)r = a \sin(k\theta), the analogous parametric equations are
x(θ)=asin(kθ)cos(θ),x(\theta) = a \sin(k\theta) \cos(\theta),
y(θ)=asin(kθ)sin(θ).y(\theta) = a \sin(k\theta) \sin(\theta). These representations highlight the rotational offset between cosine and sine variants, with the sine version rotated by π/(2k)\pi/(2k) relative to the cosine one.
Applying trigonometric product-to-sum identities to the cosine parametric form yields expanded expressions:
x(θ)=a2[cos((k+1)θ)+cos((k1)θ)],x(\theta) = \frac{a}{2} \left[ \cos((k+1)\theta) + \cos((k-1)\theta) \right],
y(θ)=a2[sin((k+1)θ)sin((k1)θ)],y(\theta) = \frac{a}{2} \left[ \sin((k+1)\theta) - \sin((k-1)\theta) \right],
for integer k>1k > 1. Similar expansions apply to the sine version, expressing the curve as a superposition of circular motions.
The rose curve is a special case of the hypotrochoid, obtained when the tracing point lies on the rolling circle's circumference, and also arises as the pedal curve of a hypocycloid with appropriate radius ratios.

Properties

Petal Configuration

The petal configuration of a rose curve, defined by the polar equation r=acos(kθ)r = a \cos(k\theta) or r=asin(kθ)r = a \sin(k\theta), depends primarily on the value of the parameter kk. For integer values of k1k \geq 1, the number of petals is kk if kk is odd and 2k2k if kk is even. These petals are equally spaced angularly, with consecutive petals separated by π/k\pi / k radians. In general, each petal corresponds to a in the polar plane where r0r \geq 0, bounded between consecutive zeros of the trigonometric function cos(kθ)\cos(k\theta) or sin(kθ)\sin(k\theta). The zeros occur where the argument kθk\theta satisfies the equation for the cosine or sine function equaling zero, delineating the extents of each petal. For rational values of k=p/qk = p/q in lowest terms, where pp and qq are positive integers, the number of petals is pp if both pp and qq are odd, and 2p2p otherwise. The curve closes after traversing θ\theta from 0 to πq\pi q if both pp and qq are odd, or to 2πq2\pi q otherwise. For rational non-integer kk, the petals may exhibit overlap or result from the curve looping multiple times before closing, leading to more complex configurations compared to the discrete petals of cases. For kk, the curve does not close.

Symmetry

The rose curve exhibits distinct reflection symmetries depending on whether it is defined using the cosine or function. The cosine form, r=acos(kθ)r = a \cos(k\theta), is symmetric about the polar axis (θ=0\theta = 0), meaning that the curve is invariant under reflection across this axis. In contrast, the form, r=asin(kθ)r = a \sin(k\theta), possesses about the line θ=π/2\theta = \pi/2, reflecting the orientation of its petal arrangement relative to the cosine variant. For integer values of kk, the of the rose curve is determined by the parity of kk. When kk is an odd integer, the curve has rotational symmetry of order kk, achieved by rotations of 2π/k2\pi/k radians around the origin. For even integer kk, the order increases to 2k2k, corresponding to rotations of π/k\pi/k radians. These rotational symmetries, combined with the reflection symmetries, generate the full DkD_k for odd kk and D2kD_{2k} for even kk, which describes the complete set of isometries preserving the curve. When k=p/qk = p/q is rational in lowest terms, the symmetry properties are influenced by both numerator pp and denominator qq, with the curve closing after a period of πq\pi q if both pp and qq are odd, or 2πq2\pi q otherwise, enabling a finite periodic structure. In such cases, the rotational symmetry order reduces to a value tied to pp and qq, typically the number of distinct lobes, while the overall group remains dihedral, though of lower order than in the irrational case where no finite rotational symmetry exists beyond order 2. The value of kk also affects the overall orientation and perceived symmetry of the rose curve; for even integer kk, the doubled petal count relative to odd kk produces a "star-like" configuration with enhanced rotational redundancy, emphasizing the 2k-fold symmetry that aligns with the D2kD_{2k}.

Area

Total Area

The total area enclosed by the rose curve r=acos(kθ)r = a \cos(k\theta) (or equivalently r=asin(kθ)r = a \sin(k\theta)) is given by the standard polar area formula A=120Tr2(θ)dθ,A = \frac{1}{2} \int_0^T r^2(\theta) \, d\theta, where TT is the angular interval over which the curve is traced once without retracing. For integer kk, this interval is T=πT = \pi when kk is odd and T=2πT = 2\pi when kk is even. Substituting the polar equation from the formulation section, r2(θ)=a2cos2(kθ)=a22(1+cos(2kθ))r^2(\theta) = a^2 \cos^2(k\theta) = \frac{a^2}{2} \left( 1 + \cos(2k\theta) \right). The integral simplifies to A=a240T(1+cos(2kθ))dθ=a24[θ+sin(2kθ)2k]0T.A = \frac{a^2}{4} \int_0^T \left( 1 + \cos(2k\theta) \right) d\theta = \frac{a^2}{4} \left[ \theta + \frac{\sin(2k\theta)}{2k} \right]_0^T. The sine term evaluates to zero at the limits, yielding A=a2T4A = \frac{a^2 T}{4}. Thus, for odd kk, A=πa24A = \frac{\pi a^2}{4}; for even kk, A=πa22A = \frac{\pi a^2}{2}. For non-integer kk, the curve closes after a period determined by the denominator in reduced form k=p/qk = p/q, leading to a more complex over T=2πqT = 2\pi q, but the resulting area follows analogous forms adjusted for the rational multiple, though computation is generally less simplified.

Individual Petal Area

The area of an individual in a rose curve defined by the polar equation r=acos(kθ)r = a \cos(k\theta), where kk is a positive , is computed using the standard polar area formula 12r2dθ\frac{1}{2} \int r^2 \, d\theta over the angular interval spanning one . For the central aligned with the positive x-axis, this interval is from θ=π2k\theta = -\frac{\pi}{2k} to θ=π2k\theta = \frac{\pi}{2k}, where r0r \geq 0. Substituting the equation yields the 12π/(2k)π/(2k)a2cos2(kθ)dθ.\frac{1}{2} \int_{-\pi/(2k)}^{\pi/(2k)} a^2 \cos^2(k\theta) \, d\theta. Using the identity cos2(kθ)=1+cos(2kθ)2\cos^2(k\theta) = \frac{1 + \cos(2k\theta)}{2}, the simplifies to a22π/(2k)π/(2k)1+cos(2kθ)2dθ=a24[θ+sin(2kθ)2k]π/(2k)π/(2k)=a24πk=πa24k\frac{a^2}{2} \int_{-\pi/(2k)}^{\pi/(2k)} \frac{1 + \cos(2k\theta)}{2} \, d\theta = \frac{a^2}{4} \left[ \theta + \frac{\sin(2k\theta)}{2k} \right]_{-\pi/(2k)}^{\pi/(2k)} = \frac{a^2}{4} \cdot \frac{\pi}{k} = \frac{\pi a^2}{4k}. Due to the rotational symmetry of the rose curve, all petals possess identical areas when kk is an ; specifically, there are kk petals if kk is odd and 2k2k petals if kk is even, making the total area the product of the number of petals and the individual area. This uniformity arises from the periodic nature of the cosine function, ensuring equivalent contributions from each symmetric lobe. For rational k=p/qk = p/q in lowest terms, the computation of per-petal area follows a similar integration approach over appropriate angular sectors, but the presence of self-intersections and overlaps complicates the isolation of distinct "petals," preventing a straightforward simplification akin to the integer case.

Integer k Cases

k = 1: Circle

When k=1k = 1, the rose curve degenerates into a , representing the simplest case in the family of rose curves without any multi-lobed structure. The polar is given by r=acosθr = a \cos \theta, where a>0a > 0 determines the scale. To derive the equivalent Cartesian form, start with the polar and multiply by rr:
r2=arcosθ.r^2 = a r \cos \theta.
Substitute r2=x2+y2r^2 = x^2 + y^2 and x=rcosθx = r \cos \theta:
x2+y2=ax.x^2 + y^2 = a x.
Rearrange and complete the square in xx:
x2ax+y2=0,x^2 - a x + y^2 = 0,
(xa2)2+y2=(a2)2.\left( x - \frac{a}{2} \right)^2 + y^2 = \left( \frac{a}{2} \right)^2.
This describes a of radius a/2a/2 centered at (a/2,0)(a/2, 0). The curve is interpreted as a single "petal" forming the full , serving as the base case for the rose family.
As θ\theta varies from 00 to 2π2\pi, the circle is traced twice, a feature particular to this degenerate case. The area enclosed by this circle is π(a/2)2=πa2/4\pi (a/2)^2 = \pi a^2 / 4, which aligns with the general formula for the area of one petal in odd-kk rose curves.

k = 2: Quadrifolium

The quadrifolium is a four-petaled rose curve arising when k=2k = 2 in the polar equation r=acos(kθ)r = a \cos(k\theta), featuring four equal lobes symmetrically positioned along the coordinate axes at angles θ=0\theta = 0, π/2\pi/2, π\pi, and 3π/23\pi/2. This configuration distinguishes it as a classic example of an even-kk rose, where the even value doubles the number of petals to 2k=42k = 4 compared to the odd case. The complete quadrifolium is traced as θ\theta varies from 0 to 2π2\pi. The resulting implicit Cartesian equation is (x2+y2)3=a2(x2y2)2(x^2 + y^2)^3 = a^2 (x^2 - y^2)^2, which eliminates the polar parameters and reveals the curve as a sextic . The total enclosed area of the quadrifolium is πa2/2\pi a^2 / 2, equivalent to half the area of the of radius aa. Each individual petal occupies an area of πa2/8\pi a^2 / 8, reflecting the uniform division among the four lobes.

k = 3: Trifolium

The trifolium, corresponding to the rose curve with k=3k=3, exhibits a three-petaled resembling a three-leaf or , with petals oriented at 120° intervals along the directions θ=0\theta = 0, θ=2π/3\theta = 2\pi/3, and θ=4π/3\theta = 4\pi/3. This configuration arises from the polar equation r=acos(3θ)r = a \cos(3\theta), where the petals extend to a maximum radius of aa along these axes. The curve is fully traced as θ\theta varies from 0 to 2π2\pi, covering all three petals without overlap or additional structure in the second half of the interval. In Cartesian coordinates, the trifolium is represented by the equation (x2+y2)2=ax(x23y2)(x^2 + y^2)^2 = a x (x^2 - 3 y^2), forming an algebraic curve of degree 4. It serves in geometric constructions, such as the pedal curve of a deltoid with respect to its center or as a hypotrochoid generated by a circle of radius R/4R/4 rolling inside a fixed circle of radius RR with the tracing point at distance R/4R/4 from the rolling center. The total area enclosed by the trifolium is πa2/4\pi a^2 / 4, equivalent to one-quarter the area of the circumscribed disk of aa; each individual has an area of πa2/12\pi a^2 / 12.

k ≥ 4: General Patterns

For values of k4k \geq 4, rose curves exhibit increasingly complex petal arrangements while adhering to the fundamental pattern where the number of petals is kk if kk is odd and 2k2k if kk is even. When kk is even, such as k=4k=4, the resulting octafolium displays 8 petals arranged in a star-like configuration around the origin. For k=6k=6, the dodecafolium features 12 , illustrating a progression toward greater petal density with each increment in kk. These even-kk cases produce visually intricate, radially symmetric forms that evoke a multi-pointed , with the completing its trace over the full interval of 00 to 2π2\pi. In contrast, for odd k5k \geq 5, the curves maintain a single continuous tracing over 00 to 2π2\pi, yielding exactly kk distinct petals without overlap. The pentafolium at k=5k=5 consists of 5 petals, while at k=7k=7, 7 petals emerge, each symmetrically positioned and unattached to others beyond the origin. Across all integer k4k \geq 4, a consistent trend emerges: as kk increases, the petals grow narrower and more numerous, enhancing the curve's overall density while preserving rotational symmetry of order kk (or 2k2k for even cases). Notably, these integer-kk roses exhibit no self-intersections apart from repeated passages through the origin, ensuring a clean, non-overlapping petal structure that contrasts with the behaviors observed in non-integer cases. The total enclosed area is πa2/4\pi a^2 / 4 for odd kk and πa2/2\pi a^2 / 2 for even kk, independent of the specific value of kk (beyond parity), while proportional to a2a^2, as detailed in the area section.

Rational k Cases

General Form for k = p/q

When k=p/qk = p/q is a rational number expressed in lowest terms with pp and qq positive integers and gcd(p,q)=1\gcd(p, q) = 1, the rose curve defined by the polar equation r=acos(kθ)r = a \cos(k \theta) or r=asin(kθ)r = a \sin(k \theta) exhibits distinct closure and structural properties compared to integer cases. The curve forms a finite, closed path due to the periodicity of the trigonometric functions involved. Specifically, the curve completes its full tracing after the polar angle θ\theta ranges from 0 to πqm\pi q m, where m=1m = 1 if both pp and qq are odd, and m=2m = 2 otherwise; this ensures the path returns to the origin without further new segments. The number of petals in the resulting rhodonea curve follows a precise rule based on the parity of pp and qq: there are pp petals if both are odd, and 2p2p petals otherwise. This configuration arises because negative values of rr in polar coordinates correspond to points in the opposite direction, effectively doubling the petal count when even is present. Depending on the values of pp and qq, the curve may feature self-intersections or looped structures, where petals overlap or cross themselves, contributing to its intricate, flower-like appearance. Regarding periodicity, the rose function repeats every T=πqT = \pi q if both pp and qq are odd, producing the complete in that interval, or every T=2πqT = 2 \pi q otherwise; since p/qp/q is in lowest terms, this represents the fundamental period without redundant tracing. Algebraically, the rose is an of degree p+qp + q when both pp and qq are odd, and degree 2(p+q)2(p + q) in all other cases, reflecting its representation as a equation in Cartesian coordinates after eliminating the polar parameters.

k = 1/2: Dürer Folium

The rose curve with parameter k=12k = \frac{1}{2} is defined by the polar equation r=acos(θ2)r = a \cos\left( \frac{\theta}{2} \right), where a>0a > 0 is a scaling constant. This equation generates a two-petaled figure with looping and self-intersection in the structure as the radius vector traces the curve. The curve, known as the Dürer folium, is associated with the geometric studies of the German artist and mathematician Albrecht Dürer (1471–1528), who explored similar roulette curves in his treatise Underweysung der Messung (1525). The number of petals is two because k=pq=12k = \frac{p}{q} = \frac{1}{2} in lowest terms, with p=1p = 1 odd and denominator q=2q = 2 even, yielding 2p=22p = 2 distinct petals arranged symmetrically around the origin. The full curve closes after θ\theta ranges from 0 to 4π4\pi, corresponding to two full rotations of the radius vector, due to the even denominator requiring an extended angular period to complete without redundancy. A notable geometric of the Dürer folium is its use as a trisectrix, allowing the trisection of an arbitrary through polar constructions involving intersections with the and an auxiliary centered at the origin of appropriate , producing points whose angles relate by a factor of one-third. This property stems from the 's epitrochoid generation with rolling ratio parameters leading to the fractional angular multiplier 12\frac{1}{2}, facilitating the division in measurements.

k = 1/3: Limaçon Trisectrix

The rose curve with k=1/3k = 1/3 is given by the polar equation r=acos(θ/3)r = a \cos(\theta/3), where a>0a > 0 is a scaling parameter. This equation generates a curve classified as the , a special case of the rose family that exhibits looped structures. The plot traces a single effective petal due to the rational form k=p/q=1/3k = p/q = 1/3 with both numerator and denominator odd, consistent with the general petal-counting rule for rational rose curves. The shape features one main outer petal accompanied by two inner loops, closely resembling a of Pascal, and the full curve closes after θ\theta ranges from 0 to 3π3\pi, as the general rule for both odd p,q dictates πq=3π\pi q = 3\pi to complete the distinct path (though the function repeats every 6π6\pi). This configuration arises from the fractional multiplier, causing the polar radius to oscillate and intersect itself, producing the characteristic looped appearance without additional windings beyond the closure point. A defining property of this curve is its utility in geometric : to trisect an angle ϕ\phi, a ray from the origin at angle ϕ\phi intersects the curve at a point P, and using an auxiliary of equal to the fixed distance (often related to a), the intersections yield points dividing the angle into three equal parts via the curve's parametric relation. This trisection capability stems from the 1/31/3 factor in the argument, allowing proportional angular divisions through polar intersections.

Irrational k Cases

Non-Periodic Behavior

When the parameter kk in the rose curve r=cos(kθ)r = \cos(k\theta) or r=sin(kθ)r = \sin(k\theta) is , the resulting curve exhibits fundamentally non-periodic behavior, failing to close upon itself after any finite interval of the polar angle θ\theta. Unlike the finite, repeating patterns observed in rational or cases, an kk produces a path that continues indefinitely without repetition, effectively requiring θ\theta to extend to to trace the full structure. This non-periodicity arises from the winding of the argument kθmod2πk\theta \mod 2\pi, which generates points densely distributed throughout the interval [0,2π)[0, 2\pi) as θ\theta increases. Since kk is irrational, the sequence {knmod2π}\{k n \mod 2\pi\} for integer nn (approximating the continuous sweep) is equidistributed in [0,2π)[0, 2\pi), ensuring that the angular progression never aligns periodically with the initial position. In contrast to rational k=p/qk = p/q in lowest terms, where the curve closes after a finite period of 2πq2\pi q, the irrational case yields infinitely many "petals" that do not overlap or repeat, creating an unending spiral-like extension within the bounding circle. Plotting such curves presents practical challenges, as no finite range of θ\theta can capture the complete form; visualizations typically approximate the behavior over large intervals, such as θ[0,100π]\theta \in [0, 100\pi], but remain inherently incomplete representations of the infinite .

Density Properties

For rose curves defined by the polar r=acos(kθ)r = a \cos(k \theta) where kk is , the image of the is dense in the closed disk of radius aa centered at the origin. This topological density means that the comes arbitrarily close to every point within the disk as θ\theta ranges over the reals, without ever forming a closed loop or discrete . Unlike rational kk, which yield finite or periodic patterns, the irrational case produces an infinite, non-repeating sequence of petal-like lobes that collectively fill the without gaps in the limit. The density stems from the dynamics on the 2-torus [0,2π)×[0,2π)[0, 2\pi) \times [0, 2\pi), where the parametrization maps θ\theta to (θmod2π,kθmod2π)(\theta \mod 2\pi, k\theta \mod 2\pi). Since kk is irrational, this induces a dense winding on the torus, as the orbit is both dense and equidistributed by the Weyl equidistribution theorem for irrational rotations. The subsequent continuous mapping (ϕ,ψ)acos(ψ)(cosϕ,sinϕ)(\phi, \psi) \mapsto a \cos(\psi) (\cos \phi, \sin \phi) sends the torus to the disk, preserving density: the preimage of any open set in the disk intersects the dense orbit, ensuring the curve's points are dense throughout. This extends the non-periodic behavior to a geometric filling property, where no finite number of iterations captures the full structure. The equidistribution on the implies that curve points approximate the disk uniformly in the ergodic sense, but the radial distribution induced by r=acos(kθ)r = a |\cos(k\theta)| results in uneven point : higher concentrations occur near (r0r \approx 0) and the boundary (rar \approx a), reflecting the probability of cosψ|\cos \psi| under the uniform measure on ψ\psi. In practice, computational plots for specific values like k=2k = \sqrt{2}
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