List of centroids

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The following is a list of centroids of various two-dimensional objects. A centroid of an object X in n-dimensional space is the intersection of all hyperplanes that divide X into two parts of equal moment about the hyperplane. Informally, it is the "average" of all points of X. For an object of uniform composition (mass, density, etc.) the centroid of a body is also its centre of mass. In the case of two-dimensional objects shown below, the hyperplanes are simply lines.

Centroids

Shape Figure \bar x \bar y Area
Right-triangular area 200px \frac{b}{3} \frac{h}{3} \frac{bh}{2}
Quarter-circular area[1] 200px \frac{4r}{3\pi} \frac{4r}{3\pi} \frac{\pi r^2}{4}
Semicircular area[2] 200px \,\!0 \frac{4r}{3\pi} \frac{\pi r^2}{2}
Quarter-elliptical area 200px \frac{4a}{3\pi} \frac{4b}{3\pi} \frac{\pi a b}{4}
Semielliptical area 200px \,\!0 \frac{4b}{3\pi} \frac{\pi a b}{2}
Semiparabolic area The area between the curve y = \frac{h}{b^2} x^2 and the \,\!y axis, from \,\!x = 0 to \,\!x = b \frac{3b}{8} \frac{3h}{5} \frac{2bh}{3}
Parabolic area The area between the curve \,\!y = \frac{h}{b^2} x^2 and the line \,\!y = h \,\!0 \frac{3h}{5} \frac{4bh}{3}
Parabolic spandrel The area between the curve \,\!y = \frac{h}{b^2} x^2 and the \,\!x axis, from \,\!x = 0 to \,\!x = b \frac{3b}{4} \frac{3h}{10} \frac{bh}{3}
General spandrel The area between the curve y = \frac{h}{b^n} x^n and the \,\!x axis, from \,\!x = 0 to \,\!x = b \frac{n + 1}{n + 2} b \frac{n + 1}{4n + 2} h \frac{bh}{n + 1}
Circular sector 200px \frac{2r\sin(\alpha)}{3\alpha} \,\!0 \,\!\alpha r^2
Circular segment 200px \frac{4r\sin^3(\alpha)}{3(2\alpha-\sin(2\alpha))} \,\!0 \frac{r^2}{2}(2\alpha -\sin(2\alpha))
Quarter-circular arc The points on the circle \,\!x^2 + y^2 = r^2 and in the first quadrant \frac{2r}{\pi} \frac{2r}{\pi} L=\frac{\pi r}{2}
Semicircular arc The points on the circle \,\!x^2 + y^2 = r^2 and above the \,\!x axis \,\!0 \frac{2r}{\pi} L=\,\!\pi r
Arc of circle The points on the curve (in polar coordinates) \,\!r = \rho, from \,\!\theta = -\alpha to \,\!\theta = \alpha \frac{\rho\sin(\alpha)}{\alpha} \,\!0 L=\,\!2\alpha \rho

See also

References

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External links

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