Gyroelongated square bicupola

Given that the edge length ${\displaystyle a}$, the surface area is: $${\displaystyle \left(10+6{\sqrt {3}}\right)a^{2}\approx 20.392a^{2},}$$ the total area of twenty equilateral triangles and ten squares. Its volume is: $${\displaystyle \left(2+{\frac {4}{3}}{\sqrt {2}}+{\frac {2}{3}}{\sqrt {4+2{\sqrt {2}}+2{\sqrt {146+103{\sqrt {2}}}}}}\right)a^{3}\approx 8.154a^{3},}$$ the total volume of two square cupolae and an octagonal antiprism.^[2] Its dihedral angles can be calculated by adding the components of cupolae and antiprism. The dihedral angle of antiprism between two adjacent triangles is approximately ${\displaystyle 153.9^{\circ }}$. The dihedral angle of each cupola between two squares is ${\displaystyle 135^{\circ }}$, and that between triangle and square is ${\displaystyle 144.7^{\circ }}$. The dihedral angle of the cupolae and antiprism between two adjacent triangles and triangle-square is ${\displaystyle 151.3^{\circ }}$ and ${\displaystyle 141.6^{\circ }}$, respectively.^[4]

The gyroelongated square bicupola is one of five Johnson solids, which is chiral, meaning that they have a "left-handed" and a "right-handed" form. In the following illustration, each square face on the left half of the figure is connected by a path of two triangular faces to a square face below it and on the left. In the figure of opposite chirality (the mirror image of the illustrated figure), each square on the left would be connected to a square face above it and on the right. These two chiral forms are not considered different Johnson solids.^{[citation needed]} It has the symmetry of dihedral group ${\displaystyle D_{4}}$.^[4]

• Weisstein, Eric W., "Gyroelongated square bicupola" ("Johnson solid") at MathWorld.