Yoshimura buckling
Yoshimura buckling, named after Japanese researcher Yoshimaru Yoshimura, is a triangular mesh buckling pattern found in thin-walled cylinders under compression along the axis of the cylinder that produces corrugated shape resembling the Schwarz lantern. This is the same pattern on found on the sleeves of Mona Lisa. Due to its axial stiffness and origami-like ability, it is being researched in applications such as aerospace, civil engineering, and robotics in addressing problems relating to compactness and rapid deployment. However, broader use is currently limited by the absence of a general mathematical framework.
History
In 1941, crease patterns in cylindrical shells were first studied by Theodore von Kármán and Hsue-Shen Tsien at the California Institute of Technology, and was later independently studied by Yoshimaru Yoshimura in a 1951 Japanese paper, with an English version published in 1955. Isolation of Japan during and after World War II made Yoshimura unaware of the earlier work.Mathematical derivation
Compatibility condition
The compatibility condition of the buckling pattern is given by:where and represent the first and second fundamental forms of the deflection surface, respectively. represents the Gaussian curvature, which is expressed as:
where and are the principal radii of curvature of the cylinder. is expressed as:
where is the length of the buckle in the circumferential direction divided by the length of the buckle in the axial direction.
- On the undeformed initial surface, the Gaussian curvature of the cylinder is 0, satisfying the compatibility condition.
- On the deformed surface, it is observed that the surface is nearly developable. Consequently, the Gaussian curvature of the cylinder is close to 0. Since the left side of the first compatibility condition is already small, the compatibility condition is satisfied.
Buckling load prediction
where represents the ratio of the cylinder wall thickness to the radius, and and represent the Young's modulus and Poisson ratio, respectively. This classical formula is occasionally referred to as Koiter's formula after Dutch engineer Warner T. Koiter, who derived it in 1945, but was first derived by R. Lorenz in 1911.
Experimental results have shown that this classical formula frequently overestimates the buckling load by a factor of 4 to 5. This discrepancy is often attributed to the buckling load's high sensitivity to imperfections in the structure's shape and load.
Conditions for equilibrium
Under a Cartesian coordinate system, the equilibrium conditions for a cylinder under axial compression can be expressed as:where and are the Young's modulus and flexural rigidity, respectively. is derived from the second equation, and can be expressed as:
with as the parameters. This carefully selected method allows for the following methods of simplication:
- — when. Represents axial and circumferential waves.
- when. Represents a variation of diamond shaped buckles.
Characteristics
Folding pattern
The Yoshimura folding pattern is composed of isosceles triangles that share a single edge at the base, forming repeated rhombuses, as seen in the Schwarz lantern crease pattern. Slightly different buckling patterns can occur based on manipulating the angles and dimensions of the individual triangles. The crease pattern for folding the Schwarz lantern from a flat piece of paper, a tessellation of the plane by isosceles triangles, has also been called the Yoshimura pattern based on the same work by Yoshimura. The Yoshimura creasing pattern is related to both the Kresling and Hexagonal folds, and can be framed as a special case of the Miura fold. Unlike the Miura fold which is rigidly deformable, both the Yoshimura and Kresling patterns require panel deformation to be folded to a compact state.Local buckling
Cylindrical shells under axial compression have been observed to exhibit local buckling, provided that they are comparatively long. Local buckling is a phenomenon where a structure undergoes local deformation, as opposed to Euler buckling, which is a deformation of the whole structure. Consequently, lengthwise along the cylinder, the buckling occurs at over 1.5 times the lobe's axial wavelength. Circumference-wise, both the cylinder and loading equipment must have complete rotational symmetry to affect the cylinder's entire circumference.This phenomenon can be further explained as a loss of total elastic energy. Considering a cylinder with fixed ends under Euler's critical load, the elastic energy decrease of the unbuckled region will overpower the increase in elastic energy of the buckled region when local buckling occurs. This results in a loss of total elastic energy.
High imperfection sensitivity
The critical buckling load of cylindrical shells under axial compression is highly sensitive to imperfections in the shape and load. With respect to the asymptotic formula from classical shell theory, where is the shell's dimensionless thickness, the buckling load approximately scales in two different ways:- for imperfections in shape.
- for imperfections in load.
Developable surface
Applications
Yoshimura buckling and its related origami patterns' possible applications have been researched, but their use in engineering remains limited. Current Yoshimura origami designs lack an overarching mathematical theory between the two dimensional creases, and three-dimensional forms. The absence of a unified theory makes it difficult for a general design method to be formulated, and current designs are extremely specific to its application.Additional research for its potential uses in engineering is still in development; researchers are attempting to develop an intuitive parametric method and general numerical theorem to tweak existing Yoshimura designs for engineering efficiency. Currently, engineering attempts to develop a deployable cylindrical structure with Yoshimura folding have only been made for membrane structures, such as soft pneumatic actuators.