The surface deformation of hydrogels is important because it can result in self-induced cracking. Each hydrogel has a characteristic wavelength of instability (λ) that depends on elastocapillary length. This length is calculated by dividing the surface tension (γ) by the elasticity (μ) of the hydrogel. The greater the wavelength of instability, the greater the elastocapillary length of instability, which makes a material more prone to cracking. The characteristic wavelength of instability can be modeled by:
Where H is the thickness of the hydrogel.