$$\rightleftharpoonup{xx}$$
$$\longleftharp{xx}$$,
$$\longrightharp{xx}$$,
Nonlinear continuum mechanics has provided a critical lens through which to understand the concentration of energy that leads to failure in soft solids1. However, the accurate prediction of this failure also requires descriptions of the microstructural characteristics that contribute to new surface creation at the crack tip2,3. One method to approach such descriptions is through in situ visualization of the crack tip during failure4,5. However, crack blunting in typical far-field fracture tests makes the acquisition of in situ data challenging by spreading out the highly deformed material, potentially outside the microscope's field of view6. Y-shaped cutting offers a unique alternative for microstructural visualization because it concentrates the region of large deformation at the tip of a blade7. Furthermore, previous work from our group demonstrates that this unique experimental approach can provide insight into the differences in failure response between far-field tearing and contact-mediated loading conditions7.
The Y-shaped cutting method used in the apparatus presented here was first described decades ago as a cutting method for natural rubber8. The method consists of a fixed blade push-cutting through a preloaded Y-shaped test piece. At the intersection of the "Y" is the crack tip, which is created prior to testing by splitting a portion of a rectangular piece into two equal "legs" (Figure 1B and Figure 2D). The primary advantages of this cutting method include the reduction of frictional contributions to the measured cutting energy, the variable blade geometry (i.e., constraint of the crack tip geometry), the control of the failure rate (via the sample displacement rate), and the separate tuning of the cutting, C, and tearing, T, energy contributions to the total energy Gcut (i.e., altering the failure energy in excess of a cutting threshold)8. The latter contributions are expressed in a simple, closed-form expression for the cutting energy9
Eqn (1)
which uses experimentally selected parameters, including sample thickness, t, average leg strain,
, preload force, fpre, and the angle between the legs and the cutting axis, θ. The cutting force, fcut, is measured with the apparatus as detailed in Zhang et al.9. Notably, the apparatus presented here includes a new, simple, and accurate mechanism for tuning the leg angle, θ, and ensuring the sample is centered. While both features are critical for a microscope-mounted setup, the mechanism may benefit future vertical implementations of the Y-shaped cutting test as well by increasing the ease of use.
Progress in determining the appropriate failure criteria for soft solids has been ongoing since the early success of sample-independent fracture geometries introduced by Rivlin and Thomas10. Critical energy release rates10, cohesive zone laws11, and various forms of stress- or energy-at-a-distance approaches12,13,14 have been used. Recently, Zhang and Hutchens leveraged the latter approach, demonstrating that Y-shaped cutting with sufficiently small radius blades could yield threshold failure conditions for soft fracture7: a threshold failure energy and a threshold length scale for failure that ranges from tens to hundreds of nanometers in homogeneous, highly-elastic polydimethylsiloxane (PDMS). These results were combined with continuum modeling and scaling theory to develop a relationship between cutting and tearing in these materials, thus demonstrating the utility of Y-shaped cutting for providing insights into all modes of soft failure. However, the behavior of many material classes, including dissipative and composite materials, remains unexplored. It is anticipated that many of these will exhibit microstructure-governed effects at length scales above the wavelength of visible light. Therefore, an apparatus was designed in this study that allows for the close visual characterization of these effects during Y-shaped cutting for the first time (e.g., in composites, including soft tissues, or of dissipative processes, anticipated on the micrometer to millimeter length scales15).