Figure 2:

Variation of the shear elastic modulus $G_{\text{s}}$ of the Skalak (SK), neo-Hookean (NH) and Yeoh (YE) laws, scaled with the shear elastic modulus of Evans law $\left(G_{\text{s}}^{\text{EV}}\right)$, with regard to the dimensionless aspiration length $L_{\text{asp}}/R_{\text{pip}}$, so that all constitutive laws result the same micropipette suction pressure $\text{Δ}P$.