Summary of nonlinear behavior in variants of the recruitment component RD model
| Model variant | A | B | C | D | E | F | G | H |
| Starting model: | ✓ | — | — | — | — | — | — | — |
| Velocity-dependent recruitment: | — | — | — | — | ✓ | — | — | — |
| Distortion-dependent recruitment: | ||||||||
| ✓ | — | — | — | ✓ | — | — | — | |
| ✓ | ✓ | ✓ | — | — | — | — | ✓ | |
| ✓ | ✓ | ✓ | ✓ | ✓ | — | ✓ | ✓ | |
| Model variant | A | B | C | D | E | F | G | H |
| Starting model: | ✓ | — | — | — | — | — | — | — |
| Velocity-dependent recruitment: | — | — | — | — | ✓ | — | — | — |
| Distortion-dependent recruitment: | ||||||||
| ✓ | — | — | — | ✓ | — | — | — | |
| ✓ | ✓ | ✓ | — | — | — | — | ✓ | |
| ✓ | ✓ | ✓ | ✓ | ✓ | — | ✓ | ✓ | |
linear F1 versus ΔL relationship and linear FSS versus ΔL relationship; B, difference in shape between large-amplitude quick stretch (rapid fall to a well-defined nadir, followed by a slower rise to an eventual steady state) and large-amplitude quick release (monotonic rise to the eventual steady state); C, difference in pattern among various amplitude quick stretches (trajectories tend to converge at a common nadir) and various amplitude quick releases (trajectories remain apart and distinct); D, difference in shape between small-amplitude (rapid rise to a zenith, followed by a slower fall to eventual steady state) and large-amplitude (monotonic rise to the eventual steady state) quick releases; E, quasi–mirror image responses of small-amplitude quick stretch and quick release; F, curvilinear up in F23 versus ΔL relationship; G, downward trend in T23 versus ΔL relationship, indicating that approach to nadir in response to large ΔL is faster than approach to nadir in response to small ΔL; H, downward trend in T90 versus ΔL relationship.