Viscoelastic Fluid
Click-drag the blob to deform it β€” fast deformation is elastic (snaps back), slow deformation is viscous (flows). Compare three rheological models.
Model Maxwell
Modulus Gβ‚€ (kPa) 10.0
Viscosity Ξ· (kPaΒ·s) 5.0
SLS spring ratio Ξ± 0.50
0.50
Ο„α΄Ώ relaxation (s)
β€”
Deborah number
β€”
Gβ€² storage (kPa)
β€”
Gβ€³ loss (kPa)
β€”
tan Ξ΄
How it works: A viscoelastic material has both springlike (elastic) and dashpot-like (viscous) elements. The Deborah number De = Ο„α΄Ώ/t_obs separates behaviour: De > 1 β†’ solid-like; De < 1 β†’ liquid-like.
Maxwell (spring + dashpot in series): dΡ/dt = σ/η + (1/G₀)·dσ/dt → exponential stress relaxation, infinite creep.
Kelvin-Voigt (spring + dashpot in parallel): Οƒ = Gβ‚€Ξ΅ + Ξ·Β·dΞ΅/dt β†’ retarded elastic creep, no stress relaxation.
Standard Linear Solid combines both: finite relaxation and finite creep, with plateau modulus Gβ‚€Β·Ξ±.

Left panel: 10Γ—10 particle blob with Maxwell springs β€” drag to deform. Colour = local stress magnitude (blueβ†’red).   Right panel: selected test curve (analytical) β€” drag the Ο‰-slider in Frequency Sweep mode.