Question 1 - Non-Newtonian Fluids Flashcards
fluid does not follow Newton’s law: viscosity is not constant but dependant upon the shear rate
non-Newtonian fluids
shear viscosity for Newtonian fluid
ratio of shear strees to shear rat and hap netween the plates H.
τ = η𝛾
τ = shear stress
η = dynamic viscosity
𝛾 = shear rate
shear viscosity for non-Newtonian fluid
η=η𝛾
τ = η𝛾𝛾
τ = shear stress
η = dynamic viscosity
𝛾 = shear rate
viscosity decreases when increasing the shear rate.
These fluids display a constant-viscosity value of the viscosity at low shear rate values followed by a decrease of the viscosity when increasing further the shear rate
shear thinning
viscosity increases when increasing the shear rate.
These fluids display a constant viscosity value at low shear rate value is followed by an increase of the viscosity when increasing the shear rate.
shear thickening
Do not flow is the applied stress is below a critical threshold called yield stress. Above this critical stress, the fluids flow with a shear stress directly proportional to the shear rate
Bingham fluid
critical threshold of applied stress needed to make Bingham fluids flow
Yield Stress
Shear thinning: ________ decreases when increasing the shear rate.
viscosity
Shear thinning: viscosity decreases when increasing the ________.
shear rate
Power Law Model equation
η = K𝛾 ^(n-1)
η = dynamic viscosity
K = consistency
𝛾 = shear rate
n = power law index
What η represents
shear viscosity
What K represents in power law
consistency
What 𝛾 represents
Shear rate
What n represents in power law model
power law index
Cross Model equation
η = (η0 - η∞)/ 1+(K𝛾)^m
η = dynamic viscosity
η0 = zero-shear viscosity
η∞ = infinite shear viscosity
K = time constant
𝛾 = shear rate
m = dimensionless constant used to modulate the transition between the zero shear constant viscosity reion to the shear thinning region
What η∞ represents
infinite shear viscosity
What K represents in cross model
time constant
What η0 represents
zero-shear viscosity
What m represents in cross model
dimensionless constant used to modulate the transition between the zero shear constant viscosity reion to the shear thinning region
extension of the Cross model with one additional parameter
employed to better describe the transition between constant-viscosity and shear-thinning
region
Carreau - Yasuda model
Carreau-Yasuda model
η = (η0 - η∞)/ (1+(K𝛾)^a)^(n-1/n)
η = dynamic viscosity
η0 = zero-shear viscosity
η∞ = infinite shear viscosity
K = time constant
𝛾 = shear rate
n = dimensionless constant used to modulate the transition between the zero shear constant viscosity reion to the shear thinning region
a = additional parameter to smoothen the transition to shear thinning
Bingham model
τ = τy + 𝜂𝑝𝛾
np = plastic viscosity
τy = yield stress
polymers that do not present a charge on the chain itself
neutral polymers
polymers that carry electric charges on the chain
polyelectrolytes
poor solvents + neutral polymers
polymer collapses into dense coils
θ solvent + neutral polymers
intra-chain interactions are balanced by polymer-solvent interactions. Polymer conformation is a random coil
good solvent + neutral polymer
pollymers are swelled in solution. Polymer conformation is a swollen random coil
polyelectrolytes with no salt
charges on polymer exert steric repulsion and the polymer conformation is extended