Rheology Flashcards

1
Q

Rheology

A

Is the study of flow properties of material

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2
Q

Viscosity

A

The resistance of a fluid to flow when it is subjected to stress

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3
Q

It is important to understand rheology properties of material because they affect

A

It is important to understand the rheological properties of materials because they affect the following:

Efficiency of mixing
Flow through pipes
Ease of packaging into and removal from containers
Physical stability of preparation
Rate of drug absorption
Spreading and adherence of preparation to skin

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4
Q

Formula

Shear stress
Shear rate

Viscosity

A
Stress = F/A
Rate = dv/dr 
dv= difference of velocity between two planes of liquid
dr= distance between two planes of liquid 

Viscosity = stress / rate

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5
Q

Rate unit

A

S^-1

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6
Q

Stress unit

A

Nm^-2

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7
Q

Newtonian fluid

Properties and formula

A

F/A = n dv/dr

n = coefficient of viscosity
Shear rate is directly proportional to shear stress

The flow curve / rheogram
Shows a straight line passing thru origin

Newtonian fluid have Constant viscosity

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8
Q

Rheogram axis

A

Stress (y) against rate (x)
n= Gradient = viscosity

Rate (y) against stress (x)
n= 1 / gradient

n = dynamic viscosity

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9
Q

Example of Newtonian fluid

A
Water
Organic solvent
Oils
True solution 
DILUTE suspension and DILUTE emulsion
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10
Q

Non Newtonian fluid types and meaning

A

Do not follow Newtonian flow

1) plastic
2) pseudoplastic
3) dilatant

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11
Q

Bingham flow and associated particle

A

Plastic flow

 The material behaves as an elastic solid at low shear stress
 A certain shear stress equivalent to the yield value must be exerted before appreciable flow begins
 At shear stress above yield value, the material resembles a Newtonian system
 Materials exhibiting plastic flow are shear thinning.

Formula
U= (F-f) / G

U= plastic viscosity 
F= shear stress
f= yield value
G= shear rate 

Plastic flow is associated with the presence of flocculated particles in a concentrated suspension.

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12
Q

Pseudoplastic and associated particles

A

Pseudoplastic materials show shear-thinning properties

 The material will flow as soon as a shear stress is applied.
 Its viscosity decreases with increasing rate of shear.
 It is often noted that the flow curve tends towards linearity at higher shear stress
 The viscosity of a pseudoplastic material is best represented by the entire flow curve.

F^N = n’G

F= shear stress
N = index of pseudoplasticity (N>1)
n' = viscosity coefficient 
G= shear rate 

Log G = NlogF - log n’

 Pseudoplastic flow is associated with polymers in solution.

E.g. Aq dispersion of hyrdrocolloid such as tragacanth, alginates, methylcellulose and synthetic materials such as PVP (polyvinylpyrrolidone)

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13
Q

Dilatant material and associated particles

A

 Dilatant materials show shear-thickening properties
 The material will flow as soon as a shear stress is applied
 Its viscosity increases with increasing shear stress

Dilatant flow is associated with high concentration of deflocculated particles
Eg suspension with high concentration (>50%) of small deflocculated particles

Dilatant flow properties pose a problem in production.

F^N = n' G
N = <1
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14
Q

Explain shear thickening

A

Under zero shear the particles are closely pack and interparticulate voids are at a minimum, which the vehicle is sufficient to fill and at low Shear rate such as those created during pouring.

AS flow rate increases the particles become displaced from the uniform distribution and the clumps that are produced results in the creation of a larger void into which the vehicle drains, so that the resistance to flow is increase and viscosity rises.

The effect is progressive with increased shear rate until eventually the material may appear paste-like as flow ceases.

Removal of shear stress results in the reestablishment of the fluid nature

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15
Q

When a non Newtonian fluid is sheared, structural changes will occur in the system, resulting in changes in viscosity of the fluid.

The degree of change is dependent on

A

 When a non-Newtonian fluid is sheared, structural changes will occur in the system, resulting in changes in viscosity of the fluid.
 The degree of changes is dependent on :
1) Rate of shear
2) Duration of shear
3) Frequency of shear

 The structural changes may be reversible or irreversible

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16
Q

Why thixotropy occurs

A

When non Newtonian material is subjected to shear, structural changes occur and the viscosity changes.

Once the shear stress is removed, even if the breakdown of structure is reversible, it may not return to its original condition instantly (rheological ground state).

Thus When material subjected to increasing shear rate and then decreased to zero, the down curve will be displaced wrt the up curve and a hysteresis loop will be included.

The area of the loop may be used as an index of the degree of breakdown. (Extent of break down)

17
Q

Up curve and down curve

A

Up curve is obtain from flow curve by increasing shear rate or stress

Down curve is from decreasing rate or stress

18
Q

Characteristics of thixotropy

A

Shear thinning ( increase stress = viscosity decrease)

Slow recovery of the apparent viscosity on standing of the system. ( up and down curve is not superimposable)

19
Q

Why thixotropy occur at molecular level

A

 Thixotropic systems are usually composed of asymmetrical particles or macromolecules that are capsule interacting by numerous secondary bond.

At rest, they produce a loose three-dimensional structure, so that the material is gel-like when unsheared.

On shearing, they become aligned and flow as the energy imparted during shearing disrupts the secondary bond thus viscosity decreased (sol-gel transformation)

Upon removal of shear stress, the system starts to reform (not immediate)

The recovery time may be reduced by applying a gentle rolling or rocking motion which helps in the reformation of the network (rheopexy) as this increases the rate of collision of particles allowing bond formation.

 Thixotropy is a desirable property in pharmaceutical suspensions and emulsions

20
Q

Dynamic viscosity

Units

A

Dyne. cm^-2. S

SI = Pa.S

Alternative: poise (P)
Centipoise cP
1cP = 1 mPa. S

21
Q

Kinematic visosity unit

A

Cm^2. S^-1

SI: m^2. S^-1

Alternative: stoke (St)
Centistoke (cSt)
1cSt = 1mm^2. S^-1

22
Q

Absolute viscosity (applies to Newtonian fluid only)?

A

Dyne. Cm^-2. S

SI: Pa. S

Alternative: poise
Centipoise

23
Q

Apparent viscosity (non Newtonian fluid)

A

Dyne. Cm^-2. S

SI: Pa. S

Alternative: poise
Centipoise

24
Q

Determination of rheological properties and the equipment required

A

 Proper choice of instrumental method is essential for meaningful assessment of rheological properties of fluids

Newtonian fluids
 Shear rate is directly proportional with shear stress
 A single point determination using a certain shear rate or stress is theoretically adequate.
”one point” instruments that operate at a single shear rate can be used.

E.g. Capillary viscometers.

Non-Newtonian fluids
 Shear rate is not directly proportional with shear stress
 “Multiple point” instruments that operate at a variety of shear rates are required to obtain a
complete rheogram
E.g. rotational viscometers

25
Q

Types of capillaries viscometer

A

U tube viscometer

Suspended level viscometer

26
Q

Types of rotational viscometer

A

Concentric cylinder viscometer

Cone and plate viscometer

27
Q

Types of efflux viscometer

A

Redwood viscometer

Flow cups

28
Q

Capillary viscometer eqn

A

n1/n2 = t1p1/ t2p2

P = density 
T = time 
n = dynamic viscosity 

V = n / p

V = kinematic viscosity.

V1/v2= t1/t2

29
Q

Capillary bore size for Ostwald viscometer

And requirement

A

U tube

Size A-H
H = biggest therefore faster flow time.

The appropriate size should be selected such that a flow time of at least 300s for Size A and at least 200s for all the other sizes obtained.

30
Q

Ubbelohde viscometer

A

Suspended level
No need to fill viscometer with a precise volume.

9sizes (1, 1A, 2 , 2A, 3, 3A, 4, 4A, 5)
Increasing bore size.

The appropriate one should be selected such that a flow time of at least 300 s for size 1 and at least 200 s for all the other sizes is obtained

31
Q

Precautions for capillary viscometer

A

Precautions for capillary viscometers
 Ensure streamline flow by avoiding vibration and maintaining a minimum flow time
 Liquid should be free from air bubbles
 Ensure viscometer is clean before use
 Ensure viscometer is clamped vertically
 Ensure accurate temperature control
(Increase temp = viscosity drop)

32
Q

Concentric cylinder Viscometer

A

 The viscometer consists of 2 coaxial cylinders
 The inner cylinder, which is suspended freely by a torsion wire, is immersed in the test liquid contained in the outer cylinder
 Either the inner cylinder (Searle type) or outer cylinder (Couette type) is rotated

33
Q

Couette type principle

A

Couette Type
Rotation of “outer cylinder” produces movement of the test liquid and a torque is transmitted to the inner cylinder.
The resultant stress on the inner cylinder is indicated by angular deflection of the pointer which moves past a scale. This corresponds to the viscosity.

n = (kø) / w
Ø = angular deflection 
W= shear rate
34
Q

Problems of concentric cylinder viscometer

A

Problems of concentric cylinder viscometers
Shear rate of test liquid across the gap is
not constant.
End effects can be significant.
Frictional heating is significant at high shear rate.
Filling is difficult if gap is small.
Large volume of test liquid is required if
the gap is big.

35
Q

Cone and plate viscometer

A

Cone and plate viscometer
 This viscometer consists of a flat circular plate with a wide angle cone
placed centrally above.
 The tip of the cone just touches the plate and the test liquid is loaded into the included gap.

n= KG/ ♎️

G = torque = stress 
♎️ = radial velocity of the plate = rate
36
Q

Advantages of cone and plate viscometer

A

 In the cone and plate viscometer, the angle should be small to avoid edge effect

Main advantages of the cone and plate viscometer:
 Volume of test liquid needed is small (~100ul)
Filling and cleaning is easy
Shear rate is constant throughout the test liquid (because of the small volume )

37
Q

Efflux viscometer principle

A

EFFLUX VISCOMETERS
 The time taken for a given volume of liquid to flow through a small orifice is determined
 The efflux time is an arbitrary measurement of viscosity
 E.g. Redwood viscometer, Flow cups
 Redwood viscometer is used in BP to determine the viscosity of a standard solution of tragacanth relative to that of water