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rheology nw

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“παντα
ρει” (everything flows … )
- Heraclito de Samos (500 A.C.)
RHEOLOGY
Contents

RHEOLOGY:

a).
Definition and Fundamental concept.

b).
Properties contributing to rheological
behaviors.


c).
Graphic presentation of rheological data.
UNIT OBJECTIVES:







After the end of this lecture, student will be able
to:
Define rheology adequately.
Describe various deformations
Define viscosity and coefficient of viscosity
Define different term used in rheology
adequately.
Classify various types of fluid systems
Distinguish different system of flow and
deformation.
UNIT OBJECTIVES





Explain newtonian flow adequately.
List various examples of Newtonian fluids
Explain non-newtonian flow adequately
List various examples of non-Newtonian
fluids
Distinguish various reograms of newtonion &
non newtonion fluids.
RHEOLOGY
rheo – to flow
 logos – science
 ology – the study of

is the study of the flow of materials that behave in
an interesting or unusual manner.
 is the study of deformation and flow of matter.
 science concerned with the deformation of
matter under the influence of stresses.

EXAMPLES









MAYONNAISE,
PEANUT BUTTER,
CHOCOLATE,
BREAD DOUGH,
PAINTS,
INKS,
ROAD BUILDING MATERIALS,
COSMETICS,
DAIRY PRODUCTS, ETC.
SIGNIFICANCE OF RHEOLOGY
SIGNIFICANCE OF RHEOLOGY
 The
study of viscosity of true liquids,
solutions, dilute and concentrated colloidal
systems is of much importance in this study
 It
is involved in the mixing and flow of
materials, their packaging into containers,
the pouring from the bottle, extrusion
from a tube or a passage of the liquid to
a syringe needle.
SIGNIFICANCE OF RHEOLOGY

Can affect the patient’s acceptability of the
product,
physical
stability,
biologic
availability, absorption rate of drugs in the
gastrointestinal tract.

Influence
the
choice
of
processing
equipments in the pharmaceutical system
RHEOLOGY

Definition:

As the science concerned with the
deformation of matter under the influence
of
stress,
which
may
be
applied
perpendicularly to the surface of the body
(tensile stress) tangentially to the surface of
the body (a shearing stress) or at any other
angle to the surface of the body.
TYPES OF DEFORMATION:
 ELASTIC
DEFORMATION
 PLASTIC
DEFORMATION
TYPES OF DEFORMATION:
 ELASTIC
DEFORMATION:
it is the spontaneous and reversible
deformation. the work spent for the
deformation is recoverable when the body
returns to its original position after the
removal of the applied stress.
TYPES OF DEFORMATION:
PLASTIC DEFORMATION:
it is the permanent and irreversible
deformation. the work spent for the
deformation is dissipated as heat.
It is not recoverable mechanically after force
is removed.
PLASTIC DEFORMATION is also
referred to as flow and is exhibited by
viscous bodies.

TYPES OF FLUIDS:

NEWTONIAN FLUIDS:

NON NEWTONIAN FLUIDS
TYPES OF FLUIDS:
 NEWTONIAN
FLUIDS:
fluids that obey Newton's law are called
as Newtonian fluids
NON NEWTONIAN FLUIDS:
fluids that donot obey Newton's law are
called as Newtonian fluids
Time –independent
Time –dependent
NEWTONIAN
SYSTEMS
FLOW
CHARACTERISTICS OF NEWTONIAN FLUIDS
Newtonian (Newtonian Law of Flow)
 “the higher the viscosity of a liquid, the
greater is the force per unit area (shearing
stress) required to produce a certain rate
of shear”
WHAT IS SHEARING STRESS?
 Shear
– is a stress which is applied parallel or
tangential to a face of a material, as opposed
to a normal stress which is applied
perpendicularly.
 Shear
stress
Measured in (SI unit):
pascal
Commonly used symbols:
τ
Expressed in other quantities:τ = F / A
Newtonian (Newtonian Law of Flow)
Force
Area
Stress,  
F
A
L
h
Strain   
L
h
d
Shear Rate   
dt
Shear rate: Change in velocity/distance
measured in direction of flow at right angles
EXPLANATION OF TERMS USED:
SHEAR: is the movement of material relative to
parallel layer.
 SHEAR STRESS (F’): is the force per unite area
required to bring about flow (F/A)
 SHEAR RATE (S) difference in velocity dv,
between two planes of liquids separated by
distance dr (i.e. dv/dr)
F/A α dv/dr

STRAIN
 Strain
is the absolute amount of
distortion which occurs, expressed as a
fraction of an original dimension of the
unstressed
sample.
Strain
is
dimensionless.
VISCOSITY





DEFINITION:
As the measure of resistance of a fluid to deformation
under shear stress.
It describes the fluids internal resistance to flow .
It may be thought as a measure of fluid friction.
UNITS:
 Poise,centipoise
 Pascal,dynes/cm2
 Stokes, centistokes
VISCOSITY

Application of a shearing force to a fluid usually
causes it to flow because fluid cannot support a
strain for very long periods of time. When the force
is removed, irreversible deformation occurs.
VISCOSITY
The shear stress that causes a particular rate of
shear is obtained by dividing the shearing force by
the surface area to which the shearing force is
tangentially applied.
 The ratio of the applied shear stress to the rate
of shear is called coefficient of viscosity.



FLUIDITY: it is the reciprocal of viscosity
Ø = 1/ h
KINEMATIC VISCOSITY:
It is the absolute viscosity divided by the density of liquid
at a specified temperature
Kinematic viscosity = viscosity /density
The unite is Stoke (s) or centistoke(cs)
Thank you
Any questions ??


For reference:
PHYSICAL PHARMACY BY AGARWAL Pg:76-106
For further reference:
Cooper and Gunn’s Tutorial Pharmacy
Edited by S. J. Carter, 6th edition, 2005
(Pages: 115-127)

Remington, The science and practice of Pharmacy, 21st
edition, vol. 1, 2005
(Pages: 338-356)
Newtonian Fluid
Newtonian
behaviour:Viscosity remains constant no matter
what the shear rate.
From IDF 1982
Consistency curve for a
Newtonian fluid.
EXAMPLES OF NEWTONIAN FLUIDS





Water
Milk
Vegetable oils
Fruit juices
Sugar and salt solutions
FLOW CHARACTERISTICS OF NEWTONIAN FLUIDS
For a Newtonian fluid, the viscosity, by
definition,
depends
only
on
temperature and pressure (and also
the chemical composition of the fluid if
the fluid is not a pure substance), not
on the forces acting upon it.
NON-NEWTONIAN
SYSTEMS
NON - NEWTONIAN FLUIDS

Many pharmaceutical liquids like concentrated suspensions
and emulsions do not follow Newton’s equation because
the value of η varies with the rate of shear.

Therefore, it is usual to consider the apparent viscosities of
these systems at particular rate of shear, where the
apparent viscosity, ηapp, is the ratio of shear stress to shear
rate at a given point on the flow diagram.
NON - NEWTONIAN FLUIDS

In a non-Newtonian fluid, the relation between the
shear stress and the strain rate is nonlinear, and can
even be time-dependent. Therefore a constant
coefficient of viscosity cannot be defined.

A ratio between shear stress and rate of strain (or
shear-dependent viscosity) can be defined, this concept
being more useful for fluids without time-dependent
behavior.
NON - NEWTONIAN FLUIDS

Non-Newtonian Examples
 An
inexpensive, non-toxic example of
a non-Newtonian fluid is a suspension
of
starch
(e.g. cornflour)
in
water,(uncooked imitation custard,
being a suspension of primarily
cornflour, has the same properties).
NON - NEWTONIAN FLUIDS
 The
three types of Non Newtonian fluids
are plastic, pseudoplastic and dilatant, in
which the apparent viscosity varies with
the rate of shear.
NON NEWTONION
FLOW
NON NEWTONION
FLOW
(Time –independent)
SIMPLE
PLASTIC
FLOW
PSEUDOPLASTIC
FLOW
DILATANT FLOW
SIMPLE PLASTIC FLOW

When the graph is seen, the line does not pass
through the origin of graph but arises at some point
on the shear stress axis.

This indicates that a certain shearing stress must be
exerted before flow begins, which is called yield
value.
Contd..
The quantitative behavior of these systems is usually
expressed in terms of the Bingham equation :
 U or ηpl = F-fB
--------du/dx
Where fB is Bingham yield value.

RHEOGRAM
SIMPLE PLASTIC FLOW
The system behaving like a solid flows when such a
stress is applied to it, exhibiting elastic deformation
that are reversible when these small stresses are
removed.
 Materials showing plastic behavior are often termed
as Bingham bodies after the name of the scientist.

EXAMPLES OF PLASTIC FLOW

1. Bingham
plastics.
clay suspensions,
toothpaste,
Mayonnaise
The classic case is ketchup which will not
come out of the bottle until you stress it by
shaking
Semi solids
Thank you
Any questions ??


For reference:
PHYSICAL PHARMACY BY AGARWAL Pg:76-106
For further reference:
Cooper and Gunn’s Tutorial Pharmacy
Edited by S. J. Carter, 6th edition, 2005
(Pages: 115-127)

Remington, The science and practice of Pharmacy, 21st
edition, vol. 1, 2005
(Pages: 338-356)
PSEUDOPLASTIC FLOW
 It
can be seen from the graph that the curve
arises from the origin and no yield value exists,
hence the flow begins immediately on
application of a shearing stress.
 The slope of the curve gradually increases
until it reaches a maximum value.
PSEUDOPLASTIC FLOW

The decrease in apparent viscosity with
increasing rates of shear in plastic and
pseudoplastic systems results from the
breakdown of structures (i.e. aggregates of
dispersed particles) in the system under the
influence of shear,.
PSEUDOPLASTIC FLOW

Greater breakdown occurs at higher rates, although
beyond certain high shear rates no further
structural breakdown can occur and the apparent
viscosity then becomes constant.
Contd..
 When
the shear stress is reduced or
removed, reformation of the structures in
these systems occurs immediately and the
flow curve obtained from measurements at
decreasing shear rate is superimposable on
that obtained from measurements taken at
increasing shear rates.
Contd..

The occurrence of a yield value in plastic systems
indicates that stronger forces than those in
pseudoplastic systems must first be overcome
before flow can occur.

To distinguish between plastic and pseudoplastic
systems it is necessary to obtain measurements at
low shear rates.
Contd..
 Extrapolation of linear portions of flow curves
obtained at high rates of shear should not be carried
out to provide possible yield values since the system
may in fact be a pseudoplastic one.

Hence differentiation between these two behaviors
often depends upon the sensitivity of the method of
measurement at low shear rates.
PSEUDOPLASTIC FLOW






Also known as Shear-thinning non-Newtonian Liquid.
examples
tragacanth
Gelatin
Cmc
Mucilages & gum
RHEOGRAM
DILATANT FLOW
 It can be seen from the graph that the slope of
curve gradually decreases to a constant value, which
indicates that the apparent viscosity must increase
with increase in shear rate up to a maximum value.

Dilatancy is usually exhibited by concentrated
dispersions of deflocculated particles.
DILATANT FLOW

It is suggested that in these systems the
particles are arranged in a state of close
packing and the small amount of liquid present
is sufficient to fill the narrow spaces between
adjacent particles.
DILATANT FLOW
These thin liquid films allow the system to flow
like a liquid when the rate of shear is low.
 However at high shear rates, the particles will
become displaced from their close packed
arrangement which results in the formation of
larger void spaces in the system.

DILATANT FLOW

The liquid continuous medium is now
insufficient to fill all the spaces between
particles, hence the movement of the latter
relative to each other involves a greater
amount of friction and the apparent viscosity
therefore increases.
DILATANT FLOW

This effect may be troublesome in high speed
milling processes since the viscosity of dilatant
suspensions may increase so much that the
high rates of shear involved in the operation of
these mills that overloading of the motors may
occur.
SHEAR-THICKENING NON-NEWTONIAN
LIQUID
Shear-thickening: The
increase of viscosity with increasing rate
of shear in a steady shear flow.
Cream
is a shear-thickening fluid.
From IDF 1982
The consistency curve for a
Pseudoplastic fluid.
Thankyou
Any questions ??


For reference:
PHYSICAL PHARMACY BY AGARWAL Pg:76-106
For further reference:
Cooper and Gunn’s Tutorial Pharmacy
Edited by S. J. Carter, 6th edition, 2005
(Pages: 115-127)

Remington, The science and practice of Pharmacy, 21st
edition, vol. 1, 2005
(Pages: 338-356)
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