methods of polymeric membrane preparation by: ehsan saljoughi
TRANSCRIPT
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Characterization of
membranes
Dr. Ehsan Saljoughi Department of Chemical Engineering, Faculty of
Engineering, Ferdowsi University of Mashhad
Email: [email protected]
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Methods of polymeric membranes characterization Scanning electron microscopy (SEM)
Atomic force microscopy (AFM)
Bubble point method
Mercury intrusion method
Solute rejection measurements
Soaking method
Thermo gravimetric analysis (TGA)
Differential scanning calorimetry (DSC)
Methods of mechanical properties measurement
Surface analysis methods X-ray photoelectron spectroscopy
Fourier transform infrared (FTIR) spectroscopy
By: Dr. Ehsan Saljoughi
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Scanning electron microscopy (SEM)
is a very convenient and simple method for
characterizing and investigating the porous
structure and substructure of microfiltration and
other asymmetrical membranes, respectively.
A clear and concise picture of the membrane can
be obtained in terms of top layer, cross-section
and bottom layer. In addition, the porosity, pore
size distribution and geometry of the pores can be
estimated from the photographs.
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Scanning electron microscopy (SEM)
A narrow beam of electrons with kinetic energies
in the order of 1-25 kV hits the membrane sample.
The incident electrons are called primary (high-
energy) electrons, and those reflected are called
secondary (low-energy) electrons.
secondary (low-energy) electrons mainly
determine the imaging.
Burning of membrane can be avoid by coating the
sample with a conducing layer, often a thin gold
layer, to prevent charging up the surface.
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Scanning electron microscopy (SEM)
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Scanning electron microscopy (SEM)
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Scanning electron microscopy (SEM)
Thickness= 164 µm
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Scanning electron microscopy (SEM)
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Scanning electron microscopy (SEM)
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Scanning electron microscopy (SEM)
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FESEM and TEM
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Atomic force microscopy (AFM) Is a rather new method to characterize the surface
of a membrane.
Pore size, mean pore size, surface porosity and
roughness parameters can be obtained from the
AFM images.
A sharp tip with a diameter smaller than 100 °A is
scanning across a surface with a constant force.
London-vander waals interactions will occur
between the atoms in the tip and the surface of the
sample and these forces are detected. This will
result in line scan or profile of the surface.
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Atomic force microscopy (AFM)
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Atomic force microscopy (AFM)
0
0.005
0.01
0.015
0.02
0.025
0 50 100 150 200
Pore size, dp, (nm)
Pro
bab
ilit
y d
en
sit
y f
un
cti
on
Tw een-20 (0 w t.%)
Tw een-20 (2 w t.%)
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Atomic force microscopy (AFM)
The advantage of this technique is that no
pretreatment is required and the measurement
can be carried out under atmospheric conditions.
A disadvantage is that high surface roughness
may result in the images which are difficult to be
interpreted. Moreover, high forces may damage
the polymeric structure.
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Contact angle measurement
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Bubble-point method Provides a simple means of characterizing the maximum pore size in a
given membrane.
The top of the filter is placed in contact with a liquid (e.g. water) which fills all the pores when the membrane is wetted. The bottom of the filter in contact with air and as the air pressure is gradually increased bubbles of air penetrate through the membrane at a certain pressure.
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Bubble-point method The relationship between pressure and pore radius is
given by the Laplace equation:
If small pores are present, it is necessary to apply high
pressures or to replace the water with another liquid
e.g., by an alcohol. Because the surface tension at the t-
butanol/air interface is 20.7 mN/m whereas at the
water/air interface is 72.3.
Prp
2
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Mercury intrusion method
is a variation of the bubble-point method.
Pore size and pore size distribution can be
determined.
Mercury is forced into a dry membrane with the
volume of mercury being determined at each
pressure.
Again, the relationship pressure and pore size is
given by the Laplace equation. Because mercury
does not wet the membrane Laplace equation is
modified to:
cos2
Prp
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Mercury intrusion method
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Mercury intrusion method
θ is the contact angle of mercury with polymeric material (often 141.3 °).
Surface tension at the mercury/air interface is 0.48 N/m. Also as mentioned θ is 141.3°. Hence Laplace equation reduces to:
Where rp is expressed in nm and P in bar.
Since the volume of mercury can be determined very accurately, pore size distribution can be determined quite precisely.
Prp
7492
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Solute rejection measurements
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Solute rejection measurements
The fractional rejection Ri may be defined
according to below equation:
Roverall is given by:
)(
)(1
Feedi
permeatei
iC
CR
F
Poverall
C
CR 1
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Solute rejection measurements
Cut-off is defined as the molecular weight which is 90% rejected by the membrane.
Cut-off values of a membrane are often used in an absolute fashion (if membrane has a cut-off value of 40000, implying that all solutes with a molecular weight greater than 40000 are more than 90% rejected).
Common solutes are globular proteins such as albumin, branched polysaccharide such as dextran or a linear flexible molecule such as poly ethylene glycol.
Using gel permeation chromatography (GPC) or high performance liquid chromatography (HPLC), the molecular weight distribution of both the feed and permeate in a given test run can be determined.
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Solute rejection measurements Quantitative predictions of membrane
performance are difficult to be obtained by this method, because:
Cut-off values are often defined in different ways under different test conditions (pressure, cross-flow velocity, geometry of the test cell, concentration and type of solute, molecular weight distribution of solute) that makes it difficult to compare the results.
Other factors such as adsorption of solutes and concentration polarization influence the permeation rate and membrane selectivity.
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Porosity measurement by soaking
Membranes are soaked in distilled water or other
liquids and then weighed after mopping
superficial water with filter papers.
The wet membrane was placed in an air-
circulating oven before measuring the weight of
dry membrane.
From the two weights (wet and dry membranes),
the membrane porosity is calculated using the
following equation:
1000(%)
Ah
WWP
L
drywet
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Porosity measurement by soaking
Where P is the membrane porosity.
Q0 is the weight of wet membrane (g).
Q1 is the weight of dry membrane (g).
A is the membrane surface area (cm2).
h is the membrane thickness (mm).
ρL is liquid (water) density (gr/cm3).
In order to minimize the experimental errors, the
porosity of each membrane sample should be
measured three times and the results are
presented on average.
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Mechanical/Thermal Analysis
Mechanical properties measurement
Tensile test machine
Results are elongation and tensile strength
Thermal properties measurement
Thermo gravimetric analysis (TGA)
Differential scanning calorimetry (DSC)
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Thermogravimetric analysis (TGA)
A sample of membrane is dried to remove
moisture and then programmed from room
temperature to a certain high temperature at a
constant rate (°C/min) under the nitrogen
atmosphere.
During mentioned increase in temperature,
degradation of polymeric membrane occurs in
three steps.
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Thermogravimetric analysis (TGA)
The first step represents the volatilization of the volatile matter and/or the evaporation of residual absorbed water.
The second step represents the main thermal degradation of the polymeric chains.
The third step symbolizes the carbonization of the degraded products to ash.
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Thermo gravimetric analysis (TGA)
0
20
40
60
80
100
0 200 400 600 800
Wei
gh
t (%
)
Temperature ( C)
Polyethersulfone
Cellulose acetate
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Thermogravimetric analysis (TGA)
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Thermo gravimetric analysis (TGA)
Effect of heating rate: 1) 5 °C/min, 2) 10°C/min, 3) 16
°C/min, 4) 22 °C/min
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Differential scanning calorimetry (DSC) A sample of membrane is dried to remove moisture and then
programmed from room temperature to a certain temperature at a
constant rate (°C/min) under the nitrogen atmosphere.
Heat flow is plotted versus temperature.
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Dynamic Mechanical Thermal Analysis (DMTA)
Determination of Glass Transition Temperature (Tg)
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Surface analysis methods
are based on the concepts outlined schematically in below:
A solid surface is excited by means of radiation or particles bombardment and the emission products are detected.
Emission products, provide information about the presence of specific groups, atoms or bonds.
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Surface analysis methods
Important methods of surface analysis are: X-ray photoelectron spectroscopy (XPS)
Fourier transform infrared (FTIR) spectroscopy
transmission electron microscopy (TEM)
XPS is a surface sensitive technique and
measures the elemental composition (except H)
and chemical binding information for the top 1–5
nm depth of the surface region
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X-ray photoelectron spectroscopy (XPS)
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X-ray photoelectron spectroscopy (XPS)
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Fourier transform infrared (FTIR) spectroscopy
FTIR is able to provide significant qualitative detail about
the types of functional groups such as CO, OH, CN, …
FTIR offers much deeper depth of penetration (from
<200 nm to >1m)
By: Dr. Ehsan Saljoughi