Nanoporous Polymer Films from Immiscible Polymer Blends: Pore Size and Composition Dependence

Similar documents
Ion Beam Sputtering: Practical Applications to Electron Microscopy

Formation of Oriented Fibers Using Injection of PEO Solutions inside Electric Fields Defined by Two Parallel Suspended Electrodes

BIOACTIVE COATINGS ON 316L STAINLESS STEEL IMPLANTS

Composite Electromagnetic Wave Absorber Made of Permalloy or Sendust and Effect of Sendust Particle Size on Absorption Characteristics

vii TABLE OF CONTENTS CHAPTER TITLE PAGE DECLARATION DEDICATION ACKNOWLEDGEMENT ABSTRACT ABSTRAK

Study on Wet Etching of AAO Template

JOURNAL INTEGRATED CIRCUITS AND SYSTEMS, VOL 1, NO. 3, JULY

Applications and Benefits of Multi-Walled Carbon Nanotubes (MWCNT)

Applying NiTi Shape-Memory Thin Films to Thermomechanical Data Storage Technology

Ultra-High Density Phase-Change Storage and Memory

Improved Contact Formation for Large Area Solar Cells Using the Alternative Seed Layer (ASL) Process

APPLICATION OF X-RAY COMPUTED TOMOGRAPHY IN SILICON SOLAR CELLS

Supporting Information

Laser beam sintering of coatings and structures

DENSITY MEASURING SYSTEMS

Technology White Papers nr. 13 Paul Holister Cristina Román Vas Tim Harper

Physical & Chemical Properties. Properties

PERMEABILITY MEASUREMENT

Sn-Cu Intermetallic Grain Morphology Related to Sn Layer Thickness

Fluid Mechanics: Static s Kinematics Dynamics Fluid

Surface Area and Porosity

Supporting Online Material for

Development of New Inkjet Head Applying MEMS Technology and Thin Film Actuator

Molar Mass of Polyvinyl Alcohol by Viscosity

Usage of Carbon Nanotubes in Scanning Probe Microscopes as Probe. Keywords: Carbon Nanotube, Scanning Probe Microscope

Lecture 24 - Surface tension, viscous flow, thermodynamics

THE USE OF OZONATED HF SOLUTIONS FOR POLYSILICON STRIPPING

Testing and characterization of anti-reflection coatings on glass

OPTIMIZING OF THERMAL EVAPORATION PROCESS COMPARED TO MAGNETRON SPUTTERING FOR FABRICATION OF TITANIA QUANTUM DOTS

Molysulfide. Particle Size Analysis

1. INTRODUCTION ABSTRACT

Radiation Curable Components and Their use in Hard, Scratch Resistant Coating Applications

GLOBAL COLLEGE OF ENGINEERING &TECHNOLOGY: YSR DIST. Unit VII Fiber Optics Engineering Physics

CHAPTER 2 EXPERIMENTAL. g/mol, Sigma-Aldrich, Germany Magnesium acetate tetrahydrate (C 4 H 6 MgO. 4 4H 2 O), assay 99.0%,

PHYSISORPTION DETERMINATIONS

MANUFACTURE OF CONTROLLED DRUG DELIVERY DEVICE OF POLYCAPROLACTONE BY SELECTIVE LASER SINTERING ABSTRACT

EXPERIMENT 11 UV/VIS Spectroscopy and Spectrophotometry: Spectrophotometric Analysis of Potassium Permanganate Solutions.

Hydrogen Adsorption on Nanoporous Biocarbon

Raman spectroscopy Lecture

SEM Analysis of CO 2 Laser Treated Cotton Grey Fabric

Effect of PWB Plating on the Microstructure and Reliability of SnAgCu Solder Joints

The chemical interactions of the template molecule are primarily dependent on the choice of polymer

Mixing in the process industry: Chemicals Food Pharmaceuticals Paper Polymers Minerals Environmental. Chemical Industry:

SORPTION ISOTHERM STUDY ON TWO POLYAMIDE NANOFIBEROUS MEMBRANES. Yan WANG, Jakub WIENER, Guocheng ZHU

Activity Two. Getting to Know the Water Molecule

Coating Technology: Evaporation Vs Sputtering

Heterogeneous Catalysis and Catalytic Processes Prof. K. K. Pant Department of Chemical Engineering Indian Institute of Technology, Delhi

, Yong-Min Kwon 1 ) , Ho-Young Son 1 ) , Jeong-Tak Moon 2 ) Byung-Wook Jeong 2 ) , Kyung-In Kang 2 )

BET Surface Area Analysis of Nanoparticles

7. DYNAMIC LIGHT SCATTERING 7.1 First order temporal autocorrelation function.

EXPERIMENTAL METHODS IN COLLOIDS AND SURFACES

Refractive Index Measurement Principle

Spectroscopic Ellipsometry:

Nanoparticle Deposition on Packaging Materials by the Liquid Flame Spray

ENERGY CARRIERS AND CONVERSION SYSTEMS Vol. II - Liquid Hydrogen Storage - Takuji Hanada, Kunihiro Takahashi

Basic Equations, Boundary Conditions and Dimensionless Parameters

Introduction to VLSI Fabrication Technologies. Emanuele Baravelli

Characterization of surfaces by AFM topographical, mechanical and chemical properties

Scanning Electron Microscopy Services for Pharmaceutical Manufacturers

COMPLEXITY RISING: FROM HUMAN BEINGS TO HUMAN CIVILIZATION, A COMPLEXITY PROFILE. Y. Bar-Yam New England Complex Systems Institute, Cambridge, MA, USA

Engine Bearing Materials

MICROSTRUCTURAL AND MECHANICAL CHARACTERIZATION OF GRAY CAST IRON AND AlSi ALLOY AFTER LASER BEAM HARDENING

Fracture Analysis of Concrete Using Scanning Electron Microscopy

FABRICATION AND CHARACTERIZATION OF

<788> PARTICULATE MATTER IN INJECTIONS

Lapping and Polishing Basics

SOLID STATE CHEMISTRY - SURFACE ADSORPTION

Solution for Homework #1

Plastics and Polymer Business. Properties enhancement for Plastics

vap H = RT 1T 2 = kj mol kpa = 341 K

Thermodynamics of Mixing

Pulsed laser deposition of organic materials

Why? Intermolecular Forces. Intermolecular Forces. Chapter 12 IM Forces and Liquids. Covalent Bonding Forces for Comparison of Magnitude

Defects Introduction. Bonding + Structure + Defects. Properties


Oil absorption in mesoporous silica particles

Near-field scanning optical microscopy (SNOM)

Barrier Coatings: Conversion and Production Status

Analysis of Blind Microvias Forming Process in Multilayer Printed Circuit Boards

LIPE- Institut National des Sciences Appliquées Toulouse, France Contact:

Measuring Line Edge Roughness: Fluctuations in Uncertainty

Over the last 50 years, commercial silicon photovoltaics

HEAVY OIL FLOW MEASUREMENT CHALLENGES

SALES SPECIFICATION. SC7640 Auto/Manual High Resolution Sputter Coater

PSD, Polymeric Fibers and the Permeability of Refractory Castables

POROUS BURNER - A New Approach to Infrared

Strength of Concrete

Chemical Engineering - CHEN

Phase Characterization of TiO 2 Powder by XRD and TEM

THE INFLUENCE OF SHAPE AND SPATIAL DISTRIBUTION OF METAL PARTICLES ON THE THERMAL CONDUCTIVITY OF METAL-POLYMER COMPOSITES

First let us consider microscopes. Human eyes are sensitive to radiation having wavelengths between

Microlenses immersed in nematic liquid crystal with electrically. controllable focal length

Objectives. Experimentally determine the yield strength, tensile strength, and modules of elasticity and ductility of given materials.

TIE-31: Mechanical and thermal properties of optical glass

Nanotribology of Hard Thin Film Coatings: A Case Study Using the G200 Nanoindenter

Light metal corrosion protection with water-borne silane systems

SECTION 623 CONCRETE BONDING COMPOUND, EPOXY MORTAR AND EPOXY POLYMER CONCRETE OVERLAY SECTION CONCRETE BONDING COMPOUND.

Interfacial Reaction between Sn Ag Co Solder and Metals

... complement Information for Processing

Calculation of Liquefied Natural Gas (LNG) Burning Rates

Transcription:

Mater. Res. Soc. Symp. Proc. Vol. 856E 25 Materials Research Society BB1.13.1 Nanoporous Polymer Films from Immiscible Polymer Blends: Pore Size and Composition Dependence Tong Liu, Rahmi Ozisik, Richard W. Siegel Department of Materials Science and Engineering, and Rensselaer Nanotechnology Center, Rensselaer Polytechnic Institute, Troy, NY 1218. Abstract Nanoporous polymer films have been prepared using immiscible blends of polyetherimide (PEI) and poly(caprolactone diol) (PCLD). The films were prepared by spin-coating from a common solvent dichloromethane (DCM). To create the nanoporous films, PCLD was removed by immersing the films in acetone, which dissolves PCLD only. Field emission scanning electron microscopy was used to study the porous structure. The pore structure of the films was affected by many factors such as composition of the blend, molecular weight, and various processing parameters. The formation of nanometer size pores was mainly due to the fast phase separation process during spin-coating. The pore size and pore size distribution was found to depend on the blend composition. Introduction In recent years, nanoporous materials have been receiving considerable interest from industry because of their several specific characters such as high surface area, low dielectric constant, and low refractive index. Some of the most interesting applications for nanoporous materials are as nanoporous films, which can be used as a catalyst, absorbent, filler system, gas separation layer, or biological sensor. There are many ways to make nanoporous films such as by lithography or the sol-gel method. 1 One other possible approach is to create a 2-phase mixture and remove the minority phase through physical or chemical means. This is the approach taken in this study through the use of immiscible polymer blends. Although the preparation of the nanoporous structure is important, a more important issue is the control of the size, distribution and connectivity of the pores within the material. There are many factors that would influence these factors such as polymer blend composition, molecular weight of the blend components, thermal history, and processing conditions. In order to study the effects of these on the final pore structure, a careful characterization of the pores is necessary. Various characterization methods can be used for this purpose, such as mercury injection, gas sorption, permeation test, and optical methods (direct observation). 2-5 Most of these methods characterize the pore structure by determining various macroscopic properties, which are unique to the pore structure. 2 Pore structure models are then used to estimate average parameters. However, in the optical methods, pore structure can be directly observed and pore structure parameters can be obtained by image analysis. The disadvantage of these methods is that the statistics is limited due to the small amount of samples (observable pores). To obtain

BB1.13.2 global information from the randomly selected regions (which are at the length scales of micrometers or less), statistical methods can be used. 6 In our study, PEI and PCLD were used to prepare a nanoporous polymer film. The two polymers were dissolved in their common solvent (DCM) and phase separated during spin-coating. Then, the PCLD phase was extracted from the blend by a selective solvent (acetone), thereby creating the pores in the films. The pore structure was characterized by field emission scanning electron microscopy (FESEM). Statistical methods were used to analyze the pore size data based on SEM experiments, and pore structure parameters, such as median pore size and pore size distribution were obtained. This study is focused on characterizing the PCLD content in the blend and its effect on the pore structure. Experimental and Analysis Methods Materials PEI (Ultem 1) was obtained from General Electric Plastics, Inc. The number and weight average molecular weight of PEI is 12, and 3, g/mol, respectively. The density of PEI is 1.28 g/cm 3. PCLD was purchased from Aldrich Corporation. The number average molecular weight of PCLD is 53 g/mol and its density is 1.73 g/cm 3. Dichloromethane (DCM) was used as the common solvent to dissolve both PCLD and PEI to prepare a polymer blend solution for spin-coating. The boiling temperature of DCM is 4 C. Acetone was used as the selective solvent to remove the PCLD phase from the films and create the porous structure. Sample Preparation PEI and PCLD were dissolved and mixed in DCM at room temperature using a magnetic stirrer. After the blend solution was formed, films were obtained by adding drops of the solution onto a substrate and spin-coating (SCS P67 manufactured by Specialty Coating Systems, Inc.). Spin-coating was performed at room temperature and a coating speed of 5 rpm was used. The substrates used in the experiments were highly polished silicon. To create porous films, spun-cast films were immersed in acetone to dissolve and extract the PCLD phase. Characterization In our study, a JEOL JSM-633F field emission scanning electron microscope (FESEM) was used to study the porous structure of the spun-cast films. The films were first embedded into epoxy resin and a microtome was used to cut the samples. The sample surfaces were sputter-coated with gold in an argon atmosphere. Image analysis was used to quantitatively determine the pore size and pore size distribution. 7 Several SEM images (all at the same magnification) were analyzed to obtain enough data (~2-3 pores for each sample) to calculate the median pore size and pore size distribution based on statistical models. We used the probability plot correlation coefficient (PPCC) testing method to both obtain the distribution function and to estimate the distribution parameters.

BB1.13.3 Results and Discussions Nanoporous polymer films were created by immersing PCLD/PEI blend films in acetone, which dissolved the PCLD phase selectively. The approximate thickness of the films is 1.5 µm. Figure 1 shows the cross section of a film containing 7% PCLD (all compositions are based on weight). We observed closed-cell pores (meaning the pores are not connected) at the nanometer length scale. The pores we obtained are nearly spherical in shape. The elongation of some pores in the direction parallel to the film surfaces was due to the deformation during SEM sample preparation. The effective pore size is the average of the longest and shortest diameters of the elongated pores measured from the SEM pictures. Epoxy Resin Porous Film Pores Film Surfaces Fig. 1. SEM micrograph of cross-section of a porous PEI film made from a 7% PCLD/PEI blend. Pore size is one of the important parameters that describe the pore structure. In our method, the pores were created as a result of phase separation of the two immiscible polymers. The observed pores (and pore size) are directly related to the size of the dispersed domains formed by the minor phase (PCLD), and are controlled by the minor phase content in the polymer blend based on phase coarsening and droplet coalescence phenomena during phase separation process. 7 Therefore, we used varying PCLD loadings to study the effect of minor phase content on pore size. Pore size distributions were obtained directly by image analysis from SEM micrographs and are shown in Figure 2 for 5, 7, 1, and 12% PCLD content. We counted and classified pores according to their size and calculated the percent of pores. The pore sizes ranged between 5 and 3 nm. The distributions observed in Figure 2 indicate that there is a greater possibility of having small pores than large pores using this method. In addition, since the pores must always have a finite size (x > ), a lognormal (see Equation 1) distribution is assumed, 1 ( ) ( ) ln x m f x = exp (1) 2 xσ 2π 2σ where σ is the shape parameter, and m is both the scale parameter and the median of the data that is defined as follows: ln x i ) m = exp() µ and ) µ = i N (2)

BB1.13.4.35.3.25.2.15.1.5-5 5-7 7-9 Pore Size Distribution (5%) 9-11 11-13 13-15 15-17 17-19 19-21 (a) 21-23 23-25 25-27 27-29 29-31.25.2.15.1.5-5 Pore Size Distribution (7%) 7-9 11-13 15-17 19-21 23-25 (b) 27-29 31-33.2 Pore Size Distribution (1%).25 Pore Size Distribution (12%).16.2.12.8.4.15.1.5-5 7-9 11-13 15-17 19-21 23-25 27-29 31-33 The PPCC method was used to verify whether our data obeys the lognormal distribution function. In the PPCC method, the data can be plotted against an assumed theoretical distribution in a way that the points should follow a linear relationship. 8 The correlation coefficient associated with the straight line in the probability plot shows the quality of the fit. If the data follow the assumed distribution model, the correlation coefficient would be equal to one. In general, if the correlation coefficient is greater than.9, the distribution function is accepted to represent the data successfully. In addition, the shape and scale parameters of the probability density function can be estimated from the intercept and slope of the linear plot. 8 Figure 3 shows the pore size distributions of samples with varying PCLD contents and are described by the lognormal distribution function. The correlation coefficient and distribution parameters of the lognormal distribution that were obtained by the PPCC method are given in Table 1. The correlation coefficients for different samples were all close to one, showing that the pore size data can be represented by the lognormal distribution. Table 1. Correlation coefficient and distribution parameters obtained by the PPCC method. PCLD content 5% 7% 1% 12% Correlation coefficient.985.996.981.976 Median (m) 74.8 94. 99.1 13 Shape parameter (σ).489.487.47.583-5 7-9 11-13 15-17 19-21 23-25 (c) (d) Fig. 2. Pore size distribution of porous PEI made from PCLD/PEI blends with different PCLD loadings: (a) 5%, (b) 7%, (c) 1%, (d) 12%. 27-29 31-33

BB1.13.5 The median pore size increased with increasing PCLD content (see Figure 4). This is probably due to the increasing coalescence of the minor phase during the phase separation process. The number of minor phase droplets would increase with increasing amount of minor phase that would enhance the probability of aggregation. Thus, larger minor phase domains would form after phase separation and lead to the formation of larger pores after solvent extraction. Probability Density (1/nm).14.12.1.8.6.4.2 Pore Size Distribution 5% 7% 1% 12% 5 1 15 2 25 3 35 Pore Size (nm) Fig. 3. Pore size distributions of porous PEI based on the lognormal distribution model. Conclusions The present study describes a method to create nanoporous polymer films by using immiscible polymer blends and removing the minor phase through solvent extraction. Nanometersize pores were created due to the fast phase separation during the spincoating process. Scanning electron microscopy was used to observe the pore structures. The pores obtained were found to be closed cells. Image analysis was used to measure the sizes of the pores. Statistical methods were Pore Size (nm) used to analyze the data and to obtain the relative information of the pore population. Various samples were prepared with varying PCLD content. It was found that as the PCLD content increased, the pore size also increased. The pore size distribution can be described using a lognormal distribution model. The median pore size increased from 74.5 to 13 nm as the PCLD content was increased from 5 to 12% due to increasing coalescence of the PCLD-rich phase during phase separation process. Acknowledgements This work was supported by IBM and the Nanoscale Science and Engineering Initiative of the National Science Foundation under NSF award number DMR-117792. References 1. P. Holister, C. R. Vas, T. Harper, Nanoporous materials, Technology white paper No. 5, Cientifica Ltd., (23). 2. F. A. L. Dullien, Porous media, fluid transport and pore structure; Academic: New York, (1992). 3. K. Sakai, K. Ozawa, R. Mimura and H. Ohashi, Journal of Membrane Science 32, 3-17, (1987). 11 1 9 8 7 2 4 6 8 1 12 14 PCLD Content (%) Fig. 4. Median pore size as a function of the initial PCLD content in PEI/PCLD blends.

BB1.13.6 4. C. Salmas and G. Androutsopoulos, Journal of Colloid and Interface Science 239, 178-189, (21). 5. Z. Mogri, D. R. Paul, Journal of Membrane Science 175, 253-265, (2). 6. J. S. Rustagi, Introduction to statistical methods; Rowman & Allanheld, (1984). 7. C. Chandavasu, M. Xanthos, K. K. Sirkar, C. G. Gogos, Polymer 43, 781-795, (22). 8. NIST/SEMATECH e-handbook of statistical methods, http://www.itl.nist.gov/ div898/handbook, (24).