Comparison of the submicron structure and conductivity properties of multiwalled carbon nanotube polycarbonate composites using various microscopic methods.

Slides:



Advertisements
Similar presentations
Scanning near-field optical microscopy (SNOM) for magneto-optics Paolo Vavassori INFM - National Research Center on nanoStructures and Biosystems at Surfaces.
Advertisements

SHINSHU UNIVERSITY Shinshu University Nano Fusion Technology Research Group Study on the poly(1-butene) fibrous membrane via electrospinning Daisuke Kimura.
Detection of Percolating Paths in PMMA/CB Segregated Network Composites Using EFM and C-AFM Jacob Waddell, Runqing Ou, Sidhartha Gupta, Charles A. Parker,
The Principle of Microscopy : SEM, TEM, AFM
Alloy Thin Films by Multi-Target Sputtering Karla L. Perez MSE/REU Final Presentation Adv. Prof. King and Prof. Dayananda August 5, 2004.
Nanoscale Tools Special microscopes are used to investigate atomic and molecular structures. The following pictures are just a few examples of the many.
VTSLM images taken again at (a) 4.5  (T=84.7K), (b) 3.85  (T=85.3K), (c) 22.3  (T=85.9K), and (d) 31.6  (T=86.5K) using F-H for current and A-C for.
Activities during UK-Japan Young Scientist Workshop Dr Riz Khan Room 31DJ02, x6062, Advanced Technology Institute University.
The World IS Quantized 1 nm = m 10 um = m 0.1 m Only certain energies are allowed:  E = hf = hc/, where  is a wavelength scale.
Basic Imaging Modes Contact mode AFM Lateral Force Microscopy ( LFM)
Drs. Wei Tian & Yanhui Chen Sep-Dec Microscopic technique Scanning Electron Microscope (SEM) Transmission Electron Microscope (TEM) Atomic Force.
November 14, 2005EEBE 512/ENEL Dr. KE Jones Lecture 22: Chapter 4: Surface Characterization in Biomaterials and Tissue Engineering Really just a.
NATSYCO. microscopy Optical microscopy Electron microscopy Scanning probe microscope.
Transmission Electron Microscopy
Microscopy.
Scanning Electron Microscopy
NanotechnologyNanoscience Modeling and Simulation Develop models of nanomaterials processing and predict bulk properties of materials that contain nanomaterials.
Methods and Tehniques in Surface Science
PREPARATION OF ZnO NANOWIRES BY ELECTROCHEMICAL DEPOSITION
Three-dimensional Silicon composite nanostructures, taken with a scanning electron microscope.
By: C.J. Williams and Cirstyn Michel. In the 1600’s the light microscope (LM) was invented. A light microscope passes visible light through the specimen.
In this study, it has been found that annealing at ambient air at 500 ˚C of DC sputtered Mo bilayer produce MoO x nanobelts. Evolution of MoO x nanobelts.
Resin + 3 wt.-% of type 8 Resin + 1 wt.-% of type 3 Resin + 3 wt.-% of type 9 Conclusions A detailed electrical characterization, made making use of sophisticated.
Increased surface area on nanoparticles
[1] The Chemical Society of Japan (Ed.): Ultrafine Particle Science and Application, JSSP, 28 (1985). [2] B. D. Plouffe et al. Journal of Magnetism and.
What has enabled Nanoscience? Advances in Computing Power New Generation of Scientific Instruments Scanning Probe Microscopes An incomplete list.... Very.
Holly Tourtillott University of Missouri
Nanonics General SPM The Nanonics SPM Advantage Standard Atomic Force Imaging at the Highest of Resolutions and Quality Coupled with the Unique.
CAREER: Nanoelectronic and Nanophotonic Characterization of Hybrid Hard and Soft Materials Mark C. Hersam, Northwestern University, DMR Figure.
Characterization of morphology and microstructure of different kinds of materials at NTNU Mater Sci EM Lab Yingda Yu, Tor Nilsen, Morten P. Raanes, Jarle.
TEM charcaterization Basic modes – Bright field microscopy – Dark field Microscopy –STEM – EDAX – EELS.
Chapter 4-15 Grain boundaries: are boundaries between crystals. are produced by the solidification process, for example. have a change in crystal orientation.
Reminders for this week Homework #4 Due Wednesday (5/20) Lithography Lab Due Thursday (5/21) Quiz #3 on Thursday (5/21) – In Classroom –Covers Lithography,
Scanning Probe Microscopy Colin Folta Matt Hense ME381R 11/30/04.
5 kV  = 0.5 nm Atomic resolution TEM image EBPG (Electron beam pattern generator) 100 kV  = 0.12 nm.
Azerbaijan National Academy of Sciences Institute of Radiation Problems New Challenges in the European Area: Young Scientist's1st International Baku Forum.
Engr College of Engineering Engineering Education Innovation Center Engr 1182 Nano Pre-Lab Demolding Rev: 20XXMMDD, InitialsPresentation Short.
NANO 230 Micro/Nano Characterization
Scanning Electron Microscopy
Characterization of Nanomaterials…
Lecture 6: Microscopy II PHYS 430/603 material Laszlo Takacs UMBC Department of Physics.
2. Materials Two compositions were investigated APS: within the immiscibility gap NoAPS: outside the immiscibility gap APS: 67SiO 2.11TiO 2.22BaO NoAPS:49SiO.
Conductive epitaxial ZnO layers by ALD Conductive epitaxial ZnO layers by ALD Zs. Baji, Z. Lábadi, Zs. E. Horváth, I. Bársony Research Centre for Natural.
Tools of a Biologist MICROSCOPY Two factors play an important role in microscopy: 1. Magnification compares real size of a specimen with the one viewed.
A confocal Raman microprobe analysis of partial discharge activity in gaseous voids N A Freebody 1*, A SVaughan 1, G C Montanari 2 and L Wang 2 1 University.
EEM. Nanotechnology and Nanoelectronics
Applications   Semiconductors   Electric & Magnetic Devices   Carbon Nanotubes   Oxide materials   Nanoparticles and Nanocrystals   Dielectrics.
Material Processing of Polystyrene Boron Nitride Nanocomposites Raed Ayoob Supervisor(s): Thomas Andritsch and Alun Vaughan 16 September 2015 Early Career.
SURFACE CHARACTERIZATION OF SOME BIOADHESIVES WITH POTENTIAL APPLICATIONS IN MEDICINE. AFM INVESTIGATIONS Introduction Development of resin-based adhesive.
Outline History(TEM) Background Components Specimen Preparation Imaging method Contrast formation Modifications STEM References.
2Institute of Ceramics and Glass-CSIC, Madrid, Spain
The core facility platform at the Biomedical Centre
M. Arjmand1, M. Mahmoodi2, G. A. Gelves1, S. Park2, U. Sundararaj1
Atomic Resolution Imaging
Scanning Probe Microscopy: Atomic Force Microscope
Dispersion of Carbon Nanotubes in Alumina using a Novel Mixing Technique and Spark Plasma Sintering of the Nanocomposites with Improved Fracture Toughness.
Scanning Electron Microscopy Laboratory
Characterization of CNT using Electrostatic Force Microscopy
TEM and SEM.
SEM In-situ Experiments for Breakdown Study
Introduction - characterization of materials.
Prepared by Dr Diane Aston, IOM3
MODULE B-3: SCANNING TUNNELING MICROSCOPY
Methods and Materials: Microscopic & Drug Distribution Studies
Scanning Probe Microscope
Wei Wang,1 Dong Xiao Niu,2 Xinju Yang1
Size dependent surface potential studies on Si and GeSi quantum dots
Nanocharacterization (III)
Types of Microscopy Type Probe Technique Best Resolution Penetration
Scanning Electron Microscopy (SEM)
Presentation transcript:

Comparison of the submicron structure and conductivity properties of multiwalled carbon nanotube polycarbonate composites using various microscopic methods Bernadeth Kiss-Pataki1, Zsolt Endre Horváth1, Jyri Tiusanen2 1Research Center for Natural Sciences, Research Institute of Technical Physics and Materials Science - MFA, Hungarian Academy of Sciences. 2Promolding BV MOTIVATION: The nanometer size of the fillers in nanocomposites renders more difficulty on their microscopic characterization. Characterization of the dispersion of CNT agglomerates is still considered as a demanding task. Differences in size distribution of the agglomerates under the optical diffraction limit can result in significant differences in bulk composite properties. In such cases the widely applied transmission optical microscopy (TOM) cannot provide proper structural information for satisfactory materials characterization. Moreover artefacts produced during TOM sample preparation are comparable in size with the real structural features. In case of CNT polymer composites the substantial conductivity difference between the filler and the matrix provides a way of application of the conductive tip atomic force microscopy (CT-AFM) method to the characterization CNT dispersion in polymer composites. The resolution of the CT-AFM is far better than the transmission optical microscopes resolution, whereas this difference in conductivity enables the obvious separation of conductive parts from insulating matrix. Considering the working principle of the method, the artefacts influencing the topography of the sample surfaces essentially are not involved in the obtained image. Moreover the resulted images could be processes for statistical analysis, so their automatisation seems easier, not as in case of TEM and SEM images. RESULTS: PC97CNT3; tm=300°C; iv=30 mm/s; VR=46.46 Ωcm PC97CNT3; tm=320°C; iv=42 mm/s; VR=23.27 Ωcm PC97CNT3; tm=280°C; iv=42 mm/s; VR=6171.03 Ωcm CONCLUSIONS: EXPERIMENTAL: The analyses were carried out with the aid of the transmission optical (TOM) and transmission electron microscopy (TEM). A Leica Ultracut S ultra microtome was used to attain the adequate thickness of samples. TEM analyses were made by a Philips CM 20 Microscope, and optical microscopy observation was completed using an Olympus BH2 transmission optical microscope with a Leica DFC 280 digital camera. Conductive atomic force microscopy (C-AFM) investigations were performed on previously flattened surface of samples, using a glass knife of a Leica Ultracut Ultramicrotome. The sample then was fixed to the sample holder by a carbon paste. A Multimode 8 AFM (Bruker) was operated using the same type 20 nm Pt-Ir AFM probe, in the C-AFM mode to capture the conductive AFM images, setting the following parameters under ambient conditions and room temperature: 100 pA current sensitivity and 100 mV DC sample bias voltage, in 10 μm scanning area, with 512x512 pixel resolutions. The so obtained images were binarized, and evaluated according to the transmission optical microscopic image processing method. The research leading to these results has received funding from the European Community's Seventh Framework Programme (FP7-PEOPLE-ITN-2008) under grant agreement number 238363. www.contacproject.eu Research Center for Natural Sciences, Research Institute for Technical Physics and Materials Science, Hungarian Academy of Sciences Address: H-1121 Budapest, Konkoly Thege Miklós Road Nr. 29-33 Telephone: +36-1-392-2680