Processing and performance of nanophased braided carbon/epoxy composites

2010 ◽  
Vol 168 (1-3) ◽  
pp. 22-29 ◽  
Author(s):  
Mahesh V. Hosur ◽  
Md. Mazedul Islam ◽  
Shaik Jeelani
2016 ◽  
Vol 3 (4) ◽  
pp. 15-00607-15-00607 ◽  
Author(s):  
Keiichi SHIRASU ◽  
Akihiro NAKAMURA ◽  
Go YAMAMOTO ◽  
Toshio OGASAWARA ◽  
Yoshinobu SHIMAMURA ◽  
...  

Author(s):  
Wei Zhao ◽  
Chad S. Korach

The mechanical characteristics of the epoxy matrix found in filler reinforced polymer composites is important for determining strength and performance. Locally, property variations in regions surrounding fillers can influence the overall macroscopic composite response to loading. We investigate local nanomechanical stiffness of reinforced epoxy composites by using atomic force acoustic microscopy. The effects of tip shape on the contact mechanics at the epoxy interface are found to influence the reported results significantly and will be discussed in context of different tip models. The results have direct correlation to the effect of near-filler interphase regions and the long-term influence of environmental conditions on the polymer composites.


2007 ◽  
Vol 353-358 ◽  
pp. 2167-2170 ◽  
Author(s):  
N. Abacha ◽  
M. Kubouchi ◽  
K. Tsuda ◽  
T. Sakai

Epoxy-organoclay nanocomposite were prepared and investigated in terms of mechanical properties and also in term of water diffusion and sulfuric acid corrosion resistance. Diffusion was studied through epoxy samples containing up to 6phr of organically treated montmorillonite. The diffusion of the environmental solution was measured by immersion of the samples in these solutions at elevated temperature with noting the increase in weight as immersion function of time. An evaluation by flexural strength of the nanoclay/epoxy composites samples was made to compare their mechanical performances under corrosive environment as a function of immersion time and temperature.


2008 ◽  
Vol 29 (3) ◽  
pp. 293-301 ◽  
Author(s):  
Mrinal C. Saha ◽  
Sabrina Nilufar ◽  
Mosi Major ◽  
Shaik Jeelani

Author(s):  
H. M. Thieringer

It has repeatedly been show that with conventional electron microscopes very fine electron probes can be produced, therefore allowing various micro-techniques such as micro recording, X-ray microanalysis and convergent beam diffraction. In this paper the function and performance of an SIEMENS ELMISKOP 101 used as a scanning transmission microscope (STEM) is described. This mode of operation has some advantages over the conventional transmission microscopy (CTEM) especially for the observation of thick specimen, in spite of somewhat longer image recording times.Fig.1 shows schematically the ray path and the additional electronics of an ELMISKOP 101 working as a STEM. With a point-cathode, and using condensor I and the objective lens as a demagnifying system, an electron probe with a half-width ob about 25 Å and a typical current of 5.10-11 amp at 100 kV can be obtained in the back focal plane of the objective lens.


Author(s):  
Huang Min ◽  
P.S. Flora ◽  
C.J. Harland ◽  
J.A. Venables

A cylindrical mirror analyser (CMA) has been built with a parallel recording detection system. It is being used for angular resolved electron spectroscopy (ARES) within a SEM. The CMA has been optimised for imaging applications; the inner cylinder contains a magnetically focused and scanned, 30kV, SEM electron-optical column. The CMA has a large inner radius (50.8mm) and a large collection solid angle (Ω > 1sterad). An energy resolution (ΔE/E) of 1-2% has been achieved. The design and performance of the combination SEM/CMA instrument has been described previously and the CMA and detector system has been used for low voltage electron spectroscopy. Here we discuss the use of the CMA for ARES and present some preliminary results.The CMA has been designed for an axis-to-ring focus and uses an annular type detector. This detector consists of a channel-plate/YAG/mirror assembly which is optically coupled to either a photomultiplier for spectroscopy or a TV camera for parallel detection.


Author(s):  
Joe A. Mascorro ◽  
Gerald S. Kirby

Embedding media based upon an epoxy resin of choice and the acid anhydrides dodecenyl succinic anhydride (DDSA), nadic methyl anhydride (NMA), and catalyzed by the tertiary amine 2,4,6-Tri(dimethylaminomethyl) phenol (DMP-30) are widely used in biological electron microscopy. These media possess a viscosity character that can impair tissue infiltration, particularly if original Epon 812 is utilized as the base resin. Other resins that are considerably less viscous than Epon 812 now are available as replacements. Likewise, nonenyl succinic anhydride (NSA) and dimethylaminoethanol (DMAE) are more fluid than their counterparts DDSA and DMP- 30 commonly used in earlier formulations. This work utilizes novel epoxy and anhydride combinations in order to produce embedding media with desirable flow rate and viscosity parameters that, in turn, would allow the medium to optimally infiltrate tissues. Specifically, embeding media based on EmBed 812 or LX 112 with NSA (in place of DDSA) and DMAE (replacing DMP-30), with NMA remaining constant, are formulated and offered as alternatives for routine biological work.Individual epoxy resins (Table I) or complete embedding media (Tables II-III) were tested for flow rate and viscosity. The novel media were further examined for their ability to infilftrate tissues, polymerize, sectioning and staining character, as well as strength and stability to the electron beam and column vacuum. For physical comparisons, a volume (9 ml) of either resin or media was aspirated into a capillary viscocimeter oriented vertically. The material was then allowed to flow out freely under the influence of gravity and the flow time necessary for the volume to exit was recored (Col B,C; Tables). In addition, the volume flow rate (ml flowing/second; Col D, Tables) was measured. Viscosity (n) could then be determined by using the Hagen-Poiseville relation for laminar flow, n = c.p/Q, where c = a geometric constant from an instrument calibration with water, p = mass density, and Q = volume flow rate. Mass weight and density of the materials were determined as well (Col F,G; Tables). Infiltration schedules utilized were short (1/2 hr 1:1, 3 hrs full resin), intermediate (1/2 hr 1:1, 6 hrs full resin) , or long (1/2 hr 1:1, 6 hrs full resin) in total time. Polymerization schedules ranging from 15 hrs (overnight) through 24, 36, or 48 hrs were tested. Sections demonstrating gold interference colors were collected on unsupported 200- 300 mesh grids and stained sequentially with uranyl acetate and lead citrate.


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