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Scanning electron micrograph performance

In order to determine whether the new nanotubule electrode shows improved performance, a control electrode composed of the same material but prepared via a more conventional method is required. This control LiMn204 electrode was prepared by applying the precursor solutions described above directly onto a 1 cm Pt plate and thermally processing as before. Scanning electron micrographs showed that these films consisted of LiMn204 particles with diameters of —500 nm [124]. Spectrophotomet-ric assay showed that this control electrode also contained 0.75 mg of LiMn204 per cml A polypyrrole coat identical to that applied to the tubular electrode (0.065 mg) was also applied to this control electrode. [Pg.52]

Nitrogen sorption measurements were performed on a Quantachrome Autosorb 6B (Quantachrome Corporation, Boynton Beach, FL, USA). All samples were degassed at 423 K before measurement for at least 12 hours at 1 O 5 Pa. Mercury-porosimetrie has been measured on a Porosimeter 2000 (Carlo Erba Instruments) Scanning electron micrographs were recorded using a Zeiss DSM 962 (Zeiss, Oberkochen, Germany). The samples were deposited on a sample holder with an adhesive carbon foil and sputtered with gold. [Pg.2]

Fig. 2. In situ localisation of rabl6 mRNA in developing wheat seeds. A, Scanning electron micrograph of scutellar/starchy endosperm boundary. DC, depleted cells SE, scutellar epithelial cells. B, Dark field micrograph of in situ hybridised rabl6 sense RNA probe. No specific hybridisation is visible. C, Dark field micrograph of in situ hybridised rabl6 antisense RNA probe. Note specific hybridisation to depleted cells. Scanning electron microscopy was performed according to Mundy et al. (1986) in situ hybridisation after Raikhel et al. (1989). Fig. 2. In situ localisation of rabl6 mRNA in developing wheat seeds. A, Scanning electron micrograph of scutellar/starchy endosperm boundary. DC, depleted cells SE, scutellar epithelial cells. B, Dark field micrograph of in situ hybridised rabl6 sense RNA probe. No specific hybridisation is visible. C, Dark field micrograph of in situ hybridised rabl6 antisense RNA probe. Note specific hybridisation to depleted cells. Scanning electron microscopy was performed according to Mundy et al. (1986) in situ hybridisation after Raikhel et al. (1989).
FIGURE 18.2 Scanning electron micrographs of silicon microneedles, (a) Silicon microneedles micro-fabricated using a modified form of the BOSCH deep reactive ion etching process. The microfabrication process was accomplished at CCLRC Rutherford Appleton Laboratory (Chilton, Didcot, Oxon, UK). The wafer was prepared at the Cardiff School of Engineering, Cardiff University, UK. Bar = 100 pm (b-d) platinum-coated silicon microneedles prepared using a wet-etch microfabrication process performed at the Tyndall National Institute, Cork, Ireland. Bar = 1 mm (b), 100 pm (c,d). [Pg.341]

X-Ray Photoelectron Spectroscopy was performed using aPerkin-Elmer ESCALAB Model 551 spectrometer. Scanning Electron Micrographs were obtained on a Philips 501 Scanning Electron Microscope equipped with an EDX detector. [Pg.176]

Scanning electron micrographs were taken with an ISIDS-130 microscope. Thermogravimetric analysis (TGA) was performed with an SDT Q600 (TA Instruments). A Seiko DMS 210 dynamic-mechanical analyzer was used for DMA measurements. For water content determination samples were allowed to equilibrate over saturated salt solutions in sealed jars at controlled relative... [Pg.232]

Scanning electron micrographs (SEM) were obtained using a JSM 5500 LV (Jeol, Japan) electron microscope. The observations were performed in a secondary electron (SE) and in a backscattering electron (BSE) mode at a low vacuum pressure of 12 kPa. [Pg.132]

Figure 8. Scanning electron micrographs of the products of the template-free syntheses performed at 175 °C (A) and 200 °C (B). Figure 8. Scanning electron micrographs of the products of the template-free syntheses performed at 175 °C (A) and 200 °C (B).
Fig. 17. Scanning electron micrographs of lithium deposited on lithium foil in propylene carbonate containing 1.0 mol dm-3 (a) LiCKX, or (b) LiPF6 (deposition is performed after immersion for 24 h) (reproduced with permission from Electrochim. Acta, 40 (1995) 913 [64]). Fig. 17. Scanning electron micrographs of lithium deposited on lithium foil in propylene carbonate containing 1.0 mol dm-3 (a) LiCKX, or (b) LiPF6 (deposition is performed after immersion for 24 h) (reproduced with permission from Electrochim. Acta, 40 (1995) 913 [64]).
The pores are formed from bubbles during some of the typical manufacturing processes of polymer materials. The size distribution and density distribution of both are important to performance during the polishing process. Figure 6.17 shows two scanning electron micrographs of a polymer with such pore structures the first is the sidewall cross-section of the material, and the second is the top surface after some use. [Pg.125]

Figure 10. Scanning electron micrograph of an Izod impact test fracture surface of a PA 6/EPM-g-PA 6 90/10 binary blend. Izod impact test performed at 20 C. Figure 10. Scanning electron micrograph of an Izod impact test fracture surface of a PA 6/EPM-g-PA 6 90/10 binary blend. Izod impact test performed at 20 C.
Scanning electron microscopy was performed in order to investigate the dimensions and the morphology of polypyrrole nanoparticles. The scanning electron micrographs of polypyrrole nanoparticles are presented in fig 6. The SEM micrographs of polypyrrole exhibited globular, nanometer-sized particles. The polypyrrole nanoparticles are observed... [Pg.245]

The calculation of the diffraction pattern for a periodic system revolves around the construction of the reciprocal lattice and subsequent placement of the first Brillouin zone however, in this case the aperiodicity of the pentagonal array requires a different approach due to the lack of translational symmetry. The reciprocal lattice of such an array is densely filled with reciprocal lattice vectors, with the consequence that the wave vector of a transmitted/reflected light beam encounters many diffraction paths. The resultant replay fields can be accurately calculated by taking the FT of the holograms. To perform the 2D fast Fourier transform (FFT) of the quasi-crystalline nanotube array, a normal scanning electron micrograph was taken, as shown in Fig. 1.13. [Pg.18]


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