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Nondestructive testing of defects in adhesive joints

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2. Experimental Details<br />

Polypropylene was obta<strong>in</strong>ed from Reliance Industries Ltd, India (REPOL H200F, melt flow <strong>in</strong>dex<br />

<strong>of</strong> 20 g/10m<strong>in</strong>). MWNT were obta<strong>in</strong>ed from Nanocyl CA Belgium (NC 3100, L/D=100-1000,<br />

purity=95%) and DMSRDE, Kanpur also subsequently utilized for our study. Various<br />

compositions <strong>of</strong> PP/MWNT composites us<strong>in</strong>g two different types <strong>of</strong> MWNT were prepared by<br />

melt mix<strong>in</strong>g <strong>in</strong> a conical tw<strong>in</strong> screw extruder (Micro 5, DSM Research, Netherlands) at optimized<br />

melt mix<strong>in</strong>g condition <strong>of</strong> 260 0 C with a rotational speed <strong>of</strong> 200 rpm for 15 m<strong>in</strong> <strong>in</strong> which MWNT<br />

were varied from 0.5-3 wt%. Melt mixed PP/MWNT samples were dried at 80 0 C under vacuum<br />

over night. PP/MWNT composite were melt-spun us<strong>in</strong>g a small scale sp<strong>in</strong>n<strong>in</strong>g mach<strong>in</strong>e<br />

manufactured by the Bradford University Research Ltd. UK, us<strong>in</strong>g a s<strong>in</strong>gle hole sp<strong>in</strong>neret <strong>of</strong> 1<br />

mm diameter. The fiber sp<strong>in</strong>n<strong>in</strong>g was carried out at 200 0 C with ram speed <strong>of</strong> 1.4 mm/m<strong>in</strong>. The<br />

take up speed was kept at 20 m/m<strong>in</strong> for all compositions. The melt spun fibers were further drawn<br />

at draw ratio <strong>of</strong> 8. The mechanical properties <strong>of</strong> drawn fiber were tested on a Favimat fiber tester<br />

(Textechno) with guage length <strong>of</strong> 20 mm and at a rate <strong>of</strong> 20 mm/m<strong>in</strong> for 50 filaments. Raman<br />

spectroscopy was performed us<strong>in</strong>g Job<strong>in</strong> Yovon (HR 800 micro-Raman) <strong>in</strong> the scann<strong>in</strong>g range <strong>of</strong><br />

200–2000 cm -1 with <strong>in</strong>cident laser excitation wavelength <strong>of</strong> 514 nm. Scann<strong>in</strong>g electron<br />

microscopic (SEM) analysis was performed with Hitachi S3400, operated at 15 KV. Wide-angle<br />

X-ray diffraction (WAXD) studies were carried out on a Philips X-Pert Pro. The <strong>in</strong>cident X-rays<br />

(λ=1.54 Å) from the Cu-target were monochromatized us<strong>in</strong>g a Ni filter.<br />

3. Result and Discussion<br />

3.1 Comparative study <strong>of</strong> Nanocyl NC 3100 and DMSRDE MWNT<br />

TEM images <strong>of</strong> MWNT are shown <strong>in</strong> Figure (1a, 1b) shows a network <strong>of</strong> entangled MWNT.<br />

DMSRDE produced MWNT are found to be more straight, less coiled and less entangled as<br />

compared to NC 3100. Figure 1c shows the tangential Raman band for two types <strong>of</strong> MWNT.<br />

Raman peak at ~1347 cm −1 orig<strong>in</strong>ates from disordered graphitic structure (D-band) and<br />

peak at ~1590 cm −1 orig<strong>in</strong>ates from crystall<strong>in</strong>e ordered structure <strong>of</strong> the graphene sheet (Gband);<br />

the <strong>in</strong>tensity ratio, IG/ID provides a measure <strong>of</strong> crystall<strong>in</strong>e structure <strong>in</strong> a given MWNT.<br />

The ratio <strong>of</strong> <strong>in</strong>tensity <strong>of</strong> G-band and D-band (IG/ID) depict the order structure <strong>of</strong> MWNT. IG/ID<br />

value <strong>of</strong> DMSRDE MWNT (1.31) is found higher than NC 3100 MWNT (0.87) which manifests<br />

DMSRDE produced MWNT are more ordered as compared to NC 3100.<br />

3.2 Orientation studies <strong>of</strong> PP crystal and MWNT along fiber axis<br />

Figure 2a shows the Wide angle X-ray diffraction (WAXD) pattern for PP/MWNT composites<br />

conta<strong>in</strong><strong>in</strong>g 0.5 wt% MWNT. WAXD pattern <strong>of</strong> the composites show the typical α -form <strong>of</strong> PP<br />

crystals and exhibits complete absence <strong>of</strong> the β -crystal form [6, 7]. Quantification <strong>of</strong> average<br />

orientation <strong>of</strong> PP crystal plane has been carried out us<strong>in</strong>g WAXD by perform<strong>in</strong>g azimuthal scan<br />

along the specific (110) PP crystal plane (Representative Figure 2b). The detail procedure <strong>of</strong><br />

quantification <strong>of</strong> crystal plane orientation is given below.<br />

The crystall<strong>in</strong>e orientation <strong>of</strong> the fibers has been determ<strong>in</strong>ed quantitatively us<strong>in</strong>g Hermans<br />

orientation factor [8] as generalized to a set <strong>of</strong> three crystallographic axes by Ste<strong>in</strong> [9]. This is<br />

def<strong>in</strong>ed as<br />

2<br />

3 < cos φ > −1<br />

f =<br />

2<br />

(1)

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