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Influence of the Processes Parameters on the Properties of The ...

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Chapter 4.<br />

Experimental Procedures and Protocols for Analyses<br />

3 Protocols for Analysis<br />

3.1 Granulometry<br />

Experiments have been performed at <str<strong>on</strong>g>the</str<strong>on</strong>g> "Laboratoire de Génie Chimique de Toulouse"<br />

<strong>The</strong> s<str<strong>on</strong>g>of</str<strong>on</strong>g>tware proposed by Malvern with <str<strong>on</strong>g>the</str<strong>on</strong>g> granulometer Mastersizer 2000 uses <str<strong>on</strong>g>the</str<strong>on</strong>g> Mie<br />

<str<strong>on</strong>g>the</str<strong>on</strong>g>ory and permits to limit artefacts at small sizes <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> size distributi<strong>on</strong>s. Experimentally, <str<strong>on</strong>g>the</str<strong>on</strong>g> particles pass<br />

through <str<strong>on</strong>g>the</str<strong>on</strong>g> Scirocco composed <str<strong>on</strong>g>of</str<strong>on</strong>g> a vibrating hopper where particles are placed. A compressed air supply<br />

is out <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> hopper and creates depressi<strong>on</strong> causing <str<strong>on</strong>g>the</str<strong>on</strong>g> particles to <str<strong>on</strong>g>the</str<strong>on</strong>g> sensor. Vacuum allows <str<strong>on</strong>g>the</str<strong>on</strong>g> recovery<br />

<str<strong>on</strong>g>of</str<strong>on</strong>g> particles at <str<strong>on</strong>g>the</str<strong>on</strong>g> end <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> circuit. <strong>The</strong> particles diffract light at an angle. A lens Fourier can be reduced<br />

into a single optical diffracting each source. Image result <str<strong>on</strong>g>of</str<strong>on</strong>g> diffracti<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> a light beam is a set <str<strong>on</strong>g>of</str<strong>on</strong>g> c<strong>on</strong>centric<br />

rings. <strong>The</strong> value <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> deflecti<strong>on</strong> angle and <str<strong>on</strong>g>the</str<strong>on</strong>g> amount <str<strong>on</strong>g>of</str<strong>on</strong>g> light can be accessed respectively to particle size<br />

and quantity. <strong>The</strong> deflecti<strong>on</strong> angle <str<strong>on</strong>g>of</str<strong>on</strong>g> all smaller particles is large. <strong>The</strong> light diffracted by <str<strong>on</strong>g>the</str<strong>on</strong>g> sample is<br />

recorded which can be traced back to <str<strong>on</strong>g>the</str<strong>on</strong>g> size distributi<strong>on</strong>, and <str<strong>on</strong>g>the</str<strong>on</strong>g> percentage volume in each size class. <strong>The</strong><br />

size range available is between 0.05 and 2000 micr<strong>on</strong>s.<br />

Approximately a mass <str<strong>on</strong>g>of</str<strong>on</strong>g> 200 to 300 mg <str<strong>on</strong>g>of</str<strong>on</strong>g> powder material is placed inside <str<strong>on</strong>g>the</str<strong>on</strong>g> inlet pan. It tracks<br />

<str<strong>on</strong>g>the</str<strong>on</strong>g> evoluti<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> total grain size during milling. <strong>The</strong> parameters that affect <str<strong>on</strong>g>the</str<strong>on</strong>g> measure are <str<strong>on</strong>g>the</str<strong>on</strong>g> amplitude <str<strong>on</strong>g>of</str<strong>on</strong>g><br />

vibrati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> hopper that c<strong>on</strong>trols <str<strong>on</strong>g>the</str<strong>on</strong>g> flow <str<strong>on</strong>g>of</str<strong>on</strong>g> particles introduced into <str<strong>on</strong>g>the</str<strong>on</strong>g> measuring cell and <str<strong>on</strong>g>the</str<strong>on</strong>g> pressure<br />

<str<strong>on</strong>g>of</str<strong>on</strong>g> compressed air that plays <strong>on</strong> <str<strong>on</strong>g>the</str<strong>on</strong>g> velocity <str<strong>on</strong>g>of</str<strong>on</strong>g> passage <str<strong>on</strong>g>of</str<strong>on</strong>g> particles to <str<strong>on</strong>g>the</str<strong>on</strong>g> laser beam. After various trials for<br />

analysis, we found better reproducibility <str<strong>on</strong>g>of</str<strong>on</strong>g> measurements for 70% <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> maximum amplitude <str<strong>on</strong>g>of</str<strong>on</strong>g> vibrati<strong>on</strong><br />

<str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> hopper and a pressure <str<strong>on</strong>g>of</str<strong>on</strong>g> 2 bars. Its measure range in dry dispersi<strong>on</strong> is 0.1 to 2 000 micr<strong>on</strong>s. Typical<br />

measurement time is 5 sec<strong>on</strong>ds.<br />

<strong>The</strong> size distributi<strong>on</strong>s <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> polymer powders after pre-treatment (just sieving or grinding in <str<strong>on</strong>g>the</str<strong>on</strong>g><br />

knife mill and sieving) are presented in Figure 4.17. Most <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> particles <str<strong>on</strong>g>of</str<strong>on</strong>g> different materials used have<br />

mean diameter between 100 and 175m. <strong>The</strong> mean diameter (d 50 ) <str<strong>on</strong>g>of</str<strong>on</strong>g> a grinded polymer is 89.54 m.<br />

<strong>The</strong> median diameter (d 50 ) is a very important characteristic <str<strong>on</strong>g>of</str<strong>on</strong>g> this distributi<strong>on</strong> because it<br />

represents a cummulative frequency <str<strong>on</strong>g>of</str<strong>on</strong>g> 50%, which divides <str<strong>on</strong>g>the</str<strong>on</strong>g> size distributi<strong>on</strong> into two parts <str<strong>on</strong>g>of</str<strong>on</strong>g> equal area.<br />

This parameter permits to follow easily <str<strong>on</strong>g>the</str<strong>on</strong>g> evoluti<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> particle size during a treatment <str<strong>on</strong>g>of</str<strong>on</strong>g> a powder. As an<br />

illustrati<strong>on</strong>, Figure 4.18 presents <str<strong>on</strong>g>the</str<strong>on</strong>g> variati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> <str<strong>on</strong>g>the</str<strong>on</strong>g> median size <str<strong>on</strong>g>of</str<strong>on</strong>g> P L,D LA particles submitted to a grinding<br />

treatment in a tumbling ball mill.<br />

12<br />

10<br />

400<br />

Particle Diameter Variati<strong>on</strong> with Grinding time<br />

Volume (%)<br />

8<br />

6<br />

4<br />

2<br />

Poly (Lactide-co-glycolide) : Granulometry<br />

d 50 (m)<br />

300<br />

200<br />

100<br />

0<br />

0.01 0.1 1 10 100 1000 10000<br />

Particle Size(m)<br />

0<br />

0 1000 2000 3000 4000 5000<br />

Grinding Time (min)<br />

Figure 4.17: Size distributi<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> P L,D LA particle<br />

after 30 minutes <str<strong>on</strong>g>of</str<strong>on</strong>g> grinding.<br />

Figure 4.18: Variati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> particle diameter with<br />

grinding time for P L,D LA<br />

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