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Self-Assembly of Synthetic and Biological Polymeric Systems of ...

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microscope, there are two polarized filters, the polarizer <strong>and</strong> the analyzer. The polarizer is<br />

situated below the specimen stage, <strong>and</strong> the analyzer is situated above the objectives <strong>and</strong> can<br />

be moved in <strong>and</strong> out <strong>of</strong> the light path as required. When both the analyzer <strong>and</strong> polarizer are in<br />

the optical path, in a crossed configuration, no light passes through the system <strong>and</strong> a dark field<br />

<strong>of</strong> view is present in the eyepieces.<br />

Figure 2.29. Polarized light optical microscope configuration.<br />

2.11.3.- Emission spectroscopy<br />

Inductively coupled plasma-atomic emission spectroscopy (ICP-AES) is a widespread technique<br />

for elemental analysis <strong>of</strong> a sample (56). In Figure 2.30, a scheme <strong>of</strong> an ICP-AES instrument is<br />

shown. A plasma source is used to make specific elements to emit light, after which a<br />

spectrometer separates this light in their characteristic wavelengths. This technique is<br />

especially suited for direct analysis <strong>of</strong> liquid samples. The sample solution is transformed into<br />

an aerosol by a nebuliser. Small droplets (1-10 μm) are transferred by an argon plasma. When<br />

the aerosol droplets enter the hot area <strong>of</strong> plasma, they are converted into salt particles. These<br />

salt particles are split into individual molecules that will subsequently fall apart to atoms <strong>and</strong><br />

ions. In the plasma, even more energy is transferred to the atoms <strong>and</strong> ions, promoting the<br />

excitation <strong>of</strong> their electrons. When these excited atoms <strong>and</strong> ions back to a lower excitation<br />

state or to their ground state they will emit electromagnetic radiation in the ultra-violet/visible<br />

range <strong>of</strong> the spectrum. The classical approach for ICP-AES measurement is to collect <strong>and</strong><br />

measure the emitted radiation radially, i.e. the optical axis is orthogonal to the central channel<br />

<strong>of</strong> the ICP. The limit <strong>of</strong> detection is in de order <strong>of</strong> ca. ng/ml.<br />

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