Determination of the light refraction: Difference between revisions

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Authors: [[Benutzer:Hschwarz|Hans-Jürgen Schwarz]], [[User:AHusen|Anika Husen]] <br> back to [[Polarization microscopy]]


== Abstract  ==
== [[Refraction of Light]]  ==
The refraction of a crystal is determined by the properties of its lattice and can be estimated by using  an immersion medium. For this purpose, the crystal is embedded in a substance with a known refractive index. By means of different examination methods, it is possible to determine whether the crystal has a greater or lesser refraction than the immersion medium. By comparison with several different known refractive indices, the estimation of the refractive index of the crystal can be effected. It should be noted, that [[Birefringence|birefringent]] crystals have different refractive indices at different orientations to the polarizers.
<br>'''Becke-line test'''
The Becke- line test is a method for determining, which of two materials has a greater light refraction. The Becke- line is a bright rim of light, visible along the grain boundary when the grain mount is slightly out of focus. The Becke- line moves into the higher refractive material, when lifting the lens tube/ lowering the specimen stage. If the values for refraction of two materials are the same, the Becke- line does not appear and the less they differ, the weaker it is pronounced.
[[Image:Becke-Linie 1.jpg|thumb|right|Figure 1: The Becke- line is almost not visible]]
[[Image:Becke-Linie 2.jpg|thumb|right|Figure 2: The Becke-Linie is clearly visible in the crystal]]
[[Image:Becke-Linie 3.jpg|thumb|right|Figure 3: Becke-line in the crystal]]
<br> <br>The explanation for the appearance of the Becke- line is, that the particle boundaries of crystals are rarely aligned parallel to the light ray. Because of the inclined boundary line, phenomena of refraction and reflection take place. Hereby the rays are focused and the intensity of the light is increased along the boundaries.
<br>'''Relief'''
Due to the differing light refraction of a crystal and its immersion medium, an optical relief is produced, wherein the respectively higher refractive material always appears higher in relief. The higher the difference in refractive index, the more pronounced the relief will appear. The effect is caused by the reflection of light along the boundary plane.
<br>'''Relief change'''
Birefringent crystals display two different refractive indices in every viewing direction. This can be ascertained, by rotating the crystal on the stage of the polarization microscope, to the oblique position. Because always two different indices are run through successively on rotating the crystal, the difference between the refractive index of the embedding medium and the crystal changes, causing a visible change in relief.
Summary of the most important points regarding the relief: 1. The development of the relief of a crystal  characterizes the difference of the refractive indices, between immersion medium on the one hand and the index or indices of the crystal on the other hand. 2. A pronounced change in the relief of the crystal, while turning the rotation stage (in polarized light), characterizes a difference in the two refractive indices in a birefringent crystal (i. e. birefringence).
<br>'''Chagrin'''
The term chagrin (french for grained leather) relates to the appearance of the surface of a light refracting crystal. The higher the difference between the refractive index of a crystal and the immersion medium, the more pronounced the surface structure appears.
<br>'''Schröder van der Kolk or oblique illumination method '''
[[Image:Kolk-shadow.jpg|thumb|left|Figure 4: Schröder van der Kolk - The shadow is clearly visible]]
" “The Schröder van der Kolk criterion” is another method for the comparative index determination of immersed particles. Other than the Becke- line test, which relies on a parallel and uninfluenced light conduction in the microscopes tube, the “Schroeder van der Kolk- shadow” is generated by manipulating the lighting.  A partially attenuated lighting penetrates the particle at an oblique angle of incidence. This effect can be obtained by inserting an obstacle between objective and ocular. These manipulations cause the formation of a shadow, clearly visible on one side of the particle and always visible, if there is a difference between the refractive indices of the particle and the medium. Decisive is, that if the refractive indices of particle and medium differ, the shadow only appears on one side of either particle or medium.
The following rule applies: If the particle has a higher refractive index than  the embedding medium, the shadow appears by the particle and on the side where the obstacle was introduced. The scientific explanation for this phenomenon (of partial shadow formation in cases of the explained manipulation of the lighting of the microscope) bases on the “rules of light refraction and total reflexion”. (citation needed)
== Wave plate/ Retarder==
A positive determination of interference colors can be ascertained by using a wave plate/ compensator. This device is made out of a material that has a specific birefringence. It can be added to the polarizer and analyzer, and fitted above the sample into the beam path. The wave plate is made in such a way, that, due to its birefringence, the interference colors can shift to exactly 550nm, i. e. the value of the deviation between magenta of the first and second order. This feature can be useful in determining the order of the interference color, because, by inserting the compensator, the interference color can be increased or lowered by one order, depending on the position of the crystal and wave plate to one another. Hereby the intensity of the color changes and both color orders can be matched by comparison.
Moreover, the direction of the greater refractive index can also be determined with the wave plate. In doing so, the crystal is rotated to the bright position and the compensator is inserted (must be at 45° to the horizontal line). If the interference colors increase, the higher refractive direction of the crystal is parallel to the higher refractive direction of the compensator.  If the interference colors are lowered, the higher refractive direction of the crystal is situated by the lower refractive direction of the compensator and vice versa. The directions of the higher and lower birefringence of the wave plate are usually drawn onto the compensator.
<br>
== Immersion method  ==
For the application of the immersion method, several different immersion media with a range of refractive indices have to be available. In the analysis of salts, immersion media must meet the following basic requirements: 
*For the salt analysis it is necessary to know and to guarantee the refractive index of a medium with an accuracy of 0.05.
*Therefore hygroscopic immersion media (like glycerine), or media mixtures with varying volatile components can only be used, if the refractive index can be checked with a refractometer.
*The immersion media should not dissolve the salt phases, or if they do, only very slightly. Therefore any medium with a water content is eliminated.
*The immersion media have to be transparent and non- toxic. They must not react with salts. 
*Provided that solvents are used as immersion media, they must not be too volatile (the evaporation rate should be &gt; 10, the vapor pressure &lt; 100 hPa)
<br>
{| width="100%" cellspacing="0" cellpadding="4" border="2" align="center"
|+ '''Data sheet of immersion liquids with reference to <bib id="Mainusch:2001" />'''
|-
| bgcolor="#ffff99" align ="center" | Refractiv index<br>n<sub>D</sub> bei 20°C
| bgcolor="#ffff99" align ="center" | Immersion medium (flüchtig)
| bgcolor="#ffff99" align ="center" | Immersion medium<br> (not volatile)
| bgcolor="#ffff99" | Bemerkungen
|-
| bgcolor="#ffff99" align ="center" | 1.32
| bgcolor="#ccffcc" align ="center" | methanol
| bgcolor="#ccffcc" align ="center" | &nbsp;
| bgcolor="#ccffcc" | Bezug: Merck, Okt. 2000<br>Dissolves certain salts.
|-
| bgcolor="#ffff99" align ="center" | 1.35
| bgcolor="#ccffcc" align ="center" | acetone
| bgcolor="#ccffcc" align ="center" | &nbsp;
| bgcolor="#ccffcc" | Source: Merck, Oct. 2000<br>Too volatile for the use in microscopy.
|-
| bgcolor="#ffff99" align ="center" | 1.36
| bgcolor="#ccffcc" align ="center" | ethanol (absolute)
| bgcolor="#ccffcc" align ="center" | &nbsp;
| bgcolor="#ccffcc" | Source: Roth 1999; The index was measured with the refractometer.<br>Dissolves some salts.
|-
| bgcolor="#ffff99" align ="center" | 1.38
| bgcolor="#ccffcc" align ="center" | propanol
| bgcolor="#ccffcc" align ="center" | &nbsp;
| bgcolor="#ccffcc" | Source: Roth, 1999; The index was measured with the refractometer.
|-
| bgcolor="#ffff99" align ="center" | 1.388
| bgcolor="#ccffcc" align ="center" | n-heptane
| bgcolor="#ccffcc" align ="center" | &nbsp;
| bgcolor="#ccffcc" | Source: Merck, Oct. 2000.
|-
| bgcolor="#ffff99" align ="center"  | 1.399
| bgcolor="#ccffcc" align ="center" | n-butanol
| bgcolor="#ccffcc" align ="center" | &nbsp;
| bgcolor="#ccffcc" | Bezug: Roth, 1999; The index was measured with the refractometer.
|-
| bgcolor="#ffff99" align ="center" | 1.41
| bgcolor="#ccffcc" align ="center" | n-amyl alcohol
| bgcolor="#ccffcc" align ="center" | &nbsp;
| bgcolor="#ccffcc" | Source: Merck, Oct.
2000.
|-
| bgcolor="#ffff99" align ="center" | 1.428
| bgcolor="#ccffcc" align ="center" | petroleum
| bgcolor="#ccffcc" align ="center" | &nbsp;
| bgcolor="#ccffcc" | Pharmacy product, the index was measured with the refractometer.
|-
| bgcolor="#ffff99" align ="center" | 1.446
| bgcolor="#ccffcc" align ="center" | chloroform
| bgcolor="#ccffcc" align ="center" | &nbsp;
| bgcolor="#ccffcc" | Source: Merck, Oct. 2000.
|-
| bgcolor="#ffff99" align ="center" | 1.45
| bgcolor="#ccffcc" align ="center" | kerosene
| bgcolor="#ccffcc" align ="center" | &nbsp;
| bgcolor="#ccffcc" | Pharmacy product, the index was measured with the refractometer.
|-
| bgcolor="#ffff99" align ="center" | 1.455
| bgcolor="#ccffcc" align ="center" | &nbsp;
| bgcolor="#ccffcc" align ="center" | glycerin
| bgcolor="#ccffcc" | Source: Roth, 1999; The index was measured with the refractometer.<br>Löst bestimmte Salze.
|-
| bgcolor="#ffff99" align ="center" | 1.46
| bgcolor="#ccffcc" align ="center" | &nbsp;
| bgcolor="#ccffcc" align ="center" | wallnut oil
| bgcolor="#ccffcc" | Pharmacy product, the index was measured with the refractometer.
|-
| bgcolor="#ffff99" align ="center" | 1.465
| bgcolor="#ccffcc" align ="center" | &nbsp;
| bgcolor="#ccffcc" align ="center" | caster oil
| bgcolor="#ccffcc" | Pharmacy product,the index was measured with the refractometer.
|-
| bgcolor="#ffff99" align ="center" | 1.47
| bgcolor="#ccffcc" align ="center" | turpentine
| bgcolor="#ccffcc" align ="center" | &nbsp;
| bgcolor="#ccffcc" | Twice rectified, the index was measured with the refractometer.
|-
| bgcolor="#ffff99" align ="center" | 1.474
| bgcolor="#ccffcc" align ="center" | &nbsp;
| bgcolor="#ccffcc" align ="center" | glycerin (anhydrous)
| bgcolor="#ccffcc" | Bezug: Merck, Okt. 2000.
|-
| bgcolor="#ffff99" align ="center" | 1.491
| bgcolor="#ccffcc" align ="center" | toluene
| bgcolor="#ccffcc" align ="center" | &nbsp;
| bgcolor="#ccffcc" | Source: Merck, Okt. 2000.
|-
| bgcolor="#ffff99" align ="center" | 1.505
| bgcolor="#ccffcc" align ="center" | o-xylene
| bgcolor="#ccffcc" align ="center" | &nbsp;
| bgcolor="#ccffcc" | Source: Merck, Oct. 2000.
|-
| bgcolor="#ffff99" align ="center" | 1.513
| bgcolor="#ccffcc" align ="center" | iodoethane
| bgcolor="#ccffcc" align ="center" | <nowiki>-</nowiki>
| bgcolor="#ccffcc" | Source: Merck, Oct. 2000<br>Too volatile for the use in microscopy.
|-
| bgcolor="#ffff99" align ="center" | 1.516-1.518
| bgcolor="#ccffcc" align ="center" | <nowiki>-</nowiki>
| bgcolor="#ccffcc" align ="center" | standard Zeiss immersion oil
| bgcolor="#ccffcc" | <nowiki>-</nowiki>
|-
| bgcolor="#ffff99" align ="center" | 1.53
| bgcolor="#ccffcc" align ="center" | <nowiki>-</nowiki>
| bgcolor="#ccffcc" align ="center" | clove oil
| bgcolor="#ccffcc" | Pharmacy product,the index was measured with the refractometer.
|-
| bgcolor="#ffff99" align ="center" | 1.55
| bgcolor="#ccffcc" align ="center" | <nowiki>-</nowiki>
| bgcolor="#ccffcc" align ="center" | anise oil
| bgcolor="#ccffcc" | Pharmacy product,the index was measured with the refractometer.
|}
<br>
<br><br><br>
==Weblinks==
<references />
== Literature  ==
<biblist/>
[[Category:LichtMikroskopie]] [[Category:Husen,Anika]] [[Category:Bearbeitung]] [[Category:R-MSteiger]] [[Category:R-CBlaeuer]]

Revision as of 09:27, 2 April 2012

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