Difference between revisions of "Light microscopy"
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This article | [[Image:Optical microscope nikon alphaphot +.jpg|thumb|250px|A light microscope.]] | ||
This article examines '''light microscopy''', abbreviated '''LM'''. | |||
==Resolution== | ==Resolution== | ||
<math>R = 1.22 * {gamma \over {NA_{obj} + NA_{cond}}}</math>.<ref>{{cite web |url=http://www.life.umd.edu/CBMG/faculty/wolniak/wolniakmicro.html |title=Principles of Microscopy |author= |date= |work= |publisher= |accessdate=21 January 2011}}</ref> | <math>R = 1.22 * {\gamma \over {NA_{obj} + NA_{cond}}}</math>.<ref name=pom>{{cite web |url=http://www.life.umd.edu/CBMG/faculty/wolniak/wolniakmicro.html |title=Principles of Microscopy |author= |date= |work= |publisher= |accessdate=21 January 2011}}</ref> | ||
<br> | <br> | ||
Where: | Where: | ||
* | *<math>R</math> = resolving distance; smaller better. | ||
* | *<math>NA_{obj}</math> = numerical aperture of the objective; typically 0.25 - 1.4, >1.0 is oil immersion, it is usu. inscribed on the lens itself. | ||
*gamma = wave length of light. | *<math>NA_{cond}</math> = numerical aperture of the condenser. | ||
*<math>\gamma</math> = wave length of light. | |||
It follows from the above equation that, closure of the condenser diaphragm results in a loss of resolution, i.e. R is larger.<ref name=pom/><br> | |||
Stated differently:<ref>URL: [http://www.microbehunter.com/2008/12/18/the-condenser-aperture-diaphragm/ http://www.microbehunter.com/2008/12/18/the-condenser-aperture-diaphragm/]. Accessed on: 21 January 2011.</ref><ref name=grayfield_dof>URL: [http://www.grayfieldoptical.com/depth_of_fieldfocus.html http://www.grayfieldoptical.com/depth_of_fieldfocus.html]. Accessed on: 27 May 2011.</ref> | |||
* | *Opening the condenser --> increases resolution & brightness -- but -- decreases depth of field (DOF) & contrast. | ||
* | *Closing the condenser --> increases DOF & contrast -- but -- decreases resolution & brightness. | ||
===Numerical aperture=== | |||
NA = numerical aperture. | |||
General formula for NA:<ref>URL: [http://en.wikipedia.org/wiki/Numerical_aperture http://en.wikipedia.org/wiki/Numerical_aperture]. Accessed on: 21 January 2011.</ref><br> | |||
<math>NA = n*sin(theta)</math>. | |||
Where: | |||
*n = index of refraction, n = 1.0 for air. | |||
*theta = half-angle of the max. cone of light | |||
===NA and f-number=== | |||
N = f/D. | N = f/D. | ||
Where: | Where: | ||
*N = f-number. | *N = f-number, e.g. f 1.2, f 1.4, f 11. | ||
**Smaller N = larger opening. | |||
*f = focal length. | *f = focal length. | ||
*D = diameter of entrance pupil. | *D = diameter of entrance pupil. | ||
At infinity: | At infinity:<br> | ||
N = 1/(2*NA_i) | <math>N = 1/(2*NA_i)</math>.<br> | ||
f/D = 1/(2*NA_i) | <math>f/D = 1/(2*NA_i)</math>.<br> | ||
<math>2*NA_i = D/f</math>. | |||
====Numerical aperture==== | |||
If one substitutes the above into the equation at the top:<br> | |||
<math>R = 1.22 * {\gamma \over ( D/2*f )}</math>. | |||
Notes: | |||
*Larger 'D' is better. | |||
NA = | *Larger NA = better. | ||
==Lenses== | |||
*Most lens = 'achromats' -- only correct green. | |||
*'Apochromatic' lenses - correct all colours; very expensive. | |||
==Condenser== | |||
*Condenser -- large flattened lens beneath the specimen. | |||
**Iris diaphragm. | |||
***Condenser diaphragm --> incr. contrast for resolution ---- large dia. good resol. bad contrast? | |||
****Field aperature diaphragm --> optical illumination. | |||
==Depth of field== | |||
*Abbreviated ''DOF''. | |||
*DOF depends on the aperature (small is better). | |||
Relation to other parameters:<ref name=grayfield_dof>URL: [http://www.grayfieldoptical.com/depth_of_fieldfocus.html http://www.grayfieldoptical.com/depth_of_fieldfocus.html]. Accessed on: 27 May 2011.</ref> | |||
*Inverse relationship with resolution and brightness. | |||
*Related to contrast. | |||
*High magnification --> smaller depth of field. | |||
===Formula=== | |||
<math>DOF = { \lambda_o n \over NA^2}+{ n \over M \cdot NA } e | |||
</math>.<ref>URL: [http://www.microscopyu.com/articles/formulas/formulasfielddepth.html http://www.microscopyu.com/articles/formulas/formulasfielddepth.html]. Accessed on: 27 May 2011.</ref> | |||
Where: | Where: | ||
*n = index of | *<math>\lambda_o</math> = illuminating light wavelength. | ||
* | *n = refractive index of the medium, 1.0 for air. | ||
*NA = numerical aperature (objective). | |||
*M = magnification. | |||
*e = resolution. | |||
===Increasing the DOF=== | |||
*DOF can be increased by ''focus stacking''. | |||
Software: | |||
' | *[http://hugin.sourceforge.net/ Hugin (sourceforge.net)] - does ''focus stacking'' and ''stitching''. | ||
Image: | |||
* | *[http://commons.wikimedia.org/wiki/File:Focus_stacking_Tachinid_fly.jpg Example of focus stacking (WC)]. | ||
== | ==Köhler illumination== | ||
===Rationale=== | ===Rationale=== | ||
* | *Even light distribution (avoid [[vignetting]]). | ||
===Procedure=== | ===Procedure=== | ||
#Any specimen on stage. | #Any specimen on stage. | ||
#Focus. | #Focus. | ||
# | #Adjust field aperture (bottom) - to obscure periphery of field of view (FOV). | ||
#Raise or lower condenser until field | #Raise or lower condenser until field aperture diaphragm clearly focused. | ||
#+/-Center 'field | #+/-Center 'field aperture diaphragm - using condenser centering screws. | ||
==Resolution== | |||
*Usual light microscopes are limited to about 0.2 micrometres. | |||
**Coming is "Super-resolution microscopy" - using high speed CCDs (charge-coupled devices).<ref>URL: [http://www.biocompare.com/Articles/ApplicationNote/1668/Recent-Approaches-To-%E2%80%98Super-Resolution-Microscopy-Utilizing-Camera-Detection.html http://www.biocompare.com/Articles/ApplicationNote/1668/Recent-Approaches-To-%E2%80%98Super-Resolution-Microscopy-Utilizing-Camera-Detection.html]. Accessed on: 2 May 2011.</ref> | |||
==See also== | |||
*[[Basics]]. | |||
*[[Microphotography]]. | |||
*[[Electron microscopy]]. | |||
*[[Polarization of light]]. | |||
==References== | ==References== | ||
{{Reflist}} | {{Reflist}} | ||
==External links== | |||
*[http://www.microscopyu.com/tutorials/java/depthoffield/index.html Depth of field calculator (microscopyu.com)]. | |||
[[Category:Basics]] | [[Category:Basics]] |
Latest revision as of 20:38, 23 April 2016
This article examines light microscopy, abbreviated LM.
Resolution
.[1]
Where:
- = resolving distance; smaller better.
- = numerical aperture of the objective; typically 0.25 - 1.4, >1.0 is oil immersion, it is usu. inscribed on the lens itself.
- = numerical aperture of the condenser.
- = wave length of light.
It follows from the above equation that, closure of the condenser diaphragm results in a loss of resolution, i.e. R is larger.[1]
- Opening the condenser --> increases resolution & brightness -- but -- decreases depth of field (DOF) & contrast.
- Closing the condenser --> increases DOF & contrast -- but -- decreases resolution & brightness.
Numerical aperture
NA = numerical aperture.
General formula for NA:[4]
.
Where:
- n = index of refraction, n = 1.0 for air.
- theta = half-angle of the max. cone of light
NA and f-number
N = f/D.
Where:
- N = f-number, e.g. f 1.2, f 1.4, f 11.
- Smaller N = larger opening.
- f = focal length.
- D = diameter of entrance pupil.
At infinity:
.
.
.
Numerical aperture
If one substitutes the above into the equation at the top:
.
Notes:
- Larger 'D' is better.
- Larger NA = better.
Lenses
- Most lens = 'achromats' -- only correct green.
- 'Apochromatic' lenses - correct all colours; very expensive.
Condenser
- Condenser -- large flattened lens beneath the specimen.
- Iris diaphragm.
- Condenser diaphragm --> incr. contrast for resolution ---- large dia. good resol. bad contrast?
- Field aperature diaphragm --> optical illumination.
- Condenser diaphragm --> incr. contrast for resolution ---- large dia. good resol. bad contrast?
- Iris diaphragm.
Depth of field
- Abbreviated DOF.
- DOF depends on the aperature (small is better).
Relation to other parameters:[3]
- Inverse relationship with resolution and brightness.
- Related to contrast.
- High magnification --> smaller depth of field.
Formula
.[5]
Where:
- = illuminating light wavelength.
- n = refractive index of the medium, 1.0 for air.
- NA = numerical aperature (objective).
- M = magnification.
- e = resolution.
Increasing the DOF
- DOF can be increased by focus stacking.
Software:
- Hugin (sourceforge.net) - does focus stacking and stitching.
Image:
Köhler illumination
Rationale
- Even light distribution (avoid vignetting).
Procedure
- Any specimen on stage.
- Focus.
- Adjust field aperture (bottom) - to obscure periphery of field of view (FOV).
- Raise or lower condenser until field aperture diaphragm clearly focused.
- +/-Center 'field aperture diaphragm - using condenser centering screws.
Resolution
- Usual light microscopes are limited to about 0.2 micrometres.
- Coming is "Super-resolution microscopy" - using high speed CCDs (charge-coupled devices).[6]
See also
References
- ↑ 1.0 1.1 "Principles of Microscopy". http://www.life.umd.edu/CBMG/faculty/wolniak/wolniakmicro.html. Retrieved 21 January 2011.
- ↑ URL: http://www.microbehunter.com/2008/12/18/the-condenser-aperture-diaphragm/. Accessed on: 21 January 2011.
- ↑ 3.0 3.1 URL: http://www.grayfieldoptical.com/depth_of_fieldfocus.html. Accessed on: 27 May 2011.
- ↑ URL: http://en.wikipedia.org/wiki/Numerical_aperture. Accessed on: 21 January 2011.
- ↑ URL: http://www.microscopyu.com/articles/formulas/formulasfielddepth.html. Accessed on: 27 May 2011.
- ↑ URL: http://www.biocompare.com/Articles/ApplicationNote/1668/Recent-Approaches-To-%E2%80%98Super-Resolution-Microscopy-Utilizing-Camera-Detection.html. Accessed on: 2 May 2011.