Objectives
In order to view the specimen with different objectives, they are mounted in a objective-revolver. Most microscopes have a revolver that can hold between three and six objectives. The Leitz Orthoplan has a revolver with five objectives. By twisting the revolver it is possible to look at the specimen with another objective. The objectives are centred in the revolver in such a way that the same part of the specimen is viewed each time. In most objectives, the lenses are fixed in the lens. Only the front lens of the objective is visible and is therefore the most sensitive to damage and dirt. In particular, objectives that have a higher magnification
factor come close to very close to the specimen cover glass (e.g. a Leitz 63x Planapochromate has a working distance of 0.15mm[1]). To prevent damage to the front lens, these objectives have a spring-loaded mechanism that allows the front part to slide telescopically inwards when contact is actually made with the cover glass. Objectives can be divided into different categories due to their constructive way. So there are: Achromates, Apochromates, Fluorites, PlanAchromates and PlanFluorites[3]. Achromatic objectives have been corrected for two colors and do not give a sharp image all the way to the edge. These objectives are quite simple in construction and therefore relatively inexpensive. The planAchromatic has the same color correction, however, with an extra lens the entire field of view is sharp. This is particularly important for micro photography. The Apochromatic objective is corrected for three colors and has a high Numerical Aperture due to many lenses of high quality glass types which creates a high dissolving power. PlanApochromatic objectives are also corrected for planity and therefore very suitable for microphotography. Of course these objectives are expensive to very expensive. The Fluoriten and PlanFluoriten are regularly called half Apo's in the microscopy world. The quality is between the Achromates and Apochromates[3]. Click on the schematic image below for an enlargement.

As already described in Microscopes, the exposure, the objective, the brightness and the resolving power are the four most important criteria that determine the quality of the image. The resolving power of a microscope (the resolution) is defined as the smallest distance at which two points are just separated. The resolving power depends mainly on the objective, to a lesser extent on the condenser, while the eyepiece does not contribute much. Image quality is determined by the color reproduction, transparency, contrast and resolution of the objective, while specimen properties are also important. Good image information is obtained when magnification and resolution are balanced. When higher magnification is not accompanied by higher resolving power, this results in meaningless magnification. A very important specification of the objective lens is the numerical aperture (NA), which is mainly determined by the top angle of the cone of light that can be captured by a lens. In the formula used to calculate the NA, the half aperture angle of the light cone (µ) is multiplied by the refractive index (N) of the medium between lens and specimen[2]. Theoretically, the NA of a dry lens (a lens that does not use immersion oil) can never be higher than 1.0. Since the refractive index of air is 1, the aperture angle of the lens should be 180° and the front lens is then infinitely large. Practically, these lenses reach a maximum NA value of 0.95. With oil immersion lenses, however, a higher NA can be achieved. The refractive index of this oil is 1.515. The maximum achievable NA is now 1.4.

The left side of the image below shows what would happen to the light when a dry lens with a large aperture angle is brought close to a cover glass. Light beams - || and - ||| will not reach the lens. The high numerical aperture would be useless and therefore there is no high resolving power. Immersion oil is applied on the right side (red). An objective with a high numerical aperture (from 1.0) can only be used in combination with immersion oil. The light beams are now absorbed by the objective and now the higher resolution can be used almost completely. These objectives always bear the name Öl, Oel or Oil in their inscription.

The diagram below shows the difference between low and high aperture objectives.

Objectives; tube length, cover glass correction, indication and purchase
The Leitz Orthoplan is designed for objectives with a tube length of 170mm. In 1976 Leitz switched to the then new standard of 160mm (see memo in downloads). According to Leitz this new standard can also be used normally in the Orthoplan and on several types of Leitz microscopes. Practice has proven that the 160mm tube length is indeed fine to use. Even later a new standard was introduced: the infinite objectives. These can not be used on the Leitz Orthoplan.
The thread with which Leitz objectives are screwed into the revolver is quite standard.
Objectives with a tube length of 160 and 170mm all have DIN-RMS W0.8" x 1/36".
The infinite objectives have a thread size of M19 x 0.75mm.
However, most manufacturers use this size, some have different sizes[6].
Most Leitz objectives have a standardized optical correction for a cover glass thickness of 0.17mm. From a numerical aperture of 0.4 a wrong thickness of the cover glass is noticeable. In the fifties and sixties, lenses were also manufactured where the thickness of the cover glass could be adjusted on the objective by means of a rotating ring. The thickness could be set between 0.12 and 0.22mm. This was necessary because the different manufacturers did not produce a constant 0.17mm. Even now, a 0.17mm is not always guaranteed. This should be taken into account when purchasing[5].
On all objectives there are indications such as: magnification factor, tube length, type of lens etcetera.
The enumeration below gives an explanation for the most commonly used engravings[6].
- | Can be used without cover glass |
∞ | Infinite objective |
0.17 | Corrected for a cover glass thickness of 0.17mm |
0.. of 1.. | Numerical aperture (NA) |
160 of 170 | Tube length for which the objective has been calculated |
40 : 1 | Magnification factor for older objectives |
40 | Magnification factor for newer objectives |
40x | Infinite objective magnification factor |
A | Objective without chromatic magnification |
apo | Apochromate |
C | Objective with chromatic magnification |
D | Can only be used with cover glass |
DO | To be used with or without cover glass |
FL of FI | Fluotar objective (sometimes called halfapo) |
H | To be used with heat object table |
HD | Striking light objective objective for bright and dark fields |
HI | Homogenous immersion (Jena) |
Iris | Objective with built-in iris diaphragm (intended for dark field) |
Korr | Objective where a swivel ring can be used to set a correction for cover glass thickness (0.12 - 0.22mm) |
L of LD | Long distance. Objective with extremely long working distance. Used in inversion microscope where, for example, plankton in a petri dish can be examined. |
NPL of Npl | Nearly plan objective. Objective is plan to a field of vision of 18mm |
O of o. of D. | Can be used without cover glass |
Öl, Oel, Oil / G, GL, Glyz / W | To be used with immersion oil / glycerin / water |
P | Polarization objective. Lenses are tension-free mounted |
(P) | Lenses not optimally tension-free mounted. Limited use for polarization microscopy |
Ph, Phako | Fasecontrast-objectief |
PL | Fasecontrast-objectief Olympus |
PL | Full planity (Leitz) |
Pol, POL | Polarization objective, lenses are optimally tension-free mounted |
Pv | Phase contrast objective (Leitz) |
Q | Objective with lenses of Quarts glass |
WI | Water immersion objective of (Jena) |











Purchase of objectives,
When purchasing a microscope, a choice must also be made in the objectives to be purchased. The whole must be in balance. It is not useful to equip a very simple microscope with top objectives because there should also be a good condenser, illumination, eyepiece et cetera. The opposite is also true, equipping a topmicroscope with simple achromatic objectives is of course possible, but it is a pity because with the microscope much more could be seen. For the hobbyist a new microscope with objectives of a top brand is usually not feasible as the price quickly goes up to €20.000,-. However, the second hand market is a good alternative. Experience shows that for older microscopes from Leica, Leitz and Zeiss there are still plenty of good objectives available in Europe. The market for Olympus and Nikon microscopes is much smaller. When objectives are bought from a dealer, the objective can be judged on the spot, but has the big disadvantage that usually a hefty price has to be paid for it. Take your time for the evaluation. At e.g. ABRO in Zaandam (see also under links) the prospective buyer gets the chance to test the objective itself extensively. Preferably bring your own samples.
The images below show three advertisements of dealers.
At a German trader the NPL Fluotar costs 16x €189,- , in the Netherlands €250,- while the bid on ebay is only €49,64. This bid will certainly go up but usually remains around €100,-.
The very popular objectives such as the Leitz 63x Planapo Öl with a NA of 1.4 are also expensive on ebay (≈ €400,-) but cost new €3000,-.



References:
[1] Ernst Leitz Wetzlar GmbH, prospectus 'Objective', Bestelnummer: 913397, blz 2. (see downloads for brochure)
[2] Junqueira L.C. en Carneiro J. (2004, tiende druk), Functionele histologie, Maarssen. Uitgeverij Elsevier. Chapter 1,
'Waarnemingsmethoden' p 17.
[3] Prof. Dr. Peter Böck (1989, 17., neubearbeitete auflage), Romeis Mikroskopische Technik, München. Verleger Urban & Schwarzenberg.
Chapter 1, 'Das Mikroskop und seine optischen Nebenapparate' p 4 and 5.
[4] Klaus Henkel, (Ausgabe: 14 juni 2003), Die Mikrofibel. Chapter 2.3, 'Die abbildende Optik des Mikroskops'. (see downloads or
[5] Prof. Dr. Peter Böck (1989, 17., neubearbeitete auflage), Romeis Mikroskopische Technik, München. Verleger Urban & Schwarzenberg.
Chapter 1, 'Das Mikroskop und seine optischen Nebenapparate' p 19 en 20.
[6] Klaus Henkel, (Ausgabe: 14 juni 2003), Die Mikrofibel. Chapter 2.3, 'Die abbildende Optik des Mikroskops' p 46 and 48.
(see downloads or http://www.klaus-henkel.de/)