A microscope unit is the least discussed part of an industrial microscope and the one that constrains the most. It sits between the objective and the camera, and it fixes three things: the largest sensor the system can use, the mechanical mount, and — least obviously — a focal length that scales the magnification of every objective fitted to it.
Getting the third one wrong is a common and quiet error: the system produces images at a magnification different from the number engraved on the objective, and nobody notices until a measurement is compared against a calibrated artefact.
All values below are published POMEAS figures for the MPT series and the POMEAS APO objective range. This is a selection method, not a compatibility claim, and no third-party specification is quoted.
In a finite optical system, the objective forms the image directly at a fixed distance, and anything inserted into the path — a beamsplitter, a filter, a coaxial illuminator — changes the optical path length and therefore the focus and magnification.
In an infinity-corrected system, the objective emits a collimated beam. The image is formed afterwards by a second lens — the tube lens, which is what the microscope unit contains. Because the beam between objective and tube lens is parallel, components can be inserted into that space without changing magnification or working distance.
That is why coaxial illumination is buildable into an infinity unit, and why the MPT-AF, MPT-BF and MPT-N all carry it. On an industrial station this matters constantly: filters, polarisers and illumination modules come and go between jobs, and only the infinity architecture lets that happen without re-deriving the optical setup.
| Model | Max. sensor | Mount | Tube lens focal length | Mechanical length |
|---|---|---|---|---|
| MPT-N | 4/3" (dia 22 mm) | C-mount | 180 mm | 226 mm |
| MPT-AF | 2" (dia 32 mm) | F-mount | 200 mm | 207.5 mm |
| MPT-BF | Full frame (dia 40 mm) | F-mount | 200 mm | 246 mm |
All three are published with coaxial illumination, an objective aperture of dia 20 mm, and an operating range of −10 °C to +50 °C.
Read the table as three separate decisions. The sensor limit is a ceiling on the field of view. The mount is a mechanical constraint on the camera — and note that the two larger-sensor units need F-mount cameras, not C-mount. The mechanical length is what the fixture has to accommodate, and it varies by nearly 40 mm across the range.
An infinity objective is designed for a specific tube lens focal length. The system magnification is:
system magnification = objective magnification × (unit tube lens focal length ÷ objective's design tube lens focal length)
Most infinity objectives are designed for a 200 mm tube lens, so:
- On MPT-AF or MPT-BF (200 mm): factor = 200 / 200 = 1.0 — the objective delivers its engraved magnification. - On MPT-N (180 mm): factor = 180 / 200 = 0.9 — a 10X objective delivers 9X.
The objective's design tube lens focal length has to be read from the objective's own datasheet; 200 mm is the common standard, not a universal one. Where an objective is designed for 180 mm, the factors invert.
This is not a defect — it is how infinity optics work — but it has to be in the calculation, because every field of view and every pixel-equivalent figure downstream depends on it.
With the system magnification settled, the field follows from the image circle:
field diameter ≈ max. image circle diameter ÷ system magnification
Worked examples using the published sensor limits:
- MPT-AF + 10X objective (factor 1.0 → 10X): 32 mm ÷ 10 ≈ 3.2 mm. - MPT-N + 5X objective (factor 0.9 → 4.5X): 22 mm ÷ 4.5 ≈ 4.9 mm. - MPT-BF + 2X objective (factor 1.0 → 2X): 40 mm ÷ 2 ≈ 20 mm.
Two things fall out of this. The larger-sensor units buy field of view at a given magnification, which is why MPT-BF exists for full-frame cameras. And the sensor limit is a ceiling, not a target — a camera smaller than the unit's limit simply uses less of the available field.
The unit carries the objective; the objective sets magnification, numerical aperture and working distance. Published POMEAS APO objectives:
| Objective | Magnification | NA |
|---|---|---|
| PMS-MPO2 | 2X | 0.055 |
| PMS-MPO5 | 5X | 0.14 |
| PMS-MPO10 | 10X | 0.28 |
| PMS-MPO20 | 20X | 0.42 |
| PMS-MPO50 | 50X | 0.55 |
| M Plan Apo L 20X (long working distance) | 20X | 0.34 |
NA rises with magnification, which is the expected trade: more magnification brings more resolving power and less working distance and depth of field. The long-working-distance variant (M Plan Apo L 20X, NA 0.34) trades a little NA for clearance — and MPT-AF is published as compatible with long-working-distance objectives, which is a reason to pick it where fixtures or tall samples demand clearance.
1. Camera first — its sensor size sets whether MPT-N, MPT-AF or MPT-BF is even usable, and its mount decides C versus F. 2. Field of view — from the sensor limit and the magnification, including the tube lens factor. 3. Objective — magnification, NA and working distance together; NA for resolution, working distance for the fixture. 4. Mechanical — unit length, objective aperture (dia 20 mm) and the space the coaxial illumination module needs.
It does not cover calibration: a correctly specified infinity system still has to be calibrated against an artefact before its measurements mean anything, and the tube lens factor is exactly the kind of systematic error that a pixel-scale calibration catches. It does not cover illumination choice beyond the built-in coaxial path. And it does not cover objectives from other makers — their design tube lens focal lengths have to be taken from their own datasheets, not assumed.
It holds the tube lens that forms the image from the objective's collimated beam, and it fixes the maximum sensor, the mount and the coaxial illumination path.
Because of the tube lens factor: system magnification = objective magnification × (unit focal length ÷ objective's design focal length). On MPT-N with a 200 mm-design objective the factor is 0.9.
MPT-N — 4/3" (dia 22 mm) maximum, C-mount, 180 mm tube lens, 226 mm length.
MPT-BF — full frame (dia 40 mm), F-mount, 200 mm tube lens, 246 mm length.
MPT-AF is published with an F-mount. Check the camera mount and any adapter before specifying.
Higher NA means more resolving power, and generally less working distance and depth of field. The long-working-distance 20X (NA 0.34) exists for cases where clearance matters more than the last increment of NA.
Send the camera model, sensor size, lens mount, required field of view and working distance, and POMEAS will return the microscope unit and objective with the calculated system magnification including the tube lens factor.
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