A microscope does not have a magnification. It has a chain of elements, each of which contributes a factor, and the figure that describes the image is the product of those factors.
This matters because a specification that quotes a single magnification without saying which chain produced it cannot be compared with another. Two systems both described as 1000X may differ by a factor of two in the detail they actually resolve, and both descriptions can be honest.
The objective contributes its own magnification, which is engraved on the barrel and refers to the image it forms at the specified tube lens focal length. The tube lens contributes a factor that is the ratio of its focal length to the reference focal length of the objective design. An adapter or camera mount can add a further factor.
Optical magnification is the product of the first two. Total system magnification, when a camera and a display are involved, multiplies again by the ratio of display size to sensor size.
Because these multiply, an error in any one of them scales the whole result. The adapter factor is the usual source of error, because adapters are often chosen mechanically and their optical effect is not considered.
A digital microscope's quoted magnification includes the display. The same instrument connected to a larger monitor has a larger quoted magnification while the image at the sensor is unchanged.
This is not a defect in the instrument; it is a different quantity. Screen magnification describes what an operator sees and is legitimate for visual inspection and training. It does not describe what the sensor samples, so it cannot be used to predict whether a feature will be resolvable.
The comparable figure across systems is object-space resolution: the smallest detail on the part that the system can distinguish, expressed in micrometres rather than as a multiple.
Object-space resolution combines the optical resolution of the objective with the sampling of the sensor, and it is the only figure that allows two systems of different architecture to be compared.
Across the POMEAS microscope units that publish it, object-space resolution spans 0.2 to 75 um. That span is wide because the units range from complete inspection assemblies to high-magnification optical units, and the figure is quoted at each unit's own configuration rather than at a common one.
When a requirement is written as a feature size in micrometres, the supplier can check it against this figure directly. When it is written as a magnification multiple, the supplier has to guess which chain was meant.
Higher magnification reduces both working distance and depth of field, because both follow from the same optical geometry. Working distance across the POMEAS microscope units spans 22 to 55 mm, which is modest in all cases because these units are complete assemblies with an illumination path in front of the part.
The practical consequence is that a high-magnification requirement also fixes the fixture. The part has to be presented within a narrow height band, and the illumination has to fit in the remaining space. A requirement written only in terms of magnification hides both constraints until the mechanical design begins.
A specification that can be met states four things together: the feature size to be resolved in micrometres, the field of view that must be covered in one image, the height variation of the part, and the space available in front of it.
From those four the configuration follows. The field and the sensor set the magnification; the feature size checks that the magnification is enough; the height variation sets the depth of field requirement; and the available space sets the working distance and therefore the objective family.
A specification that states only one of the four leaves the other three to be discovered during integration, and the discovery usually arrives as a rework.
Changing the camera changes the field of view at a fixed magnification, because the field is the sensor size divided by the magnification. A larger sensor covers a larger field and a smaller sensor covers a smaller one, with the same optics.
It also changes the sampling. A sensor with more pixels over the same area samples the image more finely, which can improve the effective resolution up to the optical limit and no further. Beyond that limit the extra pixels record a blur more precisely without revealing more detail.
Keeping the camera in the requirement rather than treating it as a later purchase is what prevents both surprises.
A claimed magnification can be checked with a stage micrometer: a scale of known pitch imaged at the claimed configuration. The distance between graduations in the image, divided by their known distance on the scale, gives the magnification directly.
The same measurement, repeated at the edges of the field, also reveals whether the magnification is uniform across the field. A system whose magnification varies across the field will not measure a dimension consistently regardless of the number engraved on the objective.
For the POMEAS microscope units the published distortion figure is 0.06 %, which is the geometric quantity that bounds that variation.
No. The digital figure usually includes the display, while the optical figure refers to the image at the eyepiece or sensor. The two can differ by a factor of several while both are honestly reported. Compare object-space resolution in micrometres instead.
Multiply the objective magnification by the tube lens factor, which is the tube lens focal length divided by the objective's reference focal length, then by any adapter factor. For a screen figure, multiply again by the ratio of display size to sensor size.
No. Measurement accuracy follows from object-space resolution, distortion and telecentricity, not from the magnification multiple. A high magnification with a short working distance and a small depth of field can measure worse than a moderate magnification on a stable fixture.
It is bounded by the objective's numerical aperture and by the sensor sampling. Across the POMEAS microscope units the published object-space resolution spans 0.2 to 75 um. A feature below that limit will not be resolved by increasing magnification further.
Both follow from the same optical geometry: an objective that forms a larger image must sit closer to the part for a given design. Across the POMEAS microscope units working distance spans 22 to 55 mm, and these units are complete assemblies in which the illumination path also occupies that space.
Changing the camera changes the field of view, because the field is the sensor size divided by the magnification, and it changes the sampling. It does not change the optical magnification itself.
Image a stage micrometer of known pitch at the claimed configuration and divide the imaged spacing by the true spacing. Repeating the measurement at the field edges also shows whether the magnification is uniform across the field.
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