Electrode and tab measurement is a field-of-view problem before it is anything else. The features are small — a tab edge, a coating boundary, a few tenths of a millimetre of alignment error — but they sit on a web or a stack that is tens or hundreds of millimetres wide. That combination is what makes the magnification choice the whole design.
A 200 mm wide electrode on a 2/3″ sensor needs about 11 / 200 ≈ 0.055X. At that magnification a 3.45 μm pixel resolves roughly 63 μm per pixel, so a ±0.2 mm tab-position tolerance spans about six pixels. Workable, but a ±0.05 mm coating-alignment tolerance spans under two pixels, which is not.
The honest conclusion is that one station cannot hold both. Wide-web measurement and tight-tolerance measurement are different magnifications, and production lines that need both run two stations with different optics.
Below about 0.3X the telecentric lens becomes physically large and expensive, because the front element has to be at least as large as the field of view. This is the practical reason very wide electrodes are often measured with line-scan or multi-camera stitching instead of a single telecentric view.
The models below start at 0.061X, which covers roughly 180 mm on a 2/3″ sensor. Beyond that, consider whether the measurement can be decomposed — measure tab pitch locally at higher magnification and derive the web-level geometry from encoder or stage position.
| Model | Magnification | Working distance | Resolution | Depth of field | Distortion | Telecentricity | Sensor | Mount |
|---|---|---|---|---|---|---|---|---|
| PMS-LTCM03-110-C | 0.3X | 110mm | 11.18μm | 4.44mm | 0.01% | — | 2/3″ | C-mount |
| PMS-LTCM03-110 | 0.3X | 110mm | 11.18μm | 4.4mm | 0.01% | — | 2/3″ | C-mount |
| PMS-LTCM023-90 | 0.23X | 90mm | 13.98μm | 7.25mm | 0.02% | — | 2/3″ | C-mount |
| PMS-LTCM02-110 | 0.2X | 110mm | 16.78μm | 10mm | 0.02% | — | 2/3″ | C-mount |
| PMS-LTFM0206-468 | 0.206X | 468mm | 21.16μm | — | <0.01% | <0.02° | 35 mm | F-mount |
| PMS-LTCM016-189 | 0.16X | 189mm | 25.17μm | 18.75mm | 0.01% | <0.02° | 1″ | C-mount |
| PMS-LTDC01607-120(Y) | 0.16X / 0.7X | 120mm | 25.81μm / 7.63μm | 19.23mm / 1.30mm | 0.02% | <0.02° (0.1°) | 1″ | C-mount |
| PMS-LTDC00880176-120 | 0.088X / 0.176X (dual channel) | 120mm | 30.5μm / 30.5μm | 16mm / 7.2mm | <0.05% | — | 2/3″ | Dual C-mount |
| PMS-LTFM024-398 | 0.24X | 398mm | 30.76μm | — | 0.01% | — | 35mm | F-mount |
| PMS-LTCM0108-129-G | 0.108X | 129mm | 31.06μm | 34.29mm | 0.02% | — | 1″ | C-mount |
Magnification from 0.061X to 0.3X, ordered by resolution. These are the models that reach the field of view an electrode web or a stack edge requires. Note what the resolution column shows: at this magnification a given pixel size resolves tens of microns per pixel, which is the real limit on tight alignment tolerances.
Of these, coating boundary is the one that most often produces disputes, because the "edge" is defined by a contrast threshold that drifts with illumination and with the coating formulation.
On a moving web, motion blur destroys the edge before resolution does. The constraint is exposure time × web speed < sub-pixel distance, which at low magnification is a generous number and at high magnification is not. If the line cannot be stopped or strobed, the achievable resolution is set by the strobe, not by the lens.
Backlight for the silhouette edges (electrode and tab outer boundary), and a separate front or coaxial station for coating-boundary contrast. Trying to do both in one image forces a lighting compromise that degrades the more demanding measurement. The lighting guide covers the selection.
Usually not. A 200 mm electrode needs roughly 0.055X on a 2/3″ sensor, which resolves about 60 μm per pixel with a 3.45 μm pixel. A tolerance under about two pixels is not reliably measurable, so wide coverage and tight tolerance need separate stations.
The front element must be at least as large as the field of view, so a lens covering 180 mm has a front element of similar scale. This is why very wide webs are often measured with line-scan or multi-camera stitching instead.
As a contrast boundary between coated and uncoated foil rather than a geometric edge. Its extracted position depends on illumination consistency, so backlight silhouette methods that work for the foil edge do not transfer directly to the coating boundary.
No. Thickness is not a lateral measurement and does not appear in a silhouette. It needs a confocal, interferometric, or beta/X-ray gauge depending on the material and the required range.
Motion blur before optics. The requirement is exposure time × web speed below one sub-pixel distance. If the line cannot be stopped or strobed, the strobe capability sets the achievable resolution rather than the lens.
Less so, but web flutter and stack height variation are real on most lines. Object-side telecentricity removes the magnification term that flutter would otherwise introduce, which is usually worth having when the measurement is a width or a pitch.
Specification arithmetic gets you to a shortlist, not to a verdict. Send one part with the drawing and the tolerance you have to hold, and we will run it and report what the system returns — including the features that come back as unmeasurable. A written feasibility note is worth more than another datasheet.
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