Coplanarity is the one lead-frame measurement that a standard lens gets wrong in a way that looks right. A conventional lens projects a lead tip that sits 0.05 mm higher than its neighbours to a slightly different image position — not because the lead is out of place, but because the magnification changed with object distance. Object-side telecentricity removes that term. What it does not remove is everything else, and this page is mostly about the part it does not remove.
The spec is usually stated as the maximum vertical distance between the lowest and the highest lead seating plane of a package, measured from a defined datum (typically the package body). It is a Z-axis quantity. A single 2D camera does not measure Z. What it measures is the projected position of each lead tip in a silhouette, and the Z information is inferred from that projection.
This is the reason the lens choice dominates the result. If the projection magnifies differently at different object distances, a lead that is perfectly seated but 0.05 mm further from the lens reads as laterally displaced. On a 0.5 mm pitch package that displacement can be a meaningful fraction of the tolerance.
In an object-side telecentric lens the aperture stop sits at the rear focal plane, so chief rays on the object side run parallel to the optical axis. The consequence is that magnification does not change as the object moves along Z within the depth of field. A lead tip 0.05 mm higher and a lead tip 0.05 mm lower project at the same magnification.
What telecentricity does not do: it does not make the depth of field larger, it does not improve resolution, and it does not turn a 2D image into a height map. Those three are the most common over-claims made for telecentric optics in coplanarity applications.
| Model | Magnification | Working distance | Resolution | Depth of field | Distortion | Telecentricity | Sensor | Mount |
|---|---|---|---|---|---|---|---|---|
| PMS-LTCM2-65-S | 2.0X | 65mm | 2.2μm | — | — | — | 1/2″ | C-mount |
| PMS-LTCM2-65C-S | 2.0X | 65mm | 2.2μm(adjustable) | 0.13mm(adjustable) | 0.05% | <0.016° | 1/2″ | C-mount |
| PMS-LTC2-40 | 2.0X | 40.4mm | 3μm | 0.2mm | 0.04% | — | 1/2″ | C-mount |
| PMS-LTC2-40C | 2.0X | 40.4mm | 3μm | — | — | — | 1/2″ | C-mount |
| PMS-LTCM2-110 | 2.0X | 110mm | 4.53μm | 0.27mm | 0.03% | — | 2/3″ | C-mount |
| PMS-LTCM2-110C | 2.0X | 110mm | 4.53μm | 0.27mm | 0.03% | — | 2/3″ | C-mount |
| PMS-LTCM15-110 | 1.5X | 110mm | 5.59μm | 0.44mm | 0.01% | <0.02° | 2/3″ | C-mount |
| PMS-LTCM15-110C | 1.5X | 110mm | 5.59μm | 0.44mm | 0.01% | <0.02° | 2/3″ | C-mount |
| PMS-LTCM12-110 | 1.2X | 110mm | 6.71μm | 0.67mm | 0.01% | <0.02° | 2/3″ | C-mount |
| PMS-LTCM12-110C | 1.2X | 110mm | 6.71μm | 0.67mm | 0.01% | <0.02° | 2/3″ | C-mount |
Magnification between 1.0X and 2.0X covers SOIC through small QFP lead rows on 2/3″ and 1″ sensors. Sorted here by optical resolution, finest first — resolution is what sets how repeatably a lead edge can be extracted, and therefore how tight a coplanarity tolerance the station can hold. Full FOV arithmetic is in the calculation page.
Coaxial or near-parallel backlight gives the high-contrast silhouette that makes edge extraction stable. It also collapses the part into a shadow, which is exactly where the measurement limits appear:
The instinct is to magnify until a single lead fills the frame. That is wrong. Coplanarity is a relative measurement across all leads on a package, so every lead has to be in the same image, in focus, at the same magnification. The field of view is set by the lead row width plus margin, not by one lead.
Worked backward: a QFP with a 14 mm lead row on a 2/3″ sensor (11.0 mm horizontal) needs roughly 11.0 / (14 × 1.3) ≈ 0.6X to sit comfortably with margin. A smaller SOIC with a 6 mm row can take 1.0X or higher. The magnification follows from the part; the resolution you get is then sensor pixel size divided by magnification. Use the FOV and magnification calculation rather than estimating.
Three failure modes account for most coplanarity disputes between a vision system and a contact CMM:
None of these are solved by buying a better lens. They are solved by fixturing, and by deciding up front that the system reports a proxy that has been correlated to a reference method.
Fix the lighting first — a stable silhouette is worth more than an extra megapixel. Then set magnification from the lead row, then choose the sensor so that pixel size divided by magnification gives you the sub-pixel resolution the tolerance needs, and only then compare lens models. Reversing this order is the usual reason a coplanarity station gets rebuilt.
For the lighting decision specifically, the telecentric lighting guide covers backlight, coaxial and dark-field selection for measurement.
No. A single 2D telecentric view measures the projected position of lead tips. Coplanarity in millimetres is inferred from that projection. The inference is valid when the silhouette shows the actual seating surface — true for gull-wing leads, not for J-leads or BGA balls, where the measured feature is a proxy that must be correlated against a contact or confocal reference.
The three usual causes are part tilt putting one end of the lead row at the edge of the depth of field, lead-on-lead occlusion in the silhouette, and a datum that is fixtured rather than imaged. Telecentricity removes the magnification error but does not fix any of these. Check the fixture before questioning the optics.
No. Coplanarity is a relative measurement across the whole lead row, so every lead must be in one image at the same magnification. Field of view is set by the lead row width plus margin, which usually puts QFP-class packages near 0.5X to 1.0X and only small SOIC packages above 1.0X.
No. Telecentricity makes magnification insensitive to object distance; depth of field is governed by aperture and magnification as in any lens. A part tilted enough to leave the depth of field will still produce blurred edges, and blurred edges move the extracted measurement.
A high-contrast silhouette, which means backlight with a collimated or near-collimated source. Coaxial front light is useful for inspecting lead surface condition and marking, not for coplanarity, because it does not produce a clean silhouette edge of the lead foot.
It can image them, but the silhouette shows the outer bend rather than the seating foot, so the number it returns is a proxy. Treat it as a go/no-go correlated to a reference method, not as a direct coplanarity value, and validate the correlation on the actual package family.
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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