A standard FA lens images a part in perspective, so its magnification changes with object distance and its measured distortion reaches 1.0–2.4%. A telecentric lens keeps the chief rays parallel to the optical axis, holding distortion at 0.02–0.1% and magnification effectively constant no matter where the part sits. That single optical difference decides whether a machine vision station can measure dimensions or only detect presence.
Most lens comparisons stop at “telecentric is more accurate, and more expensive.” That is not enough to specify a system with. This article puts the two families side by side using published distortion and depth-of-field figures from current POMEAS datasheets, works through what those numbers mean in microns on a real field of view, and then shows where the extra cost of a telecentric lens stops being worth paying.
Choose a telecentric lens when the output of the station is a number — a dimension, a position, an angle — and that number drives an accept/reject decision. Choose a standard FA lens when the output is a judgement — present or absent, readable or not — and when the field of view is large relative to any lens barrel you could physically mount. Everything below is the reasoning behind that split.
Distortion is the property people quote, but it is only one of three. All three come from the same root cause: where the aperture stop sits relative to the lens groups.
| Property | Telecentric lens | Standard FA lens |
|---|---|---|
| Chief-ray direction | Parallel to the optical axis | Converging toward the aperture stop |
| Magnification vs. object distance | Constant — focus error does not become size error | Changes with object distance (perspective error) |
| Viewing angle across the field | Identical for every point — effectively orthographic | Oblique away from the optical axis |
| Distortion | 0.02–0.1% | 1.0–2.4% |
| Front barrel size | At least as large as the field of view | Compact, independent of field size |
The first three rows are geometry, not tolerances. No amount of polishing makes a standard FA lens hold magnification constant with object distance, because the perspective is designed into where the chief rays converge. Software can correct the result of that geometry, but it cannot recover the depth information the lens never recorded.
These are published values from current POMEAS datasheets, not industry rules of thumb. Note that FA lens distortion is normally specified at a stated image height, because it grows toward the edge of the field.
| Lens | Type | Magnification / focal length | Distortion (published) |
|---|---|---|---|
| LTCM2-110C | Telecentric (coaxial) | 2.0×, WD 110 mm | 0.03% (TV distortion) |
| LTCM02-110 | Telecentric | 0.2×, WD 110 mm | 0.02% (TV distortion) |
| PMS-10VP110C111T | Bi-telecentric | 1.00×, WD 110 mm | <0.1% (image side) |
| LFE-16120 | Standard FA | 16.33 mm, 2/3″ | −1.00% @ y = 5.5 mm |
| LFHHH-1220M | Standard FA | 12 mm, 4/3″ | −1.78% @ y = 8.0 mm (1″) / −2.4% @ y = 11.0 mm (4/3″) |
The minimum sensor format, working distance, depth of field and resolution figures for each lens above are listed on its product page. As always, confirm against the current selection manual before designing a station — published values are typical for the stated configuration.
Percentages hide the size of the problem. Take a 2/3″ sensor (8.8 × 6.6 mm) at unit magnification, so the field of view is 8.8 × 6.6 mm, and measure a feature 5 mm from the optical axis.
| Lens | Distortion at 5 mm image height | Position error on a 5 mm offset feature |
|---|---|---|
| Telecentric, 0.03% | 0.03% | 5 mm × 0.0003 = 1.5 µm |
| Telecentric, 0.1% | 0.10% | 5 mm × 0.0010 = 5 µm |
| FA lens, 1.0% | 1.0% | 5 mm × 0.0100 = 50 µm |
| FA lens, 2.4% | 2.4% | 5 mm × 0.0240 = 120 µm |
That is a 10–80× difference in a quantity that lands directly in your tolerance budget. If the part tolerance is ±20 µm, an uncorrected 1% FA lens consumes the entire allowance before sensor noise, illumination or mechanical repeatability are considered. This is why measurement-grade stations start with the optics rather than with a more elaborate calibration routine.
The second property is harder to see on a datasheet and easier to feel on a production line. A telecentric lens specifies telecentricity — how close the chief rays come to being truly parallel — typically as a maximum angle. The bi-telecentric PMS-10VP110C111T, for example, is specified at object-side telecentricity <0.1°.
| Object moves 0.5 mm in Z | Cause of size change | Edge-position error on a 4.4 mm-half-height field |
|---|---|---|
| Telecentric, telecentricity 0.1° | Residual ray angle only | 0.5 mm × tan(0.1°) ≈ 0.9 µm |
| Standard FA lens, WD 110 mm | Perspective: scale change ≈ ΔZ / WD ≈ 0.45% | 4.4 mm × 0.0045 ≈ 20 µm |
On a well-fixtured line the part does not move half a millimetre — but parts vary in thickness, fixtures wear, and conveyor systems repeat to tens of microns at best. With an FA lens every one of those millimetres of Z variation reappears as a size error; with a telecentric lens it is suppressed to roughly the ray-angle term. This is the property that removes the need to recalibrate per part.
Telecentric lenses are often described as having unusually deep depth of field. The datasheets are more specific, and the values differ a great deal with magnification.
| Lens | Magnification | Depth of field (published) | Object resolution |
|---|---|---|---|
| LTCM02-110 | 0.2× | 10 mm | 16.78 µm |
| PMS-10VP110C111T | 1.0× | 0.58 mm | 4.44 µm |
| LTCM2-110C | 2.0× | 0.27 mm (theoretical) | NA 0.0074, F/13.5 |
The pattern matters more than any single figure: at 0.2× the depth of field is measured in millimetres, at 2× it drops below a third of a millimetre. Depth of field trades against resolution and against numerical aperture — stopping down buys axial tolerance and costs the fine-detail response you bought the lens for. Estimate it against the real height variation of your parts, and remember that a telecentric lens does not have unlimited depth of field simply because magnification is stable.
To hold chief rays parallel across a field, the front group must be at least as large as the field itself. A 40 mm field of view implies a front element of roughly 40 mm; a 200 mm field implies optics most stations cannot mount or afford. Standard FA lenses carry no such constraint, which is why they remain the only practical choice for wide-field tasks such as pallet inspection, robot guidance and large-panel presence checks.
| Constraint | Telecentric lens | Standard FA lens |
|---|---|---|
| Front barrel | Scales with field of view | Compact, independent of field |
| Practical field of view | Tens of millimetres to low hundreds | Centimetres to metres |
| Working distance | Fixed design value (e.g. 110 mm ±3% on the PMS-10VP110C111T) | Adjustable, often 0.15 m to infinity |
| Mount | C-mount, designed for a maximum sensor format | C-mount, wide focal-length range |
Note the working distance row. A telecentric lens is designed around a specific working distance and its magnification is only guaranteed at that value; an FA lens focuses from 0.15 m to infinity on a 25 mm focal length, for instance. Flexible focusing is a real advantage — just not for measurement.
A telecentric lens costs several times a comparable-focal-length FA lens of similar resolution. The premium is not margin — it is glass and tolerance. The front group is larger than the field, the design needs additional precision groups to hold distortion and telecentricity near 0.1%, and every element must be aligned to a tighter angular budget.
The decision is therefore an economic one, and it usually comes down to three questions:
| Inspection task | Recommended optics | Why |
|---|---|---|
| Dimensional gauging with accept/reject output | Telecentric | Magnification and distortion must be independent of part position |
| Deep bores, threads, connector pins | Telecentric | Orthographic view keeps side walls out of the image |
| Defect sizing against a true size threshold | Telecentric | Size error from distortion would corrupt the threshold |
| Multiple part variants at one station | Telecentric | No recalibration between variants |
| Reflective or specular surfaces | Telecentric with coaxial illumination | Parallel lighting path returns from the surface to the sensor |
| Presence/absence, orientation, counting | Standard FA | Only detection is required; accuracy is irrelevant |
| OCR, barcode and 1D/2D code reading | Standard FA | Text recognition tolerates scale variation |
| Robot guidance, bin picking | Standard FA | Wide field and compact barrel dominate |
| Large panels, pallets, furniture-scale parts | Standard FA | Telecentric front group would be impractically large |
It is worth stating plainly, because over-specifying optics is as expensive as under-specifying them. A standard FA lens wins when the decision is qualitative rather than quantitative, when the field of view exceeds any mountable barrel, when working distance must stay adjustable, and when the required accuracy is looser than a properly calibrated FA lens can already hold. A well-calibrated FA lens with good illumination is perfectly adequate for a very large share of vision tasks — it is simply not a measuring instrument.
For dimensional measurement, yes — the geometry guarantees it, since distortion is one to two orders of magnitude lower and magnification does not drift with object distance. For detection tasks the accuracy is wasted and the cost is not recovered.
Software correction reduces distortion error across the field, and for moderate fields it can be good enough. It cannot correct perspective error caused by the part sitting at a different height, because that is a change in magnification, not a fixed geometric warp. If Z variation is part of the process, software is not a substitute.
Distortion is specified at a stated image height, and it grows toward the edge of the field. A lens quoted at −1.78% at y = 8.0 mm on a 1″ sensor is quoted at −2.4% at y = 11.0 mm on a 4/3″ sensor simply because the outer field is being used.
No. Magnification is stable with object distance, but sharpness is not. Published values range from about 10 mm at 0.2× to under 0.3 mm at 2×. Depth of field is a resolution trade-off, not a free benefit of telecentricity.
Check that the lens is designed for your sensor format or larger, that the mount matches (C-mount in most cases), and that the lens resolution matches your pixel pitch. A 2/3″ lens on a 1.1″ sensor will screw on but will not cover the sensor correctly.
For measurement, the telecentric lens family spans 0.2× to 2× in object-space and bi-telecentric designs, including the LTCM02-110 0.2× for wide fields and the PMS-10VP110C111T 1.0× bi-telecentric for 1.1″ sensors. For detection and general imaging, see the FA lens family.
To go deeper on the optics themselves, read what a telecentric lens is and how it works, then work through the step-by-step selection guide to convert a tolerance into a magnification, working distance and depth-of-field requirement.
Key takeaway: the choice is not between a good lens and a cheap lens. It is between an instrument that reports a stable number and an imager that reports a stable picture. Decide which one your station needs, and the distortion figures will tell you exactly what the difference is worth.
Further reading: the test methods behind this article are documented in POMEAS Technical Reference the measurement-relevant distortion metric and how to measure it (§§8.7) + #s41).
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