A 12× zoom ratio describes how far the magnification travels, not how well the lens holds up while travelling. Two zoom lenses with the same 12× ratio can differ by an order of magnitude in distortion at the telephoto end, and that difference only shows up when the lens is asked to measure rather than to look. Before substituting a zoom lens on a station that is already running, six parameters need to be read off the datasheet and checked against the existing setup: magnification range, zoom ratio definition, sensor coverage, working distance at both ends, distortion across the range, and numerical aperture.
POMEAS publishes measured values for all six on its zoom lens line. The figures quoted below are taken from the corresponding POMEAS product pages and are the values used for selection, not theoretical maxima.
Zoom ratio is the ratio between the longest and shortest focal length (or magnification) of the lens. A lens specified as 0.58×–7.5× has a ratio of 7.5 / 0.58 ≈ 12.9, which the industry rounds to "12.5×". A lens specified 0.7×–4.5× has a ratio of 4.5 / 0.7 ≈ 6.4, sold as "6.5×".
The ratio alone does not tell you where the range sits. A 6.5× lens covering 0.7×–4.5× and a 6.5× lens covering 0.55×–7.6× occupy different parts of the magnification scale and will not be interchangeable on the same fixture without rechecking field of view and working distance.
Magnification on a zoom lens is also not a fixed property of the lens alone: it is the product of the zoom body, the tube lens (镜管), the objective (物镜), and any adapter factor. On POMEAS zoom configurations the total magnification is calculated as:
Total magnification = zoom body × tube lens × objective × 0.55
The 0.55 factor comes from the standard adapter used in these assemblies. Any substitution that changes one of the four terms changes the total, even when the zoom body ratio is identical.
1. Magnification range, not just the ratio. Read the two end values. The station's required field of view has to sit inside the range with margin at both ends, because optical performance at the extreme ends of a zoom range is never as good as in the middle.
Field of view is derived from magnification and sensor size:
FOV (mm) = sensor width (mm) / magnification
On a 2/3-inch sensor (8.8 mm × 6.6 mm), a lens at 0.58× gives a horizontal field of 8.8 / 0.58 ≈ 15.2 mm; at 7.5× it gives 8.8 / 7.5 ≈ 1.17 mm. The same lens therefore spans roughly 15 mm down to just over 1 mm of horizontal coverage — that span is what the ratio is buying.
2. Sensor coverage. A zoom lens built for a 2/3-inch sensor will vignette on a 1-inch sensor. Dark corners at the wide end are the standard symptom. If the existing camera has a larger sensor than the substitute lens covers, the corners fall off and any measurement taken there becomes unreliable.
3. Working distance at both ends. On a parfocal zoom lens the working distance stays nominally constant across the range; on a non-parfocal design it shifts. For a station with fixed mechanical mounting, a working distance that moves with magnification means the part goes out of focus every time the operator zooms. Confirm whether the lens is parfocal and what the working distance is at the wide and telephoto ends.
4. Distortion across the range. Distortion is usually quoted as a single number, and the number is usually the best case. Ask whether it is measured at one magnification or across the range. A lens specified at 0.001% and a lens specified at 0.06% differ by a factor of 60, and for measurement work this is the parameter that decides whether the lens can be used for dimensioning at all.
5. Numerical aperture and resolution. NA sets how much light the lens collects and, together with wavelength, the smallest resolvable feature. The diffraction-limited resolution is commonly estimated as:
Resolution ≈ 0.61 × λ / NA
At λ = 550 nm and NA = 0.025, that gives ≈ 13.4 µm of optical resolution. This is the optical limit of the lens; the achievable measurement resolution on a part also depends on the camera pixel pitch and the sampling ratio, and the two should never be presented as the same number.
6. Mount and thread. C-mount remains the standard for industrial zoom bodies. Confirm the mount type, and confirm whether the existing setup uses an additional tube or adapter, since that changes total magnification per the formula above.
Measured values from the POMEAS zoom lens line:
| Model | Magnification range | Zoom ratio | Sensor | Mount | Distortion | NA | Working distance |
|---|---|---|---|---|---|---|---|
| **LZL-12102-M12** | 0.58×–7.5× | 12.5× | 2/3" | — | ≈ 0.001% | 0.025 | — |
| **PMS-LZH-14105K** | 0.55×–7.6× | 14× stated (13.8× computed) | 2/3" | C-Mount | 0.04% | 0.023 | — |
| **4K-ZOOM-0.68X-5.0X** | 0.68×–5.0× | 6.5× | 1" | C-Mount | as low as 0.02% | — | 80 mm |
| **LZ-63101** | 0.7×–4.5× | 6.5× | 2/3" | coaxial | −0.06% | — | — |
| **LZG-63104-A** | 0.7×–4.5× | 6.5:1 | 2/3" | C-Mount | ≈ 0.001% | 0.03 | — |
Reading the table against the six checks:
- The LZL-12102-M12 is the closest match to a 12× requirement, spanning 0.58×–7.5× on a 2/3-inch sensor with distortion around 0.001%. - The PMS-LZH-14105K covers a slightly wider span (0.55×–7.6×) and is motorised (电动变倍), which matters when the zoom position has to be reproducible or driven from software. - The 4K-ZOOM-0.68X-5.0X is the option when the camera carries a 1-inch sensor; the other four are built for 2/3-inch and will vignette on 1-inch. - LZ-63101 and LZG-63104-A both sit at the widely used 0.7×–4.5× range, with LZG-63104-A specified at ≈ 0.001% distortion and NA 0.03.
Distortion figures quoted as "≈ 0.001%" and "0.04%" come from different models and should not be compared as if measured under identical conditions; each is the value published for that model.
Scenario 1 — Re-inspection station with mixed part sizes. A station handling parts from roughly 2 mm to 15 mm across needs the wide end for finding the part and the telephoto end for measuring a feature. The 0.58×–7.5× span gives 15.2 mm down to 1.17 mm horizontally on a 2/3-inch sensor, covering the range in one optic instead of swapping fixed-magnification lenses.
Scenario 2 — Motorised zoom driven from a recipe. When the same line runs several part numbers and the magnification has to change per recipe, reproducibility of the zoom position matters more than the span. The motorised PMS-LZH-14105K addresses this; a manual zoom body requires the operator to return to the same position by eye.
Scenario 3 — 4K / large-sensor camera upgrade. A station upgraded from a 2/3-inch to a 1-inch sensor keeps its resolution gain only if the lens covers 1 inch. Substituting a 2/3-inch zoom lens onto a 1-inch camera produces corner falloff; the 4K-ZOOM-0.68X-5.0X is specified for 1-inch coverage at 80 mm working distance.
Scenario 4 — Measurement rather than inspection. If the output of the station is a dimension rather than a pass/fail image, distortion and NA move to the top of the list. A 0.001% distortion figure and a known NA allow the optical contribution to the measurement uncertainty to be estimated; a single unqualified "low distortion" claim does not.
This is a parameter reference, not a compatibility statement. No claim is made that any POMEAS zoom lens is a drop-in replacement for a specific third-party zoom body, and none should be inferred. Whether a substitute lens works on a given station depends on the mechanical interface, the tube and objective combination already in place, the camera's flange distance, and the illumination — none of which can be settled from a datasheet.
Third-party brand and model names appear in this article only where they are publicly documented in customer-supplied intelligence (a machine vision integrator describing its own equipment). No third-party specification is quoted here, because none was independently verified.
Measurement accuracy on a real part is not equal to optical resolution. Optical resolution is a property of the lens and wavelength; measurement accuracy additionally depends on pixel sampling, contrast, edge definition, illumination stability, and the algorithm. Any number quoted as "resolution" should be read with this distinction in mind.
No. The ratio is the span between the telephoto and wide ends. A 12.5× lens in the POMEAS line runs 0.58×–7.5×, meaning the widest setting reduces the image to 0.58× and the longest enlarges it to 7.5×.
The lens does not cover the camera sensor. A zoom lens built for 2/3-inch will vignette on a 1-inch sensor. Check the sensor coverage specification before substituting.
Only if the lens is parfocal. Confirm this on the datasheet; if the working distance shifts with magnification, the part leaves focus on a fixed fixture.
It is the value published for specific POMEAS models (LZL-12102-M12, LZG-63104-A). Distortion figures from different manufacturers are measured under different conditions and are not directly comparable unless the method is stated.
Yes, for the horizontal direction: FOV = sensor width / magnification. On an 8.8 mm sensor at 0.58× that is about 15.2 mm; at 7.5× about 1.17 mm.
Distortion across the zoom range and the numerical aperture. Both need to be specified, and the distortion value should state the magnification at which it was measured.
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