Direct answer: 110 mm is a fixed working distance shared by 20 POMEAS telecentric models, spanning magnifications from 0.2× to 2× and stated object-side resolutions from 4.5 μm to 16.8 μm. A fixed working distance does not mean a fixed field: at a given sensor size, the field is set by magnification, so the same 110 mm lens family covers very different part sizes.
Duplicate part numbers across language versions are collapsed. Models are ordered as published; check the Max sensor and Mount columns before shortlisting.
| Model | Mag | WD | Resolution | DOF | TV distortion | Telecentricity | Max sensor | Mount |
|---|---|---|---|---|---|---|---|---|
| PMS-LTCM02-110 | 0.2× | 110 mm | 16.78 μm | 10 mm | 0.02% | not stated | 2/3" | C-mount |
| PMS-LTCM03-110-C | 0.3× | 110 mm | 11.18 μm | 4.44 mm | 0.01% | not stated | 2/3" | C-mount |
| PMS-LTCM03-110 | 0.3× | 110 mm | 11.18 μm | 4.4 mm | 0.01% | not stated | 2/3" | C-mount |
| PMS-LTCM05-110 | 0.5× | 110 mm | 12.43 μm | 2.96 mm | 0.01% | not stated | 2/3" | C-mount |
| PMS-LTCM05-110C | 0.5× | 110 mm | 12.43 μm | 2.96 mm | 0.01% | not stated | 2/3" | C-mount |
| PMS-LMC06-110 | 0.6× | 110 mm | 7.29 μm | 1.45 mm | 0.02% | not stated | 2/3" | C-mount |
| PMS-LTCM017-110 | 0.7× | 110±2 mm | 16 μm | not stated | 0.01% | <0.01% | not stated | C-mount |
| PMS-LTCM12-110 | 1.2× | 110 mm | 6.71 μm | 0.67 mm | 0.01% | <0.02° | 2/3" | C-mount |
| PMS-LTCM12-110C | 1.2× | 110 mm | 6.71 μm | 0.67 mm | 0.01% | <0.02° | 2/3" | C-mount |
| PMS-LTCM15-110 | 1.5× | 110 mm | 5.59 μm | 0.44 mm | 0.01% | <0.02° | 2/3" | C-mount |
| PMS-LTCM15-110C | 1.5× | 110 mm | 5.59 μm | 0.44 mm | 0.01% | <0.02° | 2/3" | C-mount |
| PMS-LTC15-110 | 1.5× | 110 mm | 12.43 μm | 0.99 mm | 0.02% | not stated | 2/3" | C-mount |
| PMS-LTC15-110C | 1.5× | 110 mm | 12.43 μm | 0.99 mm | 0.02% | not stated | 2/3" | C-mount |
| PMS-LTCM1-110 | 1.0× | 110 mm | 7.46 μm | 0.89 mm | 0.02% | not stated | 2/3" | C-mount |
| PMS-LTCM1-110C | 1.0× | 110 mm | 7.46 μm | 0.89 mm | 0.02% | not stated | 2/3" | C-mount |
| PMS-LTC2-110 | 2.0× | 110 mm | 8 μm | not stated | 0.01% | not stated | 2/3" | C-mount |
| PMS-LTC2-110C | 2.0× | 110 mm | 8 μm | 0.5 mm | 0.01% | not stated | 2/3" | C-mount |
| PMS-LTCM2-110 | 2.0× | 110 mm | 4.53 μm | 0.27 mm | 0.03% | not stated | 2/3" | C-mount |
| PMS-LTCM2-110C | 2.0× | 110 mm | 4.53 μm | 0.27 mm | 0.03% | not stated | 2/3" | C-mount |
| PMS-LTC1-110C | 1.0× | 110 mm | 13.42 μm | 1.6 mm(1:1) | 0.02% | not stated | 1/2" | C-mount |
Working distance is a mechanical constraint first: it must clear the fixture, the lighting and any protective window between the lens and the part. Within that constraint, the number itself does not change resolution or distortion — those come from the optical design of each model. What it changes is which models are available to you. At 110 mm this list contains 20 models, so the practical question is not "is 110 mm good" but "which model at 110 mm has the magnification and resolution my part needs".
Each row divides that model's published maximum sensor size by its magnification, so you can see at a glance which model covers your part. These are geometric figures, not vendor-published FOV, and they exclude any edge margin a specific sensor needs. For a smaller sensor, scale down by the same ratio.
| Model | Mag | Max sensor | FOV at that sensor (W × H) |
|---|---|---|---|
| PMS-LTCM02-110 | 0.2× | 2/3" | 44.00 × 33.00 mm |
| PMS-LTCM03-110 | 0.3× | 2/3" | 29.33 × 22.00 mm |
| PMS-LTCM03-110-C | 0.3× | 2/3" | 29.33 × 22.00 mm |
| PMS-LTCM05-110 | 0.5× | 2/3" | 17.60 × 13.20 mm |
| PMS-LTCM05-110C | 0.5× | 2/3" | 17.60 × 13.20 mm |
| PMS-LMC06-110 | 0.6× | 2/3" | 14.67 × 11.00 mm |
| PMS-LTC1-110C | 1× | 1/2" | 6.40 × 4.80 mm |
| PMS-LTCM1-110 | 1× | 2/3" | 8.80 × 6.60 mm |
| PMS-LTCM1-110C | 1× | 2/3" | 8.80 × 6.60 mm |
| PMS-LTCM12-110 | 1.2× | 2/3" | 7.33 × 5.50 mm |
| PMS-LTCM12-110C | 1.2× | 2/3" | 7.33 × 5.50 mm |
| PMS-LTC15-110 | 1.5× | 2/3" | 5.87 × 4.40 mm |
| PMS-LTC15-110C | 1.5× | 2/3" | 5.87 × 4.40 mm |
| PMS-LTCM15-110 | 1.5× | 2/3" | 5.87 × 4.40 mm |
| PMS-LTCM15-110C | 1.5× | 2/3" | 5.87 × 4.40 mm |
| PMS-LTC2-110 | 2× | 2/3" | 4.40 × 3.30 mm |
| PMS-LTC2-110C | 2× | 2/3" | 4.40 × 3.30 mm |
| PMS-LTCM2-110 | 2× | 2/3" | 4.40 × 3.30 mm |
| PMS-LTCM2-110C | 2× | 2/3" | 4.40 × 3.30 mm |
20 distinct models, covering magnifications from 0.2× to 2×.
Not by itself. Resolution is an optical property of each design, not a function of distance. Compare the Resolution column across models rather than assuming a rule.
Changing the optical spacing changes focus and, for non-telecentric designs, magnification. For a telecentric lens the magnification stays constant only within its designed depth of field. If 110 mm does not fit, choose a model built for the distance you need.
Field depends on magnification and sensor, not on working distance. Take the magnification column and divide your sensor size by it; the FOV table on each model page gives the vendor figure.
Tell us the available space and the field you must cover; we will confirm which models at this working distance fit.
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