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Polished, brushed and coated metal fail differently under a ring light: the mirror throws light away, the brushed surface fans it out, the coated surface does both. Coaxial illumination — light injected on the camera's own axis — is the primary choice for flat mirror-like and coated parts; curved or strongly brushed geometry needs a diffuse or dome source.
| Surface | Reflection path | Off-axis light | Coaxial light |
|---|---|---|---|
| Mirror-like: polished, ground, glass, wafer | Specular (Fresnel) at the angle of incidence | Lobe misses the lens; surface reads black | Even bright background; tilt or absorption breaks it |
| Brushed: brushed stainless, turned finish, rolled sheet | Elongated lobe perpendicular to the tool marks | Brightness swings with lay direction | Works on fine roughness; lay-dependent brightness remains |
| Coated: plated, chromed, anodised, PVD | Top-surface return plus a weaker return from the layer interface | One highlight; buried layers invisible | Two overlapping returns: the ghost double highlight |
A coaxial unit folds light onto the camera axis with a half-mirror, so the part is lit perpendicular to its surface and the specular return retraces the same path into the lens. The flat background turns bright and even — the precondition for seeing anything by contrast — while a scratch, burr, laser mark or 2D code that tilts or diffuses the return breaks that field.
The limit is geometric: the on-axis condition holds only where the surface normal is parallel to the axis, so a cylinder returns a narrow top band and a sphere a small spot. Curved metal belongs to a dome source. The axis itself comes from an external coaxial light or from the lens: POMEAS builds coaxial telecentric models such as PMS-LTC1-110C (1.0X, WD 110 mm, 1/2″) and PMS-LTCM1-110C (1.0X, WD 110 mm, 2/3″), matched at the factory.
| Surface / geometry | Primary light | Add or avoid |
|---|---|---|
| Flat mirror-like metal | Coaxial | Crossed polarizer if the return clips; diffuser if a hotspot appears |
| Flat brushed metal | Coaxial + diffuser, or dome | Avoid a collimated bar light along the lay |
| Coated / plated flat | Coaxial for the top layer, diffuse dome for colour and blisters | Run both channels and compare |
| Cylinder, sphere, radii | Dome | Coaxial only as a second channel on the top band |
| Recessed features, bores, side walls | Low-angle bar or point light | Coaxial cannot reach a wall facing away |
A hotspot is energy concentrated in the middle of the field. The causes are the fold-mirror geometry and the collimation of the emitted beam: a centre-biased beam is brightest at the centre, auto-exposure darkens the frame, and corner contrast is lost. Three remedies, in order:
Formula (calculated): β = sensor size ÷ FOV, so FOV = sensor size ÷ β and FOVdiag = √(FOVW² + FOVH²). The window must cover that diagonal plus an alignment margin.
Worked example. PMS-LTCM12-110C is a 1.2X coaxial telecentric lens, WD 110 mm, 2/3″ format, publishing a 7.3 × 5.5 mm field. The check runs backwards: 7.3 × 1.2 = 8.76 mm, matching the standard 2/3″ width of 8.8 mm. Its diagonal is √(7.3² + 5.5²) = 9.14 mm (calculated), so a window near 9 mm is the minimum and 11–12 mm is comfortable. Low magnification is harder — PMS-LTCM03-110-C (0.3X, WD 110 mm) gives roughly 29 × 22 mm, a diagonal near 36 mm.
Most coaxial-light failures on metal are assembly problems:
| Parameter | Specification |
|---|---|
| Supply / controller | 24 V DC; recommended controller VP-DPI2404-4-RS232T |
| Colours | Standard red 625 nm, white 6500K, blue 470 nm; optional green 525 nm, infrared 850–950 nm, ultraviolet 365–395 nm |
| Power / environment | 0.8–120 W depending on model; 0–40 °C; 20–85% RH non-condensing |
| Cable / accessories | 0.5 m standard, 1/3/5 m extensions; diffuser plate, brightness controller |
| Lifetime / housing | Over 30,000 h at 50% brightness (white); aluminium alloy |
| Surfaces / detection / customisation | Mirror-like metal, glass, wafer and other highly reflective surfaces; scratches, characters, 2D codes, surface defects; size, colour, working distance and field of view customisation |
| Symptom | Likely cause | Action |
|---|---|---|
| Field black with the light on | Not specular there, or beam blocked | Check a polished reference; verify outlet, cable, controller channel |
| Bright centre, dark corners | Hotspot — window far larger than the field | Fit the diffuser; set the light to the lens working distance |
| Defect seen in one direction only | Directional scattering from the scratch | Re-check with the part rotated 90°; add a diffuse channel |
| Washed-out frame, no contrast | Specular return clipping the sensor | Crossed polarizers; lower power, longer exposure |
| Dark ring at the field edge | Window or bore smaller than the field | Compare the field diagonal with the clear diameter |
| Dark frame after adding the analyser | Analyser blocking the useful signal too | Raise power or exposure; try partially crossed |
| Result drifts after maintenance | Geometry altered and not recorded | Restore the recorded recipe |
If the finish and defect set are defined, send the part drawing, the required field of view and the defect specification and we will confirm the coaxial configuration and control option. Lens side: the telecentric lens selection guide and what a telecentric lens is and when to use one. For glass, wafers or fibre end faces: fibre end face inspection with a 10X telecentric lens. Share your workpiece details through the contact page.
Partly, and the limit is geometric. A coaxial system illuminates effectively only where the surface normal is parallel to the coaxial axis, so a cylinder shows a narrow bright band along its top line and a sphere a small spot. That band is enough to inspect a mark near the top of the part, and it suits a shaft rotated under the camera. For full-surface work, use a diffuse dome source and keep the coaxial channel for the top band.
Not always, but it is the standard remedy when the specular return saturates the sensor and flattens contrast. A linear polarizer on the illumination side plus an analyser on the camera side, set to crossed, blocks the return that kept its polarization at the smooth surface and passes the depolarised light scattered by a scratch, an edge or a printed feature. The cost is exposure headroom, since the analyser also removes useful signal. Start without polarizers, add them when the histogram shows clipping.
It depends on whether the lens choice is still open. A built-in coaxial design matches the illumination path, front aperture and working distance at the factory, which removes the front-window alignment error that most often produces a dark ring at the field edge. POMEAS supplies telecentric lenses with a built-in coaxial channel across several magnifications. A separate coaxial light gives more freedom on window size but adds one interface to align; for a new station the built-in route is lower risk.
Often better than an off-axis light, because the on-axis return makes the flat background bright and the code elements appear as a local modulation of it. Laser marks on polished metal generally work well under coaxial illumination, and a shorter wavelength such as blue 470 nm suits a mark that changes the surface rather than the colour. Dot-peened codes create small pits that scatter off axis, so they may decode better under a diffuse or low-angle bar source. Verify with the reader software, since a code that looks acceptable can still fail decode.
Raise the illumination power first, then lengthen the exposure if the part is not moving; the coaxial light family covers a wide power range depending on model and is specified for use with a brightness controller. If power is already at the limit, move from fully crossed to a partially crossed position, which returns some of the specular component while keeping part of the contrast gain. A third option: if the hotspot rather than the specular level is the problem, a diffuser plate redistributes energy without costing exposure.
No, the coaxial versions must be selected by model. Built-in coaxial and coaxial-illumination models are specific catalogue items listed with their magnification and working distance, and non-coaxial models in the same magnification range do not have the coaxial channel. In the low-magnification range, for example, the 0.3X coaxial model is a distinct part number while the 0.2X model in the same family is not a coaxial design. Check the catalogue rather than assume, and state the coaxial requirement when requesting a quotation.
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