Depth of field is the height range around the best focus plane over which the image remains sharp enough for the task. The word acceptably is doing the work: the range depends on the criterion, which for visual inspection is the eye's tolerance and for measurement is the tolerance on the result.
This is why two datasheets can disagree about the same objective. One quotes a photographic criterion based on a print viewed at a distance, the other a metrology criterion based on edge position error. Neither is wrong, and they are not interchangeable.
For an inspection station the practical definition is the height range over which the feature being judged remains detectable. For a measurement station it is the range over which the reading stays inside tolerance.
Stating which criterion the application needs, before comparing objectives, prevents a specification built on mismatched definitions.
It also explains why field measurements often differ from catalogue figures: the criterion used in the field is the application's, not the datasheet's.
Depth of field scales roughly with the inverse square of magnification for a fixed aperture. Doubling the magnification reduces the usable height range to about a quarter. This is the dominant reason high magnification microscopy is difficult on parts with any height variation.
The practical effect is that a part which is comfortably covered at low magnification becomes a focusing problem at high magnification, even though the objective family is the same and the aperture setting identical.
The POMEAS microscope range spans magnification from 1 to 2 X and field of view from 10 to 360 mm, and the depth available at the high end is correspondingly narrow.
For a part with height variation the usual answer is to work at the lowest magnification that still resolves the feature, and to use digital magnification for display rather than optical magnification for capture.
That choice preserves depth, keeps the field, and in most inspection tasks loses nothing that matters.
On a telecentric lens, depth of field and telecentric depth are related but distinct. Depth of field is the range over which the image stays sharp. Telecentric depth is the range over which the magnification and the edge position stay constant, so the measurement remains correct.
A lens can produce a sharp image outside its telecentric range while producing a slightly wrong measurement, because the magnification has begun to change with distance. The image looks acceptable and the dimension does not.
This distinction is central to measurement applications and largely irrelevant to visual inspection. A station that only needs to see a defect can use the full depth of field; a station that measures a dimension must stay inside the telecentric range.
The practical check is to place a step artefact of known height in the field and verify that the measured dimension does not change as the step moves through the height range.
That test separates the two ranges on the actual hardware, which is more reliable than reading two datasheet figures.
Stopping down increases depth of field, because a narrower cone of light stays focused over a longer distance. The same narrowing increases diffraction, which reduces resolution. Beyond a certain point the depth gained is offset by the sharpness lost, and the image is neither deep nor sharp.
Most objectives have a setting where the two effects balance, usually two to three stops down from wide open. The exact point is model specific and worth measuring rather than assuming.
For a measurement application the criterion is not visual sharpness but edge position stability, which can peak at a different aperture than visual sharpness does.
Where the aperture is fixed by design, as on many industrial microscope units, this trade has already been made by the manufacturer and cannot be adjusted in the field.
Knowing which case applies determines whether aperture is a parameter the application can use or a constant it must live with.
Start from the height distribution of the actual production parts, not from the drawing. Measure a sample across the tolerance band and record the total spread within a part and between parts.
Compare that spread with the usable depth at the candidate magnification. If the spread is larger, the options are lower magnification, an autofocus axis, or a datum that presents a consistent surface.
For a conveyor application the between-part variation usually dominates, and a mechanical datum that presses each part against a reference is often cheaper than an autofocus axis.
Where the variation is inherent, such as on a casting or a stamped part, autofocus is usually the only workable answer, and the cycle time cost should be included in the station's throughput calculation.
Recording the height distribution as a number, rather than as a tolerance, is what makes the depth decision quantitative.
Depth of field stops being the constraint when the part is presented flat and at a controlled height, which is common on wafer, glass and machined flat surfaces. In that case the full budget can go to resolution and magnification.
At that point the limiting factors become illumination contrast, vibration and the sensor's sampling. Each of these has its own solution, and none of them is addressed by a deeper objective.
Recognising that the constraint has moved is important, because continuing to optimise depth of field wastes effort on a parameter that is no longer binding.
The check is straightforward: if the part's height variation is well inside the available depth, the depth is not the problem and the investigation should move elsewhere.
This is also the condition under which the highest magnification objectives become usable, and where their resolution advantage actually reaches the sensor.
Because it scales roughly with the inverse square of magnification at a fixed aperture. Doubling magnification reduces the usable height range to about a quarter. That is a property of the optics, not a limitation of a particular objective.
No. Depth of field is the range over which the image stays sharp. Telecentric depth is the range over which magnification and edge position stay constant, so the measurement remains correct. An image can be sharp outside the telecentric range while the dimension is already wrong.
Only up to a point. Stopping down increases depth but also increases diffraction, which reduces resolution. Most objectives balance the two two to three stops down from wide open. On fixed-aperture industrial units this trade has already been made by the manufacturer.
Place a step artefact of known height in the field and move it through the height range, recording the measured dimension at each step. The range over which the reading stays inside tolerance is the usable depth for measurement, which is usually smaller than the datasheet figure.
Measure the real height distribution first, then choose between lower magnification, an autofocus axis and better fixturing. For conveyor applications the between-part variation usually dominates, and a mechanical datum is often cheaper than autofocus.
No. Depth of field depends on magnification and aperture, not on sensor size. A larger sensor at the same magnification gives a larger field of view but the same depth. Changing the sensor does not change the focus behaviour.
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