The microscope depth of field is the range of specimen depths judged acceptably sharp for a fixed imaging configuration and focus setting. It is an object-space tolerance defined by a sharpness criterion. It differs from microscope working distance, a physical clearance, and from image-space depth of focus. The accepted range depends on numerical aperture, wavelength, detector/display sampling and the criterion used to judge blur.
An original geometric model makes the criterion explicit. Let a local light cone have object-side half-angle . An axial defocus gives blur diameter approximately . If acceptable object-space blur diameter is at most , the symmetric depth range isThis cone model ignores diffraction and aberrations; it provides a stated geometric estimate, not a universal microscope specification.
For , refractive index and numerical aperture , the total range is about7.75µm. Raising the aperture to0.50 with the same blur criterion reduces it to about3.46µm. The manufacturer's iris discussion describes this tradeoff qualitatively: closing the aperture increases depth of field while reducing resolving power.[ref]
Labeling of Objectives by Leica Microsystems. “Numerical Aperture”; “Iris Diaphragm”, depth-of-field/resolution tradeoff
In a diffraction-limited comparison, choosing a tolerable blur scale proportional to and using at small angle yields a depth scale proportional to . The prefactor depends on the stated sharpness criterion. It should not be treated as one exact range independent of contrast, sampling or the way the image is assessed.
For a simple acceptance example, suppose the adopted total range is6µm and a nominally flat inspected surface varies from−4 to+4µm about a center focus. The8µm extent does not fit inside that6µm interval. Moving focus shifts which parts qualify but does not increase the interval width. A larger-looking image also does not prove better diffraction-limited resolution or a larger axial acceptance range.
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