Separate slit spreading from circular-aperture resolution
A finite aperture spreads a wave even in a perfectly manufactured optical system. For a single slit of width w, the first dark directions satisfy w sinθ=λ. On a perpendicular screen at L, the central bright region extends between the two signs, so its width is2L tanθ. Confusing this full width with its half-width gives a factor-of-two error.
Learning outcome: Compare slit widths20,40,80 µm and circular diameters2,3,4 mm. Retain the two independent geometries and compare the stated source separation with the circular criterion. Explain which real-system observation could invalidate a claim based only on the ideal aperture formula.
Starting recap
Use normal-based angles, signed conjugate distances and explicit optical-path/reflection phases. Separate geometric direction, amplitude and energy; preserve focal and critical boundaries.
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A40 µm slit has first sine .015. At L=2 m the full central width is4(.015)/√(1−.015²)≈.0600068 m. A4 mm circular aperture has Rayleigh angle1.22×600e−9/.004=.183 mrad. The stipulated .2 mrad source pair meets this criterion; a3 mm aperture gives .244 mrad and does not.
Open the experimentPredict
For fixed wavelength, doubling a circular aperture diameter changes its Rayleigh angle by:
Experiment
Compare slit widths20,40,80 µm and circular diameters2,3,4 mm. Retain the two independent geometries and compare the stated source separation with the circular criterion. Explain which real-system observation could invalidate a claim based only on the ideal aperture formula.
Distinguish slit minima from a circular resolution criterion
Worked teaching model · synthetic values · Wavelength600 nm in air; slit far-field screen at2 m. Separately two incoherent equal-brightness point sources have angular separation.2 mrad through an ideal circular aperture. Rayleigh angle1.22 lambda/D is a stated criterion, not a universal detector or eyesight limit.
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Circular aperture criterion, not a binary detector law
Unlike graph quantities rescale independently; read units and values, not screen angles. 1: Rayleigh criterion (solid).2: supplied source separation (dashed). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Circular aperture criterion, not a binary detector law
Rayleigh criterion
| aperture diameter (mm) | angular separation (mrad) |
|---|---|
| 1 | 0.732 |
| 1.05 | 0.697143 |
| 1.1 | 0.665455 |
| 1.15 | 0.636522 |
| 1.2 | 0.61 |
| 1.25 | 0.5856 |
| 1.3 | 0.563077 |
| 1.35 | 0.542222 |
| 1.4 | 0.522857 |
| 1.45 | 0.504828 |
| 1.5 | 0.488 |
| 1.55 | 0.472258 |
| 1.6 | 0.4575 |
| 1.65 | 0.443636 |
| 1.7 | 0.430588 |
| 1.75 | 0.418286 |
| 1.8 | 0.406667 |
| 1.85 | 0.395676 |
| 1.9 | 0.385263 |
| 1.95 | 0.375385 |
| 2 | 0.366 |
| 2.05 | 0.357073 |
| 2.1 | 0.348571 |
| 2.15 | 0.340465 |
| 2.2 | 0.332727 |
| 2.25 | 0.325333 |
| 2.3 | 0.318261 |
| 2.35 | 0.311489 |
| 2.4 | 0.305 |
| 2.45 | 0.298776 |
| 2.5 | 0.2928 |
| 2.55 | 0.287059 |
| 2.6 | 0.281538 |
| 2.65 | 0.276226 |
| 2.7 | 0.271111 |
| 2.75 | 0.266182 |
| 2.8 | 0.261429 |
| 2.85 | 0.256842 |
| 2.9 | 0.252414 |
| 2.95 | 0.248136 |
| 3 | 0.244 |
| 3.05 | 0.24 |
| 3.1 | 0.236129 |
| 3.15 | 0.232381 |
| 3.2 | 0.22875 |
| 3.25 | 0.225231 |
| 3.3 | 0.221818 |
| 3.35 | 0.218507 |
| 3.4 | 0.215294 |
| 3.45 | 0.212174 |
| 3.5 | 0.209143 |
| 3.55 | 0.206197 |
| 3.6 | 0.203333 |
| 3.65 | 0.200548 |
| 3.7 | 0.197838 |
| 3.75 | 0.1952 |
| 3.8 | 0.192632 |
| 3.85 | 0.19013 |
| 3.9 | 0.187692 |
| 3.95 | 0.185316 |
| 4 | 0.183 |
| 4.05 | 0.180741 |
| 4.1 | 0.178537 |
| 4.15 | 0.176386 |
| 4.2 | 0.174286 |
| 4.25 | 0.172235 |
| 4.3 | 0.170233 |
| 4.35 | 0.168276 |
| 4.4 | 0.166364 |
| 4.45 | 0.164494 |
| 4.5 | 0.162667 |
| 4.55 | 0.160879 |
| 4.6 | 0.15913 |
| 4.65 | 0.157419 |
| 4.7 | 0.155745 |
| 4.75 | 0.154105 |
| 4.8 | 0.1525 |
| 4.85 | 0.150928 |
| 4.9 | 0.149388 |
| 4.95 | 0.147879 |
| 5 | 0.1464 |
At most 82 representative computed coordinates including endpoints; the plotted curve can use a finer grid. A table of a revealed generator is not independent measurement evidence.
supplied source separation
| aperture diameter (mm) | angular separation (mrad) |
|---|---|
| 1 | 0.2 |
| 1.05 | 0.2 |
| 1.1 | 0.2 |
| 1.15 | 0.2 |
| 1.2 | 0.2 |
| 1.25 | 0.2 |
| 1.3 | 0.2 |
| 1.35 | 0.2 |
| 1.4 | 0.2 |
| 1.45 | 0.2 |
| 1.5 | 0.2 |
| 1.55 | 0.2 |
| 1.6 | 0.2 |
| 1.65 | 0.2 |
| 1.7 | 0.2 |
| 1.75 | 0.2 |
| 1.8 | 0.2 |
| 1.85 | 0.2 |
| 1.9 | 0.2 |
| 1.95 | 0.2 |
| 2 | 0.2 |
| 2.05 | 0.2 |
| 2.1 | 0.2 |
| 2.15 | 0.2 |
| 2.2 | 0.2 |
| 2.25 | 0.2 |
| 2.3 | 0.2 |
| 2.35 | 0.2 |
| 2.4 | 0.2 |
| 2.45 | 0.2 |
| 2.5 | 0.2 |
| 2.55 | 0.2 |
| 2.6 | 0.2 |
| 2.65 | 0.2 |
| 2.7 | 0.2 |
| 2.75 | 0.2 |
| 2.8 | 0.2 |
| 2.85 | 0.2 |
| 2.9 | 0.2 |
| 2.95 | 0.2 |
| 3 | 0.2 |
| 3.05 | 0.2 |
| 3.1 | 0.2 |
| 3.15 | 0.2 |
| 3.2 | 0.2 |
| 3.25 | 0.2 |
| 3.3 | 0.2 |
| 3.35 | 0.2 |
| 3.4 | 0.2 |
| 3.45 | 0.2 |
| 3.5 | 0.2 |
| 3.55 | 0.2 |
| 3.6 | 0.2 |
| 3.65 | 0.2 |
| 3.7 | 0.2 |
| 3.75 | 0.2 |
| 3.8 | 0.2 |
| 3.85 | 0.2 |
| 3.9 | 0.2 |
| 3.95 | 0.2 |
| 4 | 0.2 |
| 4.05 | 0.2 |
| 4.1 | 0.2 |
| 4.15 | 0.2 |
| 4.2 | 0.2 |
| 4.25 | 0.2 |
| 4.3 | 0.2 |
| 4.35 | 0.2 |
| 4.4 | 0.2 |
| 4.45 | 0.2 |
| 4.5 | 0.2 |
| 4.55 | 0.2 |
| 4.6 | 0.2 |
| 4.65 | 0.2 |
| 4.7 | 0.2 |
| 4.75 | 0.2 |
| 4.8 | 0.2 |
| 4.85 | 0.2 |
| 4.9 | 0.2 |
| 4.95 | 0.2 |
| 5 | 0.2 |
At most 82 representative computed coordinates including endpoints; the plotted curve can use a finer grid. A table of a revealed generator is not independent measurement evidence.
| Quantity | Value | Unit |
|---|---|---|
| Single-slit first minimum angle | 0.859469 | degrees |
| Central slit maximum width on screen | 0.0600068 | m |
| Circular-aperture Rayleigh angle | 0.000183 | rad |
| Source angular separation | 0.0002 | rad |
| Meets stated Rayleigh separation criterion | 1 | flag |
| Diameter needed for equality | 3.66 | mm |
A narrower slit spreads its central pattern more, while a larger circular aperture lowers the stated resolution angle.
Single-slit first zeros obey w sin(theta)=lambda; the central screen width extends between both signs, giving 2L tan(theta). A circular aperture instead uses the supplied small-angle Rayleigh convention1.22lambda/D for two equal incoherent point sources. Detector noise, brightness imbalance, aberration and image processing can change actual distinguishability; this ideal criterion is not an eyesight or medical assessment.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
A narrower slit spreads its central pattern more, while a larger circular aperture lowers the stated resolution angle.
Single-slit first zeros obey w sin(theta)=lambda; the central screen width extends between both signs, giving 2L tan(theta). A circular aperture instead uses the supplied small-angle Rayleigh convention1.22lambda/D for two equal incoherent point sources. Detector noise, brightness imbalance, aberration and image processing can change actual distinguishability; this ideal criterion is not an eyesight or medical assessment.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
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