Connect optical path difference to bright and dark fringes
Predict two-slit interference from phase and compare amplitude with intensity.
Learning outcome: Relate integer and half-integer path differences to interference and explain the model’s coherence assumptions.
Starting recap
Wavelength is the distance for one cycle. Phase describes position within a cycle; a half-cycle offset reverses an oscillation.
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Why can two illuminated openings produce a dark band?
Open the experimentPredict
At separation 0.20 mm and wavelength 500 nm, predict whether path differences 0, 250 and 500 nm produce bright or dark bands.
Experiment
Inspect the first bright and dark feature rows at the default setting. Change wavelength to 700 nm and compare the feature positions while keeping separation fixed.
Compare path difference and interference fringes
Worked teaching model · synthetic values · Two equally strong coherent in-phase pointlike slit contributions; individual slit width and its diffraction envelope are neglected. Classical monochromatic scalar waves, normal incidence and ideal far-field angular interference at a screen 2 m away. Screen coordinate x uses sin(theta) = x / sqrt(L² + x²); retaining this screen geometry does not make the wave model an exact near-field calculation. Fixed screen range −80 to +80 mm; normalized intensity 0–1 with central intensity defined as one independently for each setting. No absolute power comparison, photon detection, noise, polarization mismatch or incoherence. The strip is a display encoding of model values, not a photograph or measured brightness. Features outside the finite plot remain listed.
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| Feature | Path difference / wavelength | Position (mm) | Normalized intensity | Within plot? |
|---|---|---|---|---|
| Bright order 1 | 1 | 5.000016 | 1 | Yes |
| Bright order 2 | 2 | 10.000125 | 1 | Yes |
| Bright order 3 | 3 | 15.000422 | 1 | Yes |
| Dark band 1 | 0.5 | 2.500002 | 0 | Yes |
| Dark band 2 | 1.5 | 7.500053 | 0 | Yes |
| Dark band 3 | 2.5 | 12.500244 | 0 | Yes |
Path difference is between the two slit centers. Bright orders have integer wavelength differences; dark bands have half-integer differences. Negative-side features mirror the positive side. The finite sample grid may not land exactly on an analytic maximum or minimum.
| Quantity | Value | Meaning |
|---|---|---|
| Slit center separation | 0.200 mm | Distance between two narrow openings |
| Wavelength | 500 nm | Same wavelength for all interfering contributions |
| First positive feature | 5.000016 mm | Bright order one |
| Small-angle estimate | 5.000000 mm | L × wavelength / separation |
| Relative approximation difference | 0.000313% | Relative to retained screen geometry; not experimental uncertainty |
Every setting has its own central normalization I₀. Changing slit width or separation and seeing the same peak value does not establish equal total power. The two-slit model deliberately omits the finite-width envelope that would modulate real double-slit fringes.
First positive bright fringe at 5.000016 mm; small-angle spacing estimate 5.000000 mm.
Small-angle estimate for the first positive feature differs by 0.000313% from retained screen geometry. Intensity is normalized separately for each scenario; peak height is not transmitted power.
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Explain amplitude cancellation, coherence and why normalized intensity does not measure total transmitted power.
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