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SCIENCE · INVESTIGATE AND EXPLAIN

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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Try

Why can two illuminated openings produce a dark band?

Open the experiment

Predict

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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Two-slit interference without a finite-width envelopeNormalized intensity I/I₀ · screen distance 2 m · fixed axes00.250.50.751-80-60-40-20020406080Screen position x (mm) · red marker: first positive featureBrightness strip encodes the same samples · not a camera image801 plot samples at 0.2 mm spacing · numerical feature positions are analytic
Positive-side feature positions and path differences
FeaturePath difference / wavelengthPosition (mm)Normalized intensityWithin plot?
Bright order 115.0000161Yes
Bright order 2210.0001251Yes
Bright order 3315.0004221Yes
Dark band 10.52.5000020Yes
Dark band 21.57.5000530Yes
Dark band 32.512.5002440Yes

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.

Pattern scale and approximation
QuantityValueMeaning
Slit center separation0.200 mmDistance between two narrow openings
Wavelength500 nmSame wavelength for all interfering contributions
First positive feature5.000016 mmBright order one
Small-angle estimate5.000000 mmL × wavelength / separation
Relative approximation difference0.000313%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.

Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.

Understand

Two contributions can cancel at one place

The model uses two equally strong, narrow slit contributions illuminated in phase. They have the same wavelength and a stable phase relationship: they are coherent. At the center of the screen both paths are equal, so the contributions reinforce. Away from the center their path lengths differ.

At wavelength 500 nm, a path difference of 500 nm is one full cycle, so the waves arrive in phase again. A path difference of 250 nm is half a cycle: one contribution is opposite to the other and equal amplitudes cancel. Read these conditions in the feature table before changing either control.

For the default separation 0.20 mm and screen distance 2 m, the first positive bright fringe is at 5.000016 mm. The first dark band is about 2.500002 mm from the center. Symmetric partners occur at negative positions. The first dark band is not at the first integer-wavelength path difference.

Turn path difference into phase

Let δ be path difference and λ wavelength, in the same length unit. The fraction δ/λ counts how many cycles one path adds. Phase difference is φ = 2πδ/λ radians: one cycle is 2π radians, and half a cycle is π radians. A radian is an angle unit; the phase angle describes an oscillation, not a ray’s direction on the diagram.

For integer m, δ = mλ gives bright fringes. For integer m, δ = (m + 1/2)λ gives dark bands in this equal-amplitude, in-phase-source model. At m = 0 the bright condition is the center; the first positive dark condition has m = 0 in the half-integer expression.

The far-field path-difference model is δ = d sin θ, where d is slit-center separation and θ is screen angle from the central direction. The screen is L = 2 m away. For horizontal screen coordinate x, sin θ = x/√(L² + x²). Convert x, L and d to compatible units before combining them. Keeping this geometric sine does not remove the far-field approximation used for the wave contributions.

Add amplitudes before finding intensity

Equal waves with amplitude E can sum to amplitude 2E when in phase, or zero when opposite. Intensity is proportional to the square of the resulting wave amplitude. In this ideal case the normalized pattern is I/I₀ = cos²(φ/2), where I₀ is the central intensity. At phase zero this is one; at phase π it is zero; at phase π/2 it is one-half.

A dark location does not mean the waves destroy energy everywhere. The pattern redistributes the intensity over positions. This finite, separately normalized plot is not a total-power accounting calculation. Its central value is fixed at one independently for every setting, so equal peak heights across different settings do not establish equal optical power.

The plotted curve is the numerical intensity ratio. The strip below encodes those values as display brightness on black; it is not a photograph, an exposure simulation or a prediction of human brightness perception. Use the graph and numerical table for comparisons.

Identify what was simplified

The two slits are treated as pointlike contributions. Their individual finite widths and resulting diffraction envelope are omitted, so this model’s bright fringes do not fade under a finite-width envelope. Real finite slits combine both effects. Unequal amplitudes or loss of coherence would also alter the contrast; neither is a control here.

This is a classical wave-intensity calculation. It does not simulate individual photon detections or establish conclusions about a quantum measurement experiment. A ray-only image calculation cannot produce the alternating intensity pattern shown here.

Transfer a phase claim

For wavelength 600 nm, classify path differences 300, 600 and 900 nm. Then find the normalized intensity for a 150 nm path difference in the ideal equal-amplitude model.

Check the interference transfer

300 nm and 900 nm are half-integer wavelength differences and are dark. 600 nm is one full wavelength and is bright. At 150 nm, δ/λ = 1/4 and φ = π/2, so I/I₀ = cos²(π/4) = 1/2.

OpenStax: Young’s double-slit interference introduces the coherent-source model. Continue to fringe spacing and inference to connect the pattern with the slit separation.

Apply

For coherent equal contributions with wavelength 500 nm, a path difference of 250 nm gives:

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Explain amplitude cancellation, coherence and why normalized intensity does not measure total transmitted power.

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