Physic Labs

Optics

Light interference — Young’s experiment

Measure the fringe spacing of Young's double-slit experiment while varying wavelength, slit separation and screen distance; verify i=λD/ai = \lambda D/a against the simulation readout.

High school

Equipment

  • Coherent source through two slits — “Wavelength λ” slider (400–700 nm)
  • “Slit separation a” and “Screen distance D” sliders
  • Fringe screen with intensity plot and fringe-spacing readout
  • “Reset parameters” button

Procedure

  1. Hold a and D, sweep the wavelength

    Fix “Slit separation a” and “Screen distance D”; drag “Wavelength λ” from 400 to 700 nm and watch the fringes spread. Record the readout i (mm) at two wavelengths and check that i₂/i₁ ≈ λ₂/λ₁ from i=λD/ai = \lambda D/a.

  2. Sweep a and D, build a comparison table

    Decrease a then increase D in turn; each time read i and tabulate it against λD/a\lambda D/a. Check that i is inversely proportional to a and proportional to D; use “Reset parameters” to return to the standard configuration between measurements.

  3. Predict the fringe order by color

    Set λ to the two ends of the spectrum and predict which pattern is wider before looking; explain why the experiment let Young measure visible-light wavelengths without any microscope — only a ruler for the fringe spacing.

Simulation

Experiment history

In 1801 Thomas Young presented to the Royal Institution his experiment splitting a light beam with two narrow slits, obtaining alternating bright and dark fringes — the first experimental evidence for the wave nature of light, against the corpuscular model associated with Newton. From the fringe spacing he estimated visible wavelengths at under a micrometre, a startling figure for the time. Augustin Fresnel developed the quantitative wave theory and in 1816 used a biprism to create two coherent sources without slits. After the wave theory prevailed through speed-of-light measurements (Fizeau–Foucault, 1850), the double-slit experiment became canonical; in quantum mechanics it remains the standard illustration of wave–particle duality.

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