Physic Labs

Optics

Diffraction of light

Observe single-slit Fraunhofer diffraction built from Huygens sources, and verify the minima condition asin⁡θ=mλa\sin\theta=m\lambda plus the scaling of the central maximum, Δy≈2λL/a\Delta y\approx2\lambda L/a.

Undergraduate

⚠ If you reproduce this with a laser pointer, never aim the beam at eyes or reflective surfaces; diffraction patterns are best projected on a diffuse screen.

Equipment

  • Slit plane with secondary Huygens sources; intensity screen
  • Sliders “Bước sóng λ”, “Khe rộng a”, “Khoảng màn L” (wavelength, slit width, screen distance)
  • “Đặt lại tham số” (reset parameters) button

Procedure

  1. Watch the pattern form

    Keep default settings and watch the Huygens wavelets from the slit interfere on the screen: a bright central maximum flanked by symmetric minima and weaker side lobes. Read the intensity profile and locate the first minimum.

  2. Narrow the slit

    Reduce the slit-width slider a and watch the pattern spread — counterintuitively, a narrower slit diffracts more. Read the angular position of the first minimum and check it against sin⁡θ=λ/a\sin\theta=\lambda/a; halving a should double the width Δy≈2λL/a\Delta y\approx2\lambda L/a.

  3. Change λ and L

    Sweep the wavelength slider and then the screen distance L: the whole pattern scales linearly with both, Δy∝λL\Delta y\propto\lambda L. Pick one setting, compute the slit width from the measured central width via a=2λL/Δya=2\lambda L/\Delta y, and verify it against the slider value.

Simulation

Experiment history

Francesco Maria Grimaldi coined the word “diffraction” after watching light bend around obstacles, published posthumously in 1665; he even described the fringes that wave theory would later explain. Newton examined the phenomenon but read it through his particle view of light, slowing acceptance of the wave picture. Augustin-Jean Fresnel's 1818 prize memoir united Huygens' principle with interference and computed diffraction patterns quantitatively — the famous Poisson-spot test confirmed it experimentally. Fraunhofer's grating work in the 1820s then made diffraction a precision tool for measuring wavelengths, the ancestor of modern spectroscopy.

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