Problem 9 IYPT 2027

9. Photographic bokeh

Optics

Problem Description & Analysis

Official Problem Statement

Bokeh is an effect observed in photographs that show objects at different distances from the camera and have both sharp and out-of-focus areas. If a slit is placed in front of the lens of the camera, the image may have unusual anisotropic distortions in out-of-focus areas, while in-focus areas remain undistorted and sharp. Investigate how the properties and sharpness of resulting images depend on relevant parameters.


Geometric Optics — Circle of Confusion

When a point source lies outside the camera’s focal plane, the cone of light from the lens forms a Circle of Confusion (CoC) on the sensor instead of a point:

$$c = frac{f^2}{N,d_o}left|frac{d_o – d_text{focus}}{d_text{focus}}right|$$

f — focal length (m)
N — f-number (= f/D_aperture)
D = f/N — aperture diameter (m)
d_o — object distance from lens (m)
d_focus — distance the camera is focused at (m)
c — CoC diameter on sensor (m)

Thin-lens law to convert object distance to image distance:

$$frac{1}{d_o} + frac{1}{d_i} = frac{1}{f}$$


Depth of Field

Depth of Field (DoF) is the range of object distances for which CoC stays below an acceptable threshold c_max (typically c_max ≈ d_sensor/1500 for digital cameras):

$$text{DoF} approx frac{2,N,c_text{max},d_o^2}{f^2}$$

Key relationship: smaller N (wider aperture) → shallower DoF → stronger bokeh.

f-number Aperture dia. (f=50mm) Depth of field Bokeh
f/1.4 35.7 mm Very shallow Very large
f/2.8 17.9 mm Shallow Large
f/5.6 8.9 mm Moderate Moderate
f/11 4.5 mm Deep Small
f/22 2.3 mm Very deep Gone + diffraction

Fourier Optics — Bokeh Shape

In Fraunhofer (far-field) diffraction, the intensity distribution at the focal plane is the squared magnitude of the 2D Fourier transform of the aperture function A(u,v). This is the Point Spread Function (PSF):

$$text{PSF}(x,y) = left|mathcal{F}{A(u,v)}right|^2$$

For a circular aperture of diameter D:

$$text{PSF}(r) = left[frac{2J_1(pi D r/lambda f)}{pi D r/lambda f}right]^2$$

where J₁ is the first-order Bessel function. First zero at r = 1.22λf/D (Rayleigh criterion).

Aperture shape → Bokeh shape:
• Circular aperture → Airy disc (disc + concentric rings) — smoothest bokeh
• Hexagonal aperture → hexagonal disc — common in mid-range lenses
• n-sided polygon → n “sword” streaks radiating from bright points
• Star/heart → Fourier transform of that shape (decorative)

Diffraction and Optimal Aperture

At very small apertures, diffraction dominates over geometric blur. The optimal f-number balancing geometric aberrations and diffraction is:

$$N_text{opt} approx sqrt{frac{f cdot c_text{max}}{1.22,lambda}}$$

For f = 50mm, c_max = 0.03mm, λ = 0.55μm: N_opt ≈ f/8.


Cat’s-Eye Bokeh

Off-axis point sources produce elliptical “cat’s-eye” bokeh due to mechanical vignetting: the lens barrel clips the effective aperture as seen from the edge of the sensor, making it elliptical rather than circular. This effect is desirable in cinematic lenses.


Experimental Setup

Constructing aperture filters

  • Cut aperture shapes (circle, hexagon, heart, star) from black card stock.
  • Attach to the lens front or hold in a filter holder.
  • Photograph a background of point light sources (LED arrays, city lights at night).
  • Keep focused object distance fixed; vary the background defocus distance.

Quantitative measurements

  • Measure CoC diameter at various defocus distances; compare with formula.
  • Measure DoF vs. f-number and verify the N·d_o²/f² scaling.
  • Extract PSF by photographing a single LED from far away; compare FFT of bokeh image with aperture shape.

Core of the Problem — The Slit and Anisotropic Distortion

The problem statement specifically asks about a slit placed in front of the lens that causes “unusual anisotropic distortions.” This anisotropy follows directly from the 2D Fourier transform of the aperture function:

Circular aperture (standard)

• Aperture: $A(u,v) = text{circ}(r/R)$
• Fourier transform: Airy disc pattern (disc + concentric rings)
Isotropic: rotationally symmetric — round bokeh in all directions

Vertical slit

• Aperture: $A(u,v) = text{rect}(u/w)cdottext{rect}(v/H)$ with $H gg w$
• Fourier transform: $text{sinc}(wx/lambda f)cdottext{sinc}(Hy/lambda f)$
Anisotropic: PSF is stretched in the $x$-direction (perpendicular to slit)

PSF width in each direction is inversely proportional to the aperture dimension in that direction:

$$Delta x_text{PSF} = frac{lambda f}{w}, qquad Delta y_text{PSF} = frac{lambda f}{H}$$

Since $H gg w$, we have $Delta x gg Delta y$ — the PSF is stretched horizontally (perpendicular to the slit). Out-of-focus points appear as elongated horizontal streaks on the sensor instead of circles.

Slit Aspect Ratio and Anisotropy

$$text{Bokeh stretch ratio} = frac{Delta x_text{PSF}}{Delta y_text{PSF}} = frac{H}{w}$$

A slit with $H/w = 10$ produces bokeh stretched 10× in the transverse direction. This linear relationship between slit geometry and bokeh distortion is directly testable.

Aperture type PSF / Bokeh shape Isotropy
Circle Airy disc + rings Fully isotropic
Vertical slit Horizontal line (sinc²) Anisotropic — transverse stretch
Hexagon Hexagonal disc Nearly isotropic (6 axes)
Triangle Disc + 3 lobes Anisotropic (120°)
$n$-point star $n$ radial spikes Anisotropic ($360°/n$)

Interactive Python Simulation — Aperture Shapes and PSF Patterns

This simulation computes the 2D Fourier transform of four aperture shapes and shows the corresponding bokeh (PSF) patterns:

Key results from the simulation:

  • Slit: PSF is a narrow horizontal line — out-of-focus highlights become horizontal streaks (this IS the anisotropic distortion the problem asks about).
  • Circle: PSF is fully rotationally symmetric — round isotropic bokeh.
  • Hexagon: hexagonal PSF — common in commercial lenses with 6-blade apertures.
  • Core law: PSF width ∝ λf / aperture dimension — smaller aperture dimension → larger PSF in that direction.

References

  1. Goodman, J.W. (2005). Introduction to Fourier Optics, 3rd ed. Roberts & Company.
  2. Hecht, E. (2016). Optics, 5th ed. Pearson.
  3. Born, M. & Wolf, E. (2013). Principles of Optics, 7th ed. Cambridge University Press.
  4. Nasse, H.H. (2010). Depth of Field and Bokeh. Carl Zeiss Camera Lens Division Technical Note.
  5. IYPT 2027 Problem 9. iypt.org

Technical Glossary

Term Persian equivalent Definition
Bokeh بوکه The aesthetic quality of out-of-focus blur in photography; from Japanese 暈け (haze/blur)
Circle of Confusion (CoC) دایره‌ی گیجی The disk formed on the sensor by an out-of-focus point; its shape mirrors the aperture shape
Point Spread Function (PSF) تابع گسترش نقطه The image of an ideal point source; describes how any out-of-focus point is smeared by the lens system
Aperture دیافراگم The opening through which light enters the lens; its shape (circle, slit, polygon) determines bokeh shape
Depth of Field (DoF) عمق میدان The range of distances over which the CoC stays below the human perception threshold
Fraunhofer diffraction پراش فراونهوفر Far-field diffraction; diffraction pattern = Fourier transform of the aperture — circle → Airy disc; slit → elongated streak
F-number (f-stop) عدد f Ratio of focal length to aperture diameter: $N = f/D$; smaller N = wider aperture = more blur
Anisotropic bokeh بوکه‌ی ناهمسانگرد Bokeh that differs in shape along different directions; a narrow vertical slit → horizontally elongated ellipses

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