Digital Photography DeCal EECS98/198 Nathan Yan About this course -Technology of Camera Systems -Photographic Technique -Digital Lightroom About Me ^-doesn’t.

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Presentation transcript:

Digital Photography DeCal EECS98/198 Nathan Yan About this course -Technology of Camera Systems -Photographic Technique -Digital Lightroom About Me ^-doesn’t know anything about what he’s talking about About You In case you were wondering, this is the noise signature of an image, inverted

All cameras, film or digital, work the same: Photons are projected onto a photo-sensitive plane which records the light information How it works

By confining light to only photons which pass through a certain point, we begin to resolve “detail”

History of Camera Development Many pinhole-type cameras dating back to the 11 th century Joseph Niépce recorded the first photograph in 1826, using a photo-sensitive silver/chalk mixture Development of recording mediums more responsive to light: wet plates, dry plates George Eastman introduces photographic film in 1885, and debuts the “Kodak” camera in 1888 – a cheap and easy to operate camera that began to popularize cameras Oskar Barnack developed the Leica camera in 1925, which popularized 35mm film standard Ihagee introduced the first single-lens reflex camera, Exakta, in 1933, allowing photographers to view image “through the lens” Auto-focus developed in the Konica C35AF in 1977

History of Digital Camera Development Began with charged couple device (CCD) cameras that recorded to analog media Steve Sasson produced the first for Kodak in 1973 Solid state CCD that recorded output onto cassette tape Resolution: 10,000 pixels, or 0.01 megapixels First practical use in 1984, for journalism Canon RC-701 recorded images onto “video floppies” During 1984 Olympics images could be transmitted via telephone lines, and image quality was acceptable for newsprint JPEG image compression standard introduced in 1988 First true digital camera: Fuji DS-1P debuted in 1988, recording a computerized image file to onboard memory First camera with live image feed to LCD: Casio QV-10 in 1995 First “professional” digital SLR camera natively designed: 2.74MP Nikon D1 in 1999 First affordable “consumer” digital SLR: 6MP Canon Digital Rebel 300D in $1000

Input: Light «photons» Output: Electrical signals

Si

Many electrons Voltage: High Implication: Many photons detected, bright exposure Result: bright image Few electrons Voltage: Low Implication: Few photons detected, dark exposure Result: dark image Max electrons Voltage: Max Implication: Max photons detected, brightest exposure Result: White image No electrons Voltage: Zero Implication: No photons detected, darkest exposure Result: Black image

Si Photons Photoelectrons Electrical signal Accumulated charge Digital representation of electrical signal Image file Amplifier Amplified electrical signal

Photo wells Sensors ? ? ? We know the pixel is bright, but what color is it? Problem: Since the sensor only records light intensity, we can’t differentiate between colors! Thus, imaging sensors only record in black and white Solution: Color filtering, the most common form being the Bayer filter

1)Designates individual photosites to be either red, green, or blue (RGB) 2)Respective color filters are placed over each photosite 3)Thus, only the light energy corresponding to that color’s wavelength reaches the sensor 4)Thus the sensor can interpret the energy recorded at that photosite to be a measure of that certain color 5)Knowing the intensities of red, green, and blue light, we can derive the actual color

Color offset Since each photosite must be designated some color, the Bayer pattern of blue, green, and red photosites if offset, with blue tending towards top-left and red tending towards bottom-right Loses 2/3 of light information At each photosite, 2 of 3 colors are filtered out, and light information discarded Workarounds: -Expose pictures for 3x time -not practical for photography -Demosiac algorithms to interpolate missing 2/3 data D r a w b a c k s o f … Actual Image Raw Bayer Output Demosiaced Bayer Output

Photon rate Time End of exposure Ideal Rate of incoming light is constant Real life Rate of incoming light is fluctuating Photon rate Time How much fluctuation? √n Dictated by Poisson ( pwasõ) Distribution For n total photons in exposure, standard deviation =

Photons collected = n + √n If n = 10,000 photons, Photons collected = 10,000 + √10,000 = 10, photons √n, so what? Variable brightness = noise! Noise monster One of the photographer’s worst enemies

Proportion of Photon Fluctuation (√(n)/n) Photons

Proportion of Photon Fluctuation (√(n)/n) Photons

Proportion of Photon Fluctuation (√(n)/n) Photons