SCI 200 Physical Science Lecture 11 Sources of Color Rob Daniell August 4, 2011 Sources of Color Part I: Self-luminous objects Objects that emit their own light Part II: Non-luminous objects Object that a visible due to reflected light revised 2011.08.03 SCI200 - Lecture 11 2 Sources of Color Part I: Self-luminous objects Thermal radiators Non-thermal sources Sources: Malacara, Daniel: Color Vision and Colorimetry: Theory and Applications,SPIE Press, Bellingham, 2001 Especially Chapter 2. Various Wikipedia articles, particularly “Liquid Crystal Display” and “Backlight” revised 2011.08.03 SCI200 - Lecture 11 3 Sources of Color: Self-luminous objects Thermal radiation Any object with a finite temperature radiates electromagnetic (EM) waves “free” electrons vibrate (oscillate) due to thermal energy Oscillating electrons emit EM waves Light consists of EM waves between 400-700 nm An ideal thermal radiator is termed a “black body” If it radiates EM waves (light), why is it “black”? revised 2011.08.03 SCI200 - Lecture 11 4 Sources of Color: Self-luminous objects Black body A good emitter and a good absorber Because of the “free” electrons A black body not only emits EM waves, It absorbs EM waves. No reflection At low temperatures little radiation good absorption So a black body looks black revised 2011.08.03 SCI200 - Lecture 11 5 Sources of Color: Self-luminous objects Black body radiation Thermal equilibrium Characterized by a definite temperature Usually expressed in kelvins (K) TK = 273 + TC TK = 273 + (5/9)(TF –32) Characterized by a specific spectrum Intensity of radiation as a function of wavelength First use of “quantum hypothesis” revised 2011.08.03 SCI200 - Lecture 11 6 Sources of Color: Self-luminous objects Visible wavelengths: 400-700 nm Black body spectrum Wavelength of peak emission intensity lmax = 2.9 T´10 revised 2011.08.03 6 nm K SCI200 - Lecture 11 7 Sources of Color: Self-luminous objects Black body spectrum in the visible range revised 2011.08.03 SCI200 - Lecture 11 8 Sources of Color: Self-luminous objects Real (as opposed to ideal) radiators Sun Surface temperature about 5500 K Incandescent light bulbs Filament (usually tungsten) heated by electric current Bulb filled with inert gas (e.g., argon) to prevent oxidation About 90% of the power is emitted as heat Approximate black body spectrum revised 2011.08.03 SCI200 - Lecture 11 9 Sources of Color: Incandescent light bulbs Incandescent light bulbs Filament (usually tungsten) heated by electric current Bulb filled with inert gas (e.g., argon) to prevent oxidation Clear or frosted glass revised 2011.08.03 SCI200 - Lecture 11 10 Sources of Color: Self-luminous objects Solar spectrum & equivalent black body spectrum revised 2011.08.03 SCI200 - Lecture 11 11 Sources of Color: Self-luminous objects Color temperature Temperature of a black body that would have the same color as the emitter For daylight Color temperature varies through the day Color temperature varies with cloud cover etc. For incandescent bulbs Color temperature is very close to actual temperature revised 2011.08.03 SCI200 - Lecture 11 12 Sources of Color: Self-luminous objects Color temperature & chromaticity revised 2011.08.03 SCI200 - Lecture 11 13 Incandescent light sources Incandescent light sources glow from their own heat and emit a “black body spectrum.” Incandescent light sources revised 2011.08.03 SCI200 - Lecture 11 14 Sources of Color: Self-luminous objects Color temperature Note that lower color temperatures correspond to redder colors “Cooler” and “warmer” colors refer to psychological perception To produce “warmer” (redder) colors, lower the color temperature To produce “cooler” (bluer) colors, raise the color temperature revised 2011.08.03 SCI200 - Lecture 11 15 Sources of Color: Self-luminous objects Non-thermal sources Wide variety Color temperature usually has little to do with the operating temperature Color temperature is often a poor approximation to the actual color of the emitted light revised 2011.08.03 SCI200 - Lecture 11 16 Sources of Color: Self-luminous objects Gas discharge lamps Glass tube filled with A low pressure gas such as hydrogen, argon, neon A vaporized metal such as sodium or mercury When an electric current is passed through the gas or vapor, the individual atoms are caused to emit light. Atoms absorb discrete amounts of energy from the electrons Atoms reemit the energy as photons, i.e., discrete amounts of energy Discrete “lines” (wavelengths) rather than thermal continuum Spectrum details depend on the pressure of the gas or vapor revised 2011.08.03 SCI200 - Lecture 11 17 Sources of Color: Self-luminous objects Fluorescent lamps A mercury vapor lamp with the interior of the glass tube coated with a fluorescent powder. A fluorescent material Absorbs short wavelength radiation Emits longer wavelength radiation revised 2011.08.03 SCI200 - Lecture 11 18 Sources of Color: Self-luminous objects Fluorescent lamps A mercury vapor lamp with the interior of the glass tube coated with a fluorescent powder. A fluorescent material Absorbs short wavelength radiation Emits longer wavelength radiation revised 2011.08.03 SCI200 - Lecture 11 19 Applications of self-luminous sources • Television, computer monitors, electronic displays • Cathode Ray Tube (CRT) • Largely obsolete • Liquid Crystal Display (LCD) • Many variations on the basic design revised 2011.08.03 SCI200 - Lecture 11 20 Applications of self-luminous sources • Cathode Ray Tubes • Date back to the 19th century • Vacuum tube • Electron “gun” • Electrons were first known as “cathode rays” • Screen coated with phosphors • Chemicals that glow when struck by electrons revised 2011.08.03 SCI200 - Lecture 11 21 Applications of self-luminous sources • Cathode Ray Tubes • Vacuum tube • Electron “gun” • Designed to produce a narrow beam • Electromagnet deflection coils to aim the beam • Screen coated with phosphors revised 2011.08.03 SCI200 - Lecture 11 22 Applications of self-luminous sources • Cathode Ray Tubes • Red, Green, & Blue signals • Each signal controls an electron beam • Screen devided into Red, Green, & Blue pixels • Phosphors continue to glow even after the electron beam has moved on revised 2011.08.03 SCI200 - Lecture 11 23 Applications of self-luminous sources • Liquid Crystal Displays • Based on the optical activity of Liquid Crystals • Liquids of long molecules, usually organic • Rotate the plane of polarization of light • Amount of rotation can be controlled through the applied voltage • Do not emit light themselves revised 2011.08.03 SCI200 - Lecture 11 24 Applications of self-luminous sources • Liquid Crystal Displays • 1-linear polarizer (vertical) • 2-glass substrate with electrodes • Shape of electrodes determines what can be displayed • 3-Liquid crystal • 4-glass substrate with common electrode • 5-linear polarizer (horizontal) • 6-reflecting screen or backlight revised 2011.08.03 SCI200 - Lecture 11 25 Applications of self-luminous sources • Liquid Crystal Displays • Backlight • White lights plus colored filters • Fluorescent light • “white” LEDs (Light Emitting Diodes) • Colored LEDs (RBG) revised 2011.08.03 SCI200 - Lecture 11 26 Sources of Color: Self-luminous objects A note on units related to brightness candela (cd) = the luminous intensity, in a given direction, of a source that emits monochromatic radiation of frequency 540x1012 hertz (555.6 nm) and that has a radiant intensity in that direction of 1/683 watt per steradian A common candle emits roughly 1 cd A 100 W incandescent light bulb emits about 120 cd Luminous flux 1 lumen = 1 cd sr = flux from 1 cd into 1 sr Illuminance (light received per unit surface area) SI unit: 1 lux (lx) = 1 lumen m-2 English unit: 1 foot-candle (fc) = 1 lumen ft-2 = 10.76 lx revised 2011.08.03 SCI200 - Lecture 11 27 Sources of Color: Self-luminous objects Illuminance (light received per unit surface area) SI unit: 1 lux (lx) = 1 lumen m-2 English unit: 1 foot-candle (fc) = 1 lumen ft-2 = 10.76 lx Can be measured by commercially available lux meters: revised 2011.08.03 SCI200 - Lecture 11 28 Sources of Color: Self-luminous objects Another definition of “foot-candle” revised 2011.08.03 SCI200 - Lecture 11 29 Sources of Color Part II: Non-luminous objects Various causes of color: Pigments Structural elements Atomic, molecular, and crystalline properties Sources: Chapter 9 of textbook (Gilbert & Haeberli, Physics in the Arts) Misc sources (mostly Wikipedia) revised 2011.08.03 SCI200 - Lecture 11 30 Sources of Color: Non-luminous sources Pigments Chemical compounds that absorb light of different wavelengths Reflected (or scattered) light is colored Appearance depends on Source of illumination Thickness of pigment coating Mixtures of various pigments Natural: “Animal, vegetable, and mineral” Synthetic revised 2011.08.03 SCI200 - Lecture 11 31 Sources of Color: Non-luminous sources Pigments Animal pigments include Melanin Eumelanin: skin color and dark hair colors Pheomelanin: red hair Carotenoids - not strictly animal Absorbed by animals from plants, algae, and photosynthetic bacteria Responsible for pinks of flamingos and salmon Blue eyes are due to lack of pigment Rayleigh scattering (as in the atmosphere) causes more blue light to be scattered Longer wavelengths are absorbed at the back of the iris revised 2011.08.03 SCI200 - Lecture 11 32 Sources of Color: Non-luminous sources Pigments “Vegetable” (i.e., plant) pigments include Chlorophyll (green) Participates in photosynthesis Carotenoids (yellow, orange, pink, or red) Tannin (black or brown) Anthocyanins (red or bluish purple) revised 2011.08.03 SCI200 - Lecture 11 33 Sources of Color: Non-luminous sources Pigments Mineral pigments are extremely varied Often oxides of metals Each chemical compound has a unique absorption and emission spectrum Discrete wavelengths Bands of wavelengths Used in paints, dyes, makeup, etc. Usually sold as powders Final colors depend on the liquid or paste base revised 2011.08.03 SCI200 - Lecture 11 34 Sources of Color: Non-luminous sources Structural colors: Iridescence If a material layer’s thickness is similar to the wavelength of visible light Interference effects produce color revised 2011.08.03 SCI200 - Lecture 11 35 Sources of Color: Non-luminous sources Structural colors: Iridescence If a material layer’s thickness is similar to the wavelength of visible light Interference effects produce color revised 2011.08.03 SCI200 - Lecture 11 36 Sources of Color: Non-luminous sources Structural colors: Iridescence If a material layer’s thickness is similar to the wavelength of visible light Interference effects produce color Relative phase depends on angle of incidence Colors vary with relative locations of source, layer, and observer revised 2011.08.03 SCI200 - Lecture 11 37 Sources of Color: Non-luminous sources Structural colors: Iridescence Examples: Soap bubbles Oil films Bird feathers Butterfly wings Beetle shells Pearls, mother of pearl Opals Fossils shells revised 2011.08.03 SCI200 - Lecture 11 38 Sources of Color: Non-luminous sources Gemstones Chemical composition Sometimes impurities can affect colors Ruby is corundum [Al2O3] with chromium impurities Emerald is beryl [Be3Al2(SiO3)6] with chromium impurities Beryl with other impurities takes on other colors: Aquamarine is beryl with Fe2+ Heliodor is beryl with Fe3+ Marganite is beryl with Mn2+ Etc., etc. revised 2011.08.03 SCI200 - Lecture 11 39 Sources of Color: Non-luminous sources Gemstones Active participation Blue sapphire: corundum [Al2O3] with iron (Fe) and titanium (Ti) impurities. When light hits the mineral it causes electrons to jump between the Fe and the Ti. Red and green light is absorbed in the process, leaving blue to be reflected back to the observer revised 2011.08.03 SCI200 - Lecture 11 40 Sources of Color: Non-luminous sources Gemstones Color centers Defects in the crystal structure trap electrons which can absorb light Often only certain wavelengths Other wavelengths are scattered, giving color to the gem Defects can be natural Occurring when the crystal forms Defects can be artificial Produced by exposure of the crystal to various forms of radiation revised 2011.08.03 SCI200 - Lecture 11 41 Sources of Color: Non-luminous sources Gemstones Semiconductor band gaps In order to conduct electricity, electrons must gain a minimum amount of energy Recall that light of shorter wavelengths has higher energy There is a maximum wavelength that can be absorbed Threshold is different for different semiconductors revised 2011.08.03 SCI200 - Lecture 11 42 Sources of Color: Non-luminous sources Gemstones Semiconductor band gaps Threshold longer than 700 nm: opaque Threshold shorter than 400 nm: transparent Threshold between 400 nm and 700 nm: colored Red, orange, or yellow Not blue revised 2011.08.03 SCI200 - Lecture 11 43 Sources of Color: Non-luminous sources Gemstones Impurities can cause multiple band gaps Permits blue color revised 2011.08.03 SCI200 - Lecture 11 44 Summary • Self-luminous sources • Thermal • Non-thermal • Non-luminous sources • Pigments • Structural color (iridescence) • Mineral color revised 2011.08.03 SCI200 - Lecture 11 45 Summary • Self-luminous sources • Thermal • Approximately a black body spectrum • Wavelength of peak emission varies with temperature • Non-thermal • Atomic or molecular process • Excitation by electrons or other non-luminous processes revised 2011.08.03 SCI200 - Lecture 11 46 Summary • Non-luminous sources • Pigments • Chemicals whose composition determines which wavelengths are absorbed and which are reflected or transmitted • Structural color (iridescence) • Relies on destructive and constructive interference effects • Depends on relative location of source, object, and observer revised 2011.08.03 SCI200 - Lecture 11 47 Summary • Non-luminous sources • Mineral color • Wide variety of mechanisms • Color is frequently caused by • Impurities • Structural defects • Peculiarities of the electronic structure of the material (semi-conductors) revised 2011.08.03 SCI200 - Lecture 11 48 Homework Assignment • No Homework Packet • Lab 8: Color Subtraction – Thursday, August 4 • Make-up Lab – Thursday, August 11 • Test #3, Thursday, August 11 – Chapters 7, 8, & 9 – Lectures 9, 10, & 11 revised 2011.08.03 SCI200 - Lecture 11 49