Lecture #3 What you see is what you get 1/31/13 Homework • Problems up on web site • Due next Tuesday • Questions?? What are organisms’ visual tasks? Foraging Finding / choosing mates Avoiding predators Knowing when to stop What happens to light when we see? Today’s topics 1. 2. 3. 4. 5. Reflection Absorption / Transmission Measuring fR, fA, and fT Follow the photon’s path Spectral properties of light environments a. Terrestrial b. Aquatic c. Energy of a photon Light interactions • Matter will interact with light in one of 4 ways Reflected Absorbed Transmitted = Refracted Scattered • For now we will deal with transparent materials so scattering will be negligible Light interactions • Photons are conserved Light going in must go somewhere Iincident = ITrans + IReflect + Iabsorb = I0 • Express as fraction of I0 fT + fR + fA = 1 fT=fraction transmitted fR=fraction reflected fA=fraction absorbed Iabsorb I0 Ireflect Itrans 1. Reflection at interface • Light will reflect at interface between materials with different indices of refraction • For light perpendicular to surface fR = fraction _ reflected æ n2 - n1 ö fR = ç è n2 + n1 ÷ø 1 2 0 n=1.0 2 Water n=1.33 Reflection at biological interfaces is usually pretty small: air / water • fR, fraction reflected 2 fR,air-water æ n2 - n1 ö æ 1.33 -1.0003 ö =ç =ç = 0.02 ÷ ÷ è n2 + n1 ø è 1.33 +1.0003 ø 2 1 2 n=1.0 Water n=1.33 2. Absorption • Light will interact with molecules in material It can excite molecules. If it matches electron resonance, then it will be absorbed If not, it will be transmitted • We see what is not absorbed In the following, we assume… • Reflection is pretty small • Then fT + fR + fA = 1 that fT + f A = 1 and fR ≈ 0 so What does that mean??? Calculating transmission – solution of concentration, C • Beer’s law I = I 0 exp(-e l Cl) I0 I = I 0e εdepends on what substance is C is concentration l is the pathlength I, light transmitted through - e Cl l Calculating transmission - solution • Beer’s law I = I 0 exp(-e l Cl) I0 I Low concentration Less absorbed More transmitted depends on what substance is C is concentration l is the pathlength I0 I High concentration More absorbed Less transmitted Calculating transmission - solution • Beer’s law I = I 0 exp(-e l Cl) I0 I Short pathlength Less absorbed More transmitted depends on what substance is C is concentration l is the pathlength I0 I Longer pathlength More absorbed Less transmitted Calculating transmission - pure substance, like water • Beer’s law I = I 0 exp(-a l) is attenuation coefficient I0 I l Units all cancel so take exponential of a unitless number ε l C L-1 l L length-1 concentration-1 = L-1 molecules-1L3 = L2/molecule length concentration = molecule / L3 Transmission / absorption depend on wavelength I fT = = exp(-a l l) I0 fA = 1- fT =1- exp(-a l l) 3. Measuring transmission / absorption Measure I0 - just beam flashlight Fiber optic Spectrometer Measuring transmission /absorption Measure I with object in beam flashlight Fiber optic Transmission = I / I0 fT + f R + f A = 1 For small fR fA = 1-fT Spectrometer For reflective objects Specular reflection For opaque objects light scatters in all directions Specular reflection Scattered Reflected light vs scattered light Scattering / reflection depend on wavelength • n depends on Measuring reflection / scattering Fiber optic Light source How can we measure I0? Spectrometer Measuring reflection / scattering Fiber optic Light source Spectrometer Measure I0 of light Use white target that reflects all wavelengths Measuring reflection / scattering Fiber optic Light source Spectrometer Measure I reflected from object fRorS = I / I0 fRorS + fA + fT = 1 where reflection and scattering depend on angle For small fT fRorS = 1 - fA Examples of absorption and reflection • The return of the spectrometer Why does absorption matter? • Retinal pigments absorb certain wavelengths • Biological materials - Photosynthesis uses light to power life - Wavelengths scattered depend on absorption - Colors of animals, food - Define our environment 4. The photon’s path - How do we see? Sensitivity • Light from a source, I • Reflected by object, R • Detected by eye, S Intensity • Q= I *R *S Reflectance Q = quanta of light detected What light illuminates an object? • Irradiance Light flux on a surface - from all directions Photons /s m2 Irradiance Depending on detector set up, we might measure irradiance or radiance • Irradiance Light flux on a surface - from all directions Photons /s m2 Irradiance • Radiance Light flux from a particular direction and angle Photons /s m2 sr Radiance Light measurement • Many light meters measure watts / m2 Watts are joules / s and so are related to photons / s We’ll convert that in a minute • Some light meters measure lux This is like watts / m2 but they take human sensitivity into account Lux meter (measures irradiance – all angles) Bright sunlight 20,000 lux Eyes respond to photons • Eye doesn’t care about watts • Chemical reactions in eye detect individual photons Energy of light source is given in watts 75 W light bulb 5 mW laser How many photons in a Watt • Watt is a measure of power = energy / time 1 watt = 1 J/s • Convert watts to photons energy energy # photons Lightsource _ power(W ) = = * s one _ photon s # photons Lightsource _ power(W ) = s energy / one _ photon Energy of a photon – thank Planck • E = hf = h c / h is Planck’s constant = 6.6256 x 10-34 Js For 400 nm light: E = (6.6256 x 10-34 Js) (2.998 x 108m/s) 400 x 10-9 m E = 4.96 x 10-19J per photon Energy of photon determines #photons/watt Red laser More photons per W at longer wavelength Red laser • Laser power is 3 mW at 650 nm • # photons/s = Power energy per photon = 0.003 W 3.0x10-19J/photon = 9.8 x 1015 photons / s 5. Natural light sources • Lots of variation in natural light Light at high noon Light at dawn, dusk Light at midnight Light in forest Light at ocean surface Light 100 m depth • Illuminant shapes what we can see Light environment : sky conditions Light environment : sky conditions Light environment : sky conditions Environment : Lighting conditions Light environment : Viewing angle Light environment : time of day Light environment : Time of day Solar spectrum 1.2 Irradiance in watts / m2 Relative intensity 1.0 0.8 0.6 0.4 0.2 0.0 300 400 500 600 700 Wavelength (nm) 800 900 1000 Light spectrum in terms of photon flux Since there are more photons per watt at longer wavelengths, the curve shape changes when presented as photons / m2 sec Loew and McFarland 1990 Compare spectra of sunlight and moonlight Why are they similar? Why are they different? Loew and McFarland 1990 Light from sun versus moon Moon Sun Earth How does solar spectrum vary for high noon vs dawn / dusk Sun angle changes with time of day This changes pathlength through atmosphere Dawn / dusk Lose mid to long wavelengths at dawn and dusk Loew and McFarland 1990 Fleishman et al. 1997 Here are light spectra (irradiance) for forest habitats Shade Terrestrial habitats Fleishman et al. 1997 Shade Sun Terrestrial habitats Why is light in the forest different?Absorption of light by chlorophylls Light reflecting off vegetation Fleishman et al. 1997 Shade Sun Terrestrial habitats Fleishman et al. 1997 Shade Sun Terrestrial habitats Affects of the terrestrial environment • Lighting and contrast with background determines how easily you can be seen Cryptic (camouflage) - blend in Conspicuous - stand out • Lighting and contrast with background determines how easily your food can be detected Light under water • Water attenuates certain wavelengths more than others I = I 0 exp(-a l l) – attenuation coefficient varies with wavelength Why does α vary with wavelength? A) Water reflection depends on wavelength B) Water refraction depends on wavelength C) Water absorption depends on wavelength D) None of the above Attenuation coefficient of pure water 1 0.8 K (m-1) 0.6 0.4 Which wavelength light is transmitted best? A) 350 nm B) 450 nm C) 550 nm D) 650 nm 0.2 0 300 400 500 Wavelength 600 700 Light transmission of clear water m How can we calculate the light spectrum underwater? • We take the light spectrum at the waters surface and • Multiply it by the fraction of light that is transmitted Solar illumination at different depths Incident sunlight m Light penetration “Blue” oceanic waters Levine Sci Am 1982 400 450 500 550 600 650 700 nm Light penetration “Blue” oceanic waters Levine Sci Am 1982 400 450 500 550 600 650 700 nm Light penetration “Blue” oceanic waters Levine Sci Am 1982 400 450 500 550 600 650 700 nm Light at dawn / dusk in air or under water Loew and McFarland 1990 Note photons/s not Watts Decrease in light intensity with depth 1 Relative light intensity 0.9 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0 0 50 100 150 Depth 200 250 Decrease in light intensity with depth - log scale 1 0.1 0 200 400 600 0.01 Relative light intensity 0.001 0.0001 1E-05 1E-06 1E-07 1E-08 1E-09 1E-10 1E-11 Limit of human sensitivity 1E-12 1E-13 1E-14 Depth 800 1000 Land & Nilsson Table 2.1 Color of transmitted light “Blue” oceanic waters Levine Sci Am 1982 400 450 500 550 600 650 700 nm Color of water Light penetration Rivers and lakes can vary in water clarity Different waters attenuate differently 1+2 open ocean 3 ocean with chlorophyll 4 coastal waters with chlorophyll and dissolved organics “Fresh” water “Green” river water Swampy “red” waters Which curve describes light attenuation in Green River? 4 3 2 1 Aquatic environment • • • • • Depth Habitat (coral reef vs ocean) Camouflage - blending in Light levels (especially in deep ocean) Kind of water that you’re in How light is transmitted / attenuated FishBase: Fish at depth viewer Amphiprion ocellaris Amphiprion at depth 0m 10 m 25 m 50 m