Revising and Validating Spectral Irradiance Reference Standards for Photovoltaic
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Guide for the Use of the International System of Units (SI)
Guide for the Use of the International System of Units (SI) m kg s cd SI mol K A NIST Special Publication 811 2008 Edition Ambler Thompson and Barry N. Taylor NIST Special Publication 811 2008 Edition Guide for the Use of the International System of Units (SI) Ambler Thompson Technology Services and Barry N. Taylor Physics Laboratory National Institute of Standards and Technology Gaithersburg, MD 20899 (Supersedes NIST Special Publication 811, 1995 Edition, April 1995) March 2008 U.S. Department of Commerce Carlos M. Gutierrez, Secretary National Institute of Standards and Technology James M. Turner, Acting Director National Institute of Standards and Technology Special Publication 811, 2008 Edition (Supersedes NIST Special Publication 811, April 1995 Edition) Natl. Inst. Stand. Technol. Spec. Publ. 811, 2008 Ed., 85 pages (March 2008; 2nd printing November 2008) CODEN: NSPUE3 Note on 2nd printing: This 2nd printing dated November 2008 of NIST SP811 corrects a number of minor typographical errors present in the 1st printing dated March 2008. Guide for the Use of the International System of Units (SI) Preface The International System of Units, universally abbreviated SI (from the French Le Système International d’Unités), is the modern metric system of measurement. Long the dominant measurement system used in science, the SI is becoming the dominant measurement system used in international commerce. The Omnibus Trade and Competitiveness Act of August 1988 [Public Law (PL) 100-418] changed the name of the National Bureau of Standards (NBS) to the National Institute of Standards and Technology (NIST) and gave to NIST the added task of helping U.S. -
Extraction of Incident Irradiance from LWIR Hyperspectral Imagery Pierre Lahaie, DRDC Valcartier 2459 De La Bravoure Road, Quebec, Qc, Canada
DRDC-RDDC-2015-P140 Extraction of incident irradiance from LWIR hyperspectral imagery Pierre Lahaie, DRDC Valcartier 2459 De la Bravoure Road, Quebec, Qc, Canada ABSTRACT The atmospheric correction of thermal hyperspectral imagery can be separated in two distinct processes: Atmospheric Compensation (AC) and Temperature and Emissivity separation (TES). TES requires for input at each pixel, the ground leaving radiance and the atmospheric downwelling irradiance, which are the outputs of the AC process. The extraction from imagery of the downwelling irradiance requires assumptions about some of the pixels’ nature, the sensor and the atmosphere. Another difficulty is that, often the sensor’s spectral response is not well characterized. To deal with this unknown, we defined a spectral mean operator that is used to filter the ground leaving radiance and a computation of the downwelling irradiance from MODTRAN. A user will select a number of pixels in the image for which the emissivity is assumed to be known. The emissivity of these pixels is assumed to be smooth and that the only spectrally fast varying variable in the downwelling irradiance. Using these assumptions we built an algorithm to estimate the downwelling irradiance. The algorithm is used on all the selected pixels. The estimated irradiance is the average on the spectral channels of the resulting computation. The algorithm performs well in simulation and results are shown for errors in the assumed emissivity and for errors in the atmospheric profiles. The sensor noise influences mainly the required number of pixels. Keywords: Hyperspectral imagery, atmospheric correction, temperature emissivity separation 1. INTRODUCTION The atmospheric correction of thermal hyperspectral imagery aims at extracting the temperature and the emissivity of the material imaged by a sensor in the long wave infrared (LWIR) spectral band. -
Solar Radiation
SOLAR CELLS Chapter 2. Solar Radiation Chapter 2. SOLAR RADIATION 2.1 Solar radiation One of the basic processes behind the photovoltaic effect, on which the operation of solar cells is based, is generation of the electron-hole pairs due to absorption of visible or other electromagnetic radiation by a semiconductor material. Today we accept that electromagnetic radiation can be described in terms of waves, which are characterized by wavelength ( λ ) and frequency (ν ), or in terms of discrete particles, photons, which are characterized by energy ( hν ) expressed in electron volts. The following formulas show the relations between these quantities: ν = c λ (2.1) 1 hc hν = (2.2) q λ In Eqs. 2.1 and 2.2 c is the speed of light in vacuum (2.998 × 108 m/s), h is Planck’s constant (6.625 × 10-34 Js), and q is the elementary charge (1.602 × 10-19 C). For example, a green light can be characterized by having a wavelength of 0.55 × 10-6 m, frequency of 5.45 × 1014 s-1 and energy of 2.25 eV. - 2.1 - SOLAR CELLS Chapter 2. Solar Radiation Only photons of appropriate energy can be absorbed and generate the electron-hole pairs in the semiconductor material. Therefore, it is important to know the spectral distribution of the solar radiation, i.e. the number of photons of a particular energy as a function of wavelength. Two quantities are used to describe the solar radiation spectrum, namely the spectral power density, P(λ), and the photon flux density, Φ(λ) . -
Solar Constant
ME 432 Fundamentals of Modern Photovoltaics Discussion 2: A Nuclear Fusion Power Plant 9.3(107) Miles Away 26 August 2020 The Sun • Sun’s core: Fusion reaction - the conversion of H to He, T=20,000,000 K • Sun’s surface: Photosphere T=5800K • All life and power on earth comes to us from the sun http://www.solcomhouse.com/thesun.htm (photosynthesis, fossil fuels) Today’s Objectives • Estimate the power density and peak wavelength emitted by a black body at a given temp T • Derive the solar constant and the average solar irradiation at the earth’s surface • Describe 4 ways to directly capture the energy of the sun on earth • List some advantages & challenges for the widescale adoption of solar photovoltaics • Describe the main solar photovoltaic technologies available today, and their relative merits/shortcomings Today’s Objectives • Estimate the power density and peak wavelength emitted by a black body at a given temp T • Derive the solar constant and the average solar irradiation at the earth’s surface • Describe 4 ways to directly capture the energy of the sun on earth • List some advantages & challenges for the widescale adoption of solar photovoltaics • Describe the main solar photovoltaic technologies available today, and their relative merits/shortcomings Planck’s Law of Blackbody Radiation • Hot bodies emit electromagnetic radiation with a spectral distribution that is determined by the temperature • For a “black body”, which is an idealization of a perfect absorber, the spectral distribution is given by Planck’s Law of Blackbody Radiation • As a black body is heated, the total emitted radiation increases and the wavelength of the peak emission decreases • The sun is a very good approximation of a black body at temperature T=5800K hc 1240 (eV-nm) Useful relationship: E = hυ = E (eV) = λ λ (nm) Planck’s Law of Blackbody Radiation • The expression for the unique electromagnetic spectrum that is emitted by a perfect blackbody. -
Radiometric and Photometric Measurements with TAOS Photosensors Contributed by Todd Bishop March 12, 2007 Valid
TAOS Inc. is now ams AG The technical content of this TAOS application note is still valid. Contact information: Headquarters: ams AG Tobelbaderstrasse 30 8141 Unterpremstaetten, Austria Tel: +43 (0) 3136 500 0 e-Mail: [email protected] Please visit our website at www.ams.com NUMBER 21 INTELLIGENT OPTO SENSOR DESIGNER’S NOTEBOOK Radiometric and Photometric Measurements with TAOS PhotoSensors contributed by Todd Bishop March 12, 2007 valid ABSTRACT Light Sensing applications use two measurement systems; Radiometric and Photometric. Radiometric measurements deal with light as a power level, while Photometric measurements deal with light as it is interpreted by the human eye. Both systems of measurement have units that are parallel to each other, but are useful for different applications. This paper will discuss the differencesstill and how they can be measured. AG RADIOMETRIC QUANTITIES Radiometry is the measurement of electromagnetic energy in the range of wavelengths between ~10nm and ~1mm. These regions are commonly called the ultraviolet, the visible and the infrared. Radiometry deals with light (radiant energy) in terms of optical power. Key quantities from a light detection point of view are radiant energy, radiant flux and irradiance. SI Radiometryams Units Quantity Symbol SI unit Abbr. Notes Radiant energy Q joule contentJ energy radiant energy per Radiant flux Φ watt W unit time watt per power incident on a Irradiance E square meter W·m−2 surface Energy is an SI derived unit measured in joules (J). The recommended symbol for energy is Q. Power (radiant flux) is another SI derived unit. It is the derivative of energy with respect to time, dQ/dt, and the unit is the watt (W). -
Radiometry and Photometry
Radiometry and Photometry Wei-Chih Wang Department of Power Mechanical Engineering National TsingHua University W. Wang Materials Covered • Radiometry - Radiant Flux - Radiant Intensity - Irradiance - Radiance • Photometry - luminous Flux - luminous Intensity - Illuminance - luminance Conversion from radiometric and photometric W. Wang Radiometry Radiometry is the detection and measurement of light waves in the optical portion of the electromagnetic spectrum which is further divided into ultraviolet, visible, and infrared light. Example of a typical radiometer 3 W. Wang Photometry All light measurement is considered radiometry with photometry being a special subset of radiometry weighted for a typical human eye response. Example of a typical photometer 4 W. Wang Human Eyes Figure shows a schematic illustration of the human eye (Encyclopedia Britannica, 1994). The inside of the eyeball is clad by the retina, which is the light-sensitive part of the eye. The illustration also shows the fovea, a cone-rich central region of the retina which affords the high acuteness of central vision. Figure also shows the cell structure of the retina including the light-sensitive rod cells and cone cells. Also shown are the ganglion cells and nerve fibers that transmit the visual information to the brain. Rod cells are more abundant and more light sensitive than cone cells. Rods are 5 sensitive over the entire visible spectrum. W. Wang There are three types of cone cells, namely cone cells sensitive in the red, green, and blue spectral range. The approximate spectral sensitivity functions of the rods and three types or cones are shown in the figure above 6 W. Wang Eye sensitivity function The conversion between radiometric and photometric units is provided by the luminous efficiency function or eye sensitivity function, V(λ). -
The Nature of Light I
PHYS 320 Lecture 3 The Nature of Light I Jiong Qiu Wenda Cao MSU Physics Department NJIT Physics Department Courtesy: Prof. Jiong Qiu 9/22/15 Outline q How fast does light travel? How can this speed be measured? q How is the light from an ordinary light bulb different from the light emitted by a neon sign? q How can astronomers measure the temperatures of the Sun and stars? q How can astronomers tell what distant celestial objects are made of? q How can we tell if a celestial object is approaching us or receding from us? Light travels with a very high speed q Galileo first tried but failed to measure the speed of light . He concluded that the speed of light is very high. q In 1675, Roemer first proved that light does not travel instantaneously from his observations of the eclipses of Jupiter’s moons. q Modern technologies are able to find the speed of light; in an empty space: c = 3.00 x 108 m/s one of the most important numbers in modern physical sciences! Ex.1: The distance between the Sun and the Earth is 1AU (= 1.5x1011m). (a) how long does it take the light to travel from the Sun to an observer on the Earth? (b) A concord airplane has a speed of 600 m/ s; how long does it take a traveler on a Concord airplane to travel from the Earth to the Sun? Ex.2: A lunar laser ranging retro-reflector array was planted on the Moon on July 21, 1969, by the crew of the Apollo 11. -
Measuring the Solar Constant
SOLAR PHYSICS AND TERRESTRIAL EFFECTS 2+ Activity 3 4= Activity 3 Measuring the Solar Constant Purpose With this activity, we will let solar radiation raise the temperature of a measured quantity of water. From the observation of how much time is required for the temperature change, we can calculate the amount of energy absorbed by the water and then relate this to the energy output of the Sun. Materials Simple Jar and Thermometer small, flat sided glass bottle with 200 ml capacity—the more regular the shape the easier it will be to calculate the surface area later cork stopper for the bottle with a hole drilled in it to accept a thermometer; the regular cap of the bottle can be used, but the hole for the thermometer may have to be sealed with silicon or caulking after the thermometer is placed in it. _ thermometer with a range up to at least 50 C stopwatch black, water soluble ink metric measuring cup Option: Insulated Collector Jar and Digital Multi-Meter (DMM) Temperature Probes all of the above but substitute the temperature probes from a DMM or a computer to col- lect the data; the computer could also provide a more accurate time base a more sophisticated, insulated collector bottle could be made—try to minimize heat loss to the environment with your design. substitute different materials other than water as the solar collection material. Ethylene glycol (antifreeze) might be used, or even a photovoltaic cell could act as a collector. Re- member, some of the parameters in your calculations will need to be changed if water is not used different colors of water soluble ink Procedures 1. -
Sunlight and Seasons
Project ATMOSPHERE This guide is one of a series produced by Project ATMOSPHERE, an initiative of the American Meteorological Society. Project ATMOSPHERE has created and trained a network of resource agents who provide nationwide leadership in precollege atmospheric environment education. To support these agents in their teacher training, Project ATMOSPHERE develops and produces teacher’s guides and other educational materials. For further information, and additional background on the American Meteorological Society’s Education Program, please contact: American Meteorological Society Education Program 1200 New York Ave., NW, Ste. 500 Washington, DC 20005-3928 www.ametsoc.org/amsedu This material is based upon work initially supported by the National Science Foundation under Grant No. TPE-9340055. Any opinions, findings, and conclusions or recommendations expressed in this publication are those of the authors and do not necessarily reflect the views of the National Science Foundation. © 2012 American Meteorological Society (Permission is hereby granted for the reproduction of materials contained in this publication for non-commercial use in schools on the condition their source is acknowledged.) 2 Foreword This guide has been prepared to introduce fundamental understandings about the guide topic. This guide is organized as follows: Introduction This is a narrative summary of background information to introduce the topic. Basic Understandings Basic understandings are statements of principles, concepts, and information. The basic understandings represent material to be mastered by the learner, and can be especially helpful in devising learning activities in writing learning objectives and test items. They are numbered so they can be keyed with activities, objectives and test items. Activities These are related investigations. -
Measuring the Solar Constant
MEASURING THE SOLAR CONSTANT In this experiment, you will make a device to measure how much energy sunlight provides to Earth. Materials Per group: Procedures: ▼ 1 small, flat-sided 1. Prepare the collector bottle by pouring 150 ml of water into the glass bottle with at least 150 ml capacity bottle. Add a few drops of the ink to make it black, and place the ▼ 1 cork stopper for the thermometer through the hole in the cork or lid. Make sure the seal bottle is as tight as possible by using caulk or masking tape, if necessary. ▼ 1 thermometer with a You may need to drill a hole into the cork or metal top of the lid. range up to at least Insert the cork/lid into the bottle with the thermometer in place and 50˚C sealed (see Figure S1). ▼ Books or rocks (to prop up bottle) 2. Place the collector in shade so that it stabilizes to the mean air Per class: temperature. This takes about 10 minutes or until the temperature ▼ Stopwatch does not change any more while checking every 2-3 minutes. ▼ Black, water-soluble ink 3. Move the collector to sunlight. Make sure the unit is shaded ▼ Metric measuring cup while moving. Set the collector down so that the flat surface is as ▼ Optional: Drill perpendicular to the incoming sunlight as possible. You may need ▼ Optional: Caulk to prop up bottle with books or rocks (see Figure S1). ▼ Optional: Masking tape WARNING Do not look directly at the Sun! Looking for even a few seconds can cause permanent damage to the eyes! Note that sunglasses do not provide an adequate safeguard against looking directly at the Sun. -
Solar Constant
Extraterrestrial Life: Lecture #6 Liquid water is important because: What are the requirements for the Earth (or another planet) • solvent for organic molecules to be habitable? • allows transport of chemicals within cells • involved in many biologically important • liquid water on surface chemical reactions • atmosphere • plate tectonics / volcanism Other solvents (ammonia, methane etc) exist in liquid • magnetic field form on planets but are much less promising for life • … Normal atmospheric pressure: liquid water requires: 0o C (273K) < T < 100o C (373K) …require planets with surface temperatures in this range ! Extraterrestrial Life: Spring 2008 Extraterrestrial Life: Spring 2008 What determines the Earth’s surface temperature? Solar constant The flux of energy is the amount of energy that passes fraction of 2 incident radiation through unit area (1 m ) in one second is reflected Measured in units of watts / m2 incident Solar Solar flux declines with distance as 1 / d2: radiation L flux = remainder is 2 absorbed by 4"d the Earth and then reradiated …where d is the Sun - planet distance and L is the total If the Earth is not heating up or cooling down, the total luminosity of the Sun (watts) of incoming and outgoing radiation must balance ! Are there other sources of energy for a planet? Extraterrestrial Life: Spring 2008 Extraterrestrial Life: Spring 2008 Solar constant The fraction of the incident flux that is reflected is called Solar luminosity is 3.9 x 1026 watts the albedo of the planet: 0 < A < 1 The fraction that is absorbed is -
Basic Principles of Imaging and Photometry Lecture #2
Basic Principles of Imaging and Photometry Lecture #2 Thanks to Shree Nayar, Ravi Ramamoorthi, Pat Hanrahan Computer Vision: Building Machines that See Lighting Camera Physical Models Computer Scene Scene Interpretation We need to understand the Geometric and Radiometric relations between the scene and its image. A Brief History of Images 1558 Camera Obscura, Gemma Frisius, 1558 A Brief History of Images 1558 1568 Lens Based Camera Obscura, 1568 A Brief History of Images 1558 1568 1837 Still Life, Louis Jaques Mande Daguerre, 1837 A Brief History of Images 1558 1568 1837 Silicon Image Detector, 1970 1970 A Brief History of Images 1558 1568 1837 Digital Cameras 1970 1995 Geometric Optics and Image Formation TOPICS TO BE COVERED : 1) Pinhole and Perspective Projection 2) Image Formation using Lenses 3) Lens related issues Pinhole and the Perspective Projection Is an image being formed (x,y) on the screen? YES! But, not a “clear” one. screen scene image plane r =(x, y, z) y optical effective focal length, f’ z axis pinhole x r'=(x', y', f ') r' r x' x y' y = = = f ' z f ' z f ' z Magnification A(x, y, z) B y d B(x +δx, y +δy, z) optical f’ z A axis Pinhole A’ d’ x planar scene image plane B’ A'(x', y', f ') B'(x'+δx', y'+δy', f ') From perspective projection: Magnification: x' x y' y d' (δx')2 + (δy')2 f ' = = m = = = f ' z f ' z d (δx)2 + (δy)2 z x'+δx' x +δx y'+δy' y +δy = = Area f ' z f ' z image = m2 Areascene Orthographic Projection Magnification: x' = m x y' = m y When m = 1, we have orthographic projection r =(x, y, z) r'=(x', y', f ') y optical z axis x z ∆ image plane z This is possible only when z >> ∆z In other words, the range of scene depths is assumed to be much smaller than the average scene depth.