NIST MEASUREMENT SERVICES: Regular Spectral Transmittance
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Glossary Physics (I-Introduction)
1 Glossary Physics (I-introduction) - Efficiency: The percent of the work put into a machine that is converted into useful work output; = work done / energy used [-]. = eta In machines: The work output of any machine cannot exceed the work input (<=100%); in an ideal machine, where no energy is transformed into heat: work(input) = work(output), =100%. Energy: The property of a system that enables it to do work. Conservation o. E.: Energy cannot be created or destroyed; it may be transformed from one form into another, but the total amount of energy never changes. Equilibrium: The state of an object when not acted upon by a net force or net torque; an object in equilibrium may be at rest or moving at uniform velocity - not accelerating. Mechanical E.: The state of an object or system of objects for which any impressed forces cancels to zero and no acceleration occurs. Dynamic E.: Object is moving without experiencing acceleration. Static E.: Object is at rest.F Force: The influence that can cause an object to be accelerated or retarded; is always in the direction of the net force, hence a vector quantity; the four elementary forces are: Electromagnetic F.: Is an attraction or repulsion G, gravit. const.6.672E-11[Nm2/kg2] between electric charges: d, distance [m] 2 2 2 2 F = 1/(40) (q1q2/d ) [(CC/m )(Nm /C )] = [N] m,M, mass [kg] Gravitational F.: Is a mutual attraction between all masses: q, charge [As] [C] 2 2 2 2 F = GmM/d [Nm /kg kg 1/m ] = [N] 0, dielectric constant Strong F.: (nuclear force) Acts within the nuclei of atoms: 8.854E-12 [C2/Nm2] [F/m] 2 2 2 2 2 F = 1/(40) (e /d ) [(CC/m )(Nm /C )] = [N] , 3.14 [-] Weak F.: Manifests itself in special reactions among elementary e, 1.60210 E-19 [As] [C] particles, such as the reaction that occur in radioactive decay. -
Light and Illumination
ChapterChapter 3333 -- LightLight andand IlluminationIllumination AAA PowerPointPowerPointPowerPoint PresentationPresentationPresentation bybyby PaulPaulPaul E.E.E. Tippens,Tippens,Tippens, ProfessorProfessorProfessor ofofof PhysicsPhysicsPhysics SouthernSouthernSouthern PolytechnicPolytechnicPolytechnic StateStateState UniversityUniversityUniversity © 2007 Objectives:Objectives: AfterAfter completingcompleting thisthis module,module, youyou shouldshould bebe ableable to:to: •• DefineDefine lightlight,, discussdiscuss itsits properties,properties, andand givegive thethe rangerange ofof wavelengthswavelengths forfor visiblevisible spectrum.spectrum. •• ApplyApply thethe relationshiprelationship betweenbetween frequenciesfrequencies andand wavelengthswavelengths forfor opticaloptical waves.waves. •• DefineDefine andand applyapply thethe conceptsconcepts ofof luminousluminous fluxflux,, luminousluminous intensityintensity,, andand illuminationillumination.. •• SolveSolve problemsproblems similarsimilar toto thosethose presentedpresented inin thisthis module.module. AA BeginningBeginning DefinitionDefinition AllAll objectsobjects areare emittingemitting andand absorbingabsorbing EMEM radiaradia-- tiontion.. ConsiderConsider aa pokerpoker placedplaced inin aa fire.fire. AsAs heatingheating occurs,occurs, thethe 1 emittedemitted EMEM waveswaves havehave 2 higherhigher energyenergy andand 3 eventuallyeventually becomebecome visible.visible. 4 FirstFirst redred .. .. .. thenthen white.white. LightLightLight maymaymay bebebe defineddefineddefined -
TIE-35: Transmittance of Optical Glass
DATE October 2005 . PAGE 1/12 TIE-35: Transmittance of optical glass 0. Introduction Optical glasses are optimized to provide excellent transmittance throughout the total visible range from 400 to 800 nm. Usually the transmittance range spreads also into the near UV and IR regions. As a general trend lowest refractive index glasses show high transmittance far down to short wavelengths in the UV. Going to higher index glasses the UV absorption edge moves closer to the visible range. For highest index glass and larger thickness the absorption edge already reaches into the visible range. This UV-edge shift with increasing refractive index is explained by the general theory of absorbing dielectric media. So it may not be overcome in general. However, due to improved melting technology high refractive index glasses are offered nowadays with better blue-violet transmittance than in the past. And for special applications where best transmittance is required SCHOTT offers improved quality grades like for SF57 the grade SF57 HHT. The aim of this technical information is to give the optical designer a deeper understanding on the transmittance properties of optical glass. 1. Theoretical background A light beam with the intensity I0 falls onto a glass plate having a thickness d (figure 1-1). At the entrance surface part of the beam is reflected. Therefore after that the intensity of the beam is Ii0=I0(1-r) with r being the reflectivity. Inside the glass the light beam is attenuated according to the exponential function. At the exit surface the beam intensity is I i = I i0 exp(-kd) [1.1] where k is the absorption constant. -
Reflectance and Transmittance Sphere
Reflectance and Transmittance Sphere Spectral Evolution four inch portable reflectance/ transmittance sphere is ideal for measuring vegetation physiological states SPECTRAL EVOLUTION offers a portable, compact four inch reflectance/transmittance (R/T) integrating sphere for measuring the reflectance and transmittance of vegetation. The 4 inch R/T sphere is lightweight and portable so you can take it into the field for in situ meas- urements, delivered with a stand as well as a ¼-20 mount for use with tripods. When used with a SPECTRAL EVOLUTION spectrometer or spectroradiometer such as the PSR+, RS-3500, RS- 5400, SR-6500 or RS-8800, it delivers detailed information for measurements of transmittance and reflectance modes. Two varying light intensity levels (High and Low) allow for a broader range of samples to be measured. Light reflected or transmitted from a sample in a sphere is integrated over a full hemisphere, with measurements insensitive to sample anisotropic directional reflectance (transmittance). This provides repeatable measurements of a variety of samples. The 4 inch portable R/T sphere can be used in vegetation studies such as, deriving absorbance characteristics, and estimating the leaf area index (LAI) from radiation reflected from a canopy surface. The sphere allows researchers to limit destructive sampling and provides timely data acquisition of key material samples. The R/T sphere allows you to collect all diffuse light reflected from a sample – measuring total hemispherical reflectance. You can measure reflectance and transmittance, and calculate absorption. You can select the bulb inten- sity level that suits your sample. A white reference is provided for both reflectance and transmittance measurements. -
Black Body Radiation and Radiometric Parameters
Black Body Radiation and Radiometric Parameters: All materials absorb and emit radiation to some extent. A blackbody is an idealization of how materials emit and absorb radiation. It can be used as a reference for real source properties. An ideal blackbody absorbs all incident radiation and does not reflect. This is true at all wavelengths and angles of incidence. Thermodynamic principals dictates that the BB must also radiate at all ’s and angles. The basic properties of a BB can be summarized as: 1. Perfect absorber/emitter at all ’s and angles of emission/incidence. Cavity BB 2. The total radiant energy emitted is only a function of the BB temperature. 3. Emits the maximum possible radiant energy from a body at a given temperature. 4. The BB radiation field does not depend on the shape of the cavity. The radiation field must be homogeneous and isotropic. T If the radiation going from a BB of one shape to another (both at the same T) were different it would cause a cooling or heating of one or the other cavity. This would violate the 1st Law of Thermodynamics. T T A B Radiometric Parameters: 1. Solid Angle dA d r 2 where dA is the surface area of a segment of a sphere surrounding a point. r d A r is the distance from the point on the source to the sphere. The solid angle looks like a cone with a spherical cap. z r d r r sind y r sin x An element of area of a sphere 2 dA rsin d d Therefore dd sin d The full solid angle surrounding a point source is: 2 dd sind 00 2cos 0 4 Or integrating to other angles < : 21cos The unit of solid angle is steradian. -
A) Single-Beam
Lecture 2 Spectrophotometer Spectrophotometry is the basis for many of the instruments used in clinical chemistry. The primary reasons for this are ease of measurement, satisfactory accuracy and precision, and the suitability of spectrophotometric techniques to use in automated instruments. Spectrophotometer measures light absorption by a liquid substance at various wavelengths. The Components of unknown material can be determined, or the concentration of a number of known substances can be measured. Types of Spectrophotometer Ultraviolet (UV) Spectrophotometers. Uses ultraviolet light of wave lengths from 200 nm to 350 nm. light) of wave lengths from 350 nm to 700 nm. Spectrophotometer Block Diagram a) Single-beam b) Double-beam Most common Spectrophotometer 1. Photodiode 2. Connection wire 3. Lamp 4. Filter/Detector 5. On/Off switch and zero transmission adjustment knob 6. Wavelength selector/Readout 7. Sample chamber 8. Transmittance/absorbance control 9. Absorbance/Transmittance scale 1. Light Sources Tungsten lamp: Vis. near IR (320 nm~2500 nm) Deuterium arc lamp: UV (200~400 nm) Uses a tungsten filament and anode placed on opposite sides of a nickel box structure designed to produce the best output spectrum. Unlike tungsten lamps, the filament is not the source of light in deuterium lamps. Instead an arc is created from the filament to the anode. The arc created excites the molecular deuterium contained within the bulb to a higher energy state. The deuterium then emits light as it transitions back to its initial state Its continuous spectrum is only from 180 nm to 370 nm. Light Intensity of Tungsten and Deuterium lamps A problem with tungsten lamps is that, during operation, the tungsten progressively vaporizes from the filaments and condenses on the glass envelope. -
Multidisciplinary Design Project Engineering Dictionary Version 0.0.2
Multidisciplinary Design Project Engineering Dictionary Version 0.0.2 February 15, 2006 . DRAFT Cambridge-MIT Institute Multidisciplinary Design Project This Dictionary/Glossary of Engineering terms has been compiled to compliment the work developed as part of the Multi-disciplinary Design Project (MDP), which is a programme to develop teaching material and kits to aid the running of mechtronics projects in Universities and Schools. The project is being carried out with support from the Cambridge-MIT Institute undergraduate teaching programe. For more information about the project please visit the MDP website at http://www-mdp.eng.cam.ac.uk or contact Dr. Peter Long Prof. Alex Slocum Cambridge University Engineering Department Massachusetts Institute of Technology Trumpington Street, 77 Massachusetts Ave. Cambridge. Cambridge MA 02139-4307 CB2 1PZ. USA e-mail: [email protected] e-mail: [email protected] tel: +44 (0) 1223 332779 tel: +1 617 253 0012 For information about the CMI initiative please see Cambridge-MIT Institute website :- http://www.cambridge-mit.org CMI CMI, University of Cambridge Massachusetts Institute of Technology 10 Miller’s Yard, 77 Massachusetts Ave. Mill Lane, Cambridge MA 02139-4307 Cambridge. CB2 1RQ. USA tel: +44 (0) 1223 327207 tel. +1 617 253 7732 fax: +44 (0) 1223 765891 fax. +1 617 258 8539 . DRAFT 2 CMI-MDP Programme 1 Introduction This dictionary/glossary has not been developed as a definative work but as a useful reference book for engi- neering students to search when looking for the meaning of a word/phrase. It has been compiled from a number of existing glossaries together with a number of local additions. -
STHF-R Ultra High Flux Gamma Probe Data Sheet
Features STHF-R™ Ultra High ■ Measurement of H*(10) Flux Gamma Probe ambient gamma dose equivalent rate up to 1000 Sv/h (100 000 R/h) Description ■ To be connected to The STHF-R ultra high flux Radiagem™, MIP 10 Digital™ probe is designed for the or Avior ® meters measurements of very high ■ Waterproof: 80 m (262.5 ft) gamma dose-equivalent rates water depth up to 1000 Sv/h. ■ Detector: Silicon diode This probe is especially ■ 5 kSv maximum integrated designed for ultra high flux dose measurement which can be found in pools in nuclear ■ Compact portable design for power plants or in recycling detector and detector cable facilities. Effectively this on reel probes box is stainless steel based and waterproof up to 80 m (164 ft) underwater. It can be laid underwater in the storage pools Borated water. An optional ballast weight can be supplied to ease underwater measurements. The STHF-R probe is composed of two matched units: ■ The measurement probe including the silicon diode and the associated analog electronics. ■ An interface case which houses the processing electronics that are more sensitive to radiation; this module can be remotely located up to 50 m (164 ft) from the measurement spot. ■ An intermediate connection point with 50 m length cable to which the interface case can be connected. The STHF-R probe can be connected directly to Avior, Radiagem or MIP 10 Digital meters. The STHF-R unit receives power from the survey meter during operation. STHF-R instruments include key components of hardware circuitry (high voltage power supply, amplifier, discriminator, etc.). -
UV-VIS Nomenclature and Units
IN804 Info Note 804: UV-VIS Nomenclature and Units Ultraviolet-visible spectroscopy or ultraviolet-visible spectrophotometry (UV/VIS) involves the spectroscopy of photons in the UV-visible region. It uses light in the visible and adjacent near ultraviolet (UV) and near infrared (NIR) ranges. In this region of the electromagnetic spectrum, molecules undergo electronic transitions. This technique is complementary to fluorescence spectroscopy, in that fluorescence deals with transitions from the excited state to the ground state, while absorption measures transitions from the ground state to the excited state. UV/VIS is based on absorbance. In spectroscopy, the absorbance A is defined as: (1) where I is the intensity of light at a specified wavelength λ that has passed through a sample (transmitted light intensity) and I is the intensity of the light before it enters the sample or 0 incident light intensity. Absorbance measurements are often carried out in analytical chemistry, since the absorbance of a sample is proportional to the thickness of the sample and the concentration of the absorbing species in the sample, in contrast to the transmittance I / I of a 0 s ample, which varies exponentially with thickness and concentration. The Beer-Lambert law is used for concentration determination. The term absorption refers to the physical process of absorbing light, while absorbance refers to the mathematical quantity. Also, absorbance does not always measure absorption: if a given sample is, for example, a dispersion, part of the incident light will in fact be scattered by the dispersed particles, and not really absorbed. Absorbance only contemplates the ratio of transmitted light over incident light, not the mechanism by which light intensity decreases. -
Beer-Lambert Law: Measuring Percent Transmittance of Solutions at Different Concentrations (Teacher’S Guide)
TM DataHub Beer-Lambert Law: Measuring Percent Transmittance of Solutions at Different Concentrations (Teacher’s Guide) © 2012 WARD’S Science. v.11/12 For technical assistance, All Rights Reserved call WARD’S at 1-800-962-2660 OVERVIEW Students will study the relationship between transmittance, absorbance, and concentration of one type of solution using the Beer-Lambert law. They will determine the concentration of an “unknown” sample using mathematical tools for graphical analysis. MATERIALS NEEDED Ward’s DataHub USB connector cable* Cuvette for the colorimeter Distilled water 6 - 250 mL beakers Instant coffee Paper towel Wash bottle Stir Rod Balance * – The USB connector cable is not needed if you are using a Bluetooth enabled device. NUMBER OF USES This demonstration can be performed repeatedly. © 2012 WARD’S Science. v.11/12 1 For technical assistance, All Rights Reserved Teacher’s Guide – Beer-Lambert Law call WARD’S at 1-800-962-2660 FRAMEWORK FOR K-12 SCIENCE EDUCATION © 2012 * The Dimension I practices listed below are called out as bold words throughout the activity. Asking questions (for science) and defining Use mathematics and computational thinking problems (for engineering) Constructing explanations (for science) and designing Developing and using models solutions (for engineering) Practices Planning and carrying out investigations Engaging in argument from evidence Dimension 1 Analyzing and interpreting data Obtaining, evaluating, and communicating information Science and Engineering Science and Engineering Patterns -
LFC-050-LE Light Flux Color and Luminous Efficacy Measurement Systems Why Choose Lightfluxcolor
LFC-050-LE Light Flux Color and Luminous Efficacy Measurement Systems Why Choose LightFluxColor • Calibrations are traceable to NIST (USA) which are accepted and recognized globally. Ideal For Flux, Color & AC/DC The most economical and • Calibrated lamp standards NVLAP Electrical Characterization of: reliable solution for photometry accreditation Lab Code 200951-0 of light source needs! Automotive Lamps Traffic Lighting (ISO 17025) LED Clusters Architectural Lighting • Spectral flux standards (calibration LightFluxColor-LE Series Systems are the performed at each wavelength) are LED Bulbs Railway Lighting most affordable and reliable systems for testing supplied with each system for highest LED lighting products. Whether you are a possible accuracy. manufacturer of LED luminaires, street lights, • Single software controls all electronics and solar powered LED lanterns, LED bulbs, LightFluxColor-LE Series Systems also include provides optical and electrical data. or any other type of LED lighting product, a highly sensitive mini-calibrated CCD Array Spectrometer with spectral range from LightFluxColor Systems will meet all your testing • Competitive systems only provide 250 to 850 nm. This low noise and broad spectral requirements. LightFluxColor Systems allow luminous flux standards with CCT luminaire manufacturers to test LED products response spectrometer provide instantaneous calibration which limits overall for photometric performance. measurement of radiometric, photometric, and system accuracy. color characteristics of the LED sources. • AC/DC operation in one packaged LightFluxColor-LE Series Systems allow testing system users to test AC/DC characterization of lamps The fast results from the spectrometer helps at various input frequencies along with lumens to increase the rate of product development, • An auxiliary lamp is provided for and color parameters. -
Radiometry of Light Emitting Diodes Table of Contents
TECHNICAL GUIDE THE RADIOMETRY OF LIGHT EMITTING DIODES TABLE OF CONTENTS 1.0 Introduction . .1 2.0 What is an LED? . .1 2.1 Device Physics and Package Design . .1 2.2 Electrical Properties . .3 2.2.1 Operation at Constant Current . .3 2.2.2 Modulated or Multiplexed Operation . .3 2.2.3 Single-Shot Operation . .3 3.0 Optical Characteristics of LEDs . .3 3.1 Spectral Properties of Light Emitting Diodes . .3 3.2 Comparison of Photometers and Spectroradiometers . .5 3.3 Color and Dominant Wavelength . .6 3.4 Influence of Temperature on Radiation . .6 4.0 Radiometric and Photopic Measurements . .7 4.1 Luminous and Radiant Intensity . .7 4.2 CIE 127 . .9 4.3 Spatial Distribution Characteristics . .10 4.4 Luminous Flux and Radiant Flux . .11 5.0 Terminology . .12 5.1 Radiometric Quantities . .12 5.2 Photometric Quantities . .12 6.0 References . .13 1.0 INTRODUCTION Almost everyone is familiar with light-emitting diodes (LEDs) from their use as indicator lights and numeric displays on consumer electronic devices. The low output and lack of color options of LEDs limited the technology to these uses for some time. New LED materials and improved production processes have produced bright LEDs in colors throughout the visible spectrum, including white light. With efficacies greater than incandescent (and approaching that of fluorescent lamps) along with their durability, small size, and light weight, LEDs are finding their way into many new applications within the lighting community. These new applications have placed increasingly stringent demands on the optical characterization of LEDs, which serves as the fundamental baseline for product quality and product design.