Studies of a Diffraction Grating, Spectral Lines of Hydrogen, and Solar Spectrum
|
|
- Stephany Sharp
- 7 years ago
- Views:
Transcription
1 Studies of a Diffraction Grating, Spectral Lines of Hydrogen, and Solar Spectrum Objectives: 1. To become familiar with capturing spectral lines using a CCD camera. 2. To study selected properties of a diffraction grating. 3. To study the Balmer series of hydrogen. 4. To resolve the red spectral lines of hydrogen and deuterium. 5. To observe the absorption lines sodium, and calcium in the solar spectrum. Apparatus: Hydrogen lamp, deuterium lamp, sodium lamp, slide projector (as a white light source), beam splitter, He-Ne laser ( λ = 632.8nm ), variable slit, convex lenses (f =10 cm, 12 cm and 25 cm), prism, diffraction grating (~1000 lines/mm), monochromator, CCD camera, PC, black cardboard boxes. Part 1 Studies of a diffraction grating Introduction (Reference: Hecht, Optics) The key component of a monochromator a grating or two or even three gratings. When you look at the specification of a grating, you often see Blazed at xxx nm. Here, we briefly describe this important type of gratings. The reason for using a blazed grating design is to concentrate optical energy at a certain order. For common gratings the grooves looks like so that optical energy will, after reflecting from the grating, distribute more or less evenly among several orders, which is certainly undesirable. A blazed grating is used inside a high-end monochromator, shown in the diagrams below: γ γ mth order b a θ i γ θ r Specular b 2γ =θ r 2γ =θ r Normal to plane of grating Fig. 1-1(a) Section of a blazed grating. 1 Fig. 1-1(b) Condition for desired order.
2 Such an objective is achieved for specular reflection, i. e. θ i = 0; θ r = -2γ asin(-2γ) = mλ ; γ is the blaze angle, m is the desired order. The convention is that θ r is negative if θ i and θ r are on the same side of the normal to the plane of grating. Procedures: 1-1. Use the slide projector to form a beam an essentially plane wave of white light to incident on a blazed grating. Use the digital camera provided to record the images of the diffraction patterns (projected on a white screen) at several incident angles Analysis of the diffraction pattern obtained. Part 2 Spectral lines of hydrogen Background: Balmer examined the four visible lines in the spectrum of the hydrogen atom. Their wavelengths are 410 nm, 434 nm, 486 nm, and 656 nm. He played around with these numbers and eventually figured out that all four wavelengths λ fit into the equation R( ) 2 2 λ = 2 n, where R is the Rydberg constant (value m -1 ). This set of lines is called the Balmer series. Later, other researchers found that the series could be extended into ultraviolet wavelengths. The same formula still works, with larger values of n. From Balmer s equation, it is clear when n gets larger, the lines are getting closer together. The accepted values of the Balmer series (in air) are listed below: Table 1 Balmer Series Balmer Series (blue and violet regions) Wavelength (nm) Relative Intensity n Color or region UV UV UV Violet Violet Violet Blue 2
3 Experiment setup: Hydrogen Lamp f=12cm f=25cm Beam splitter slit prism f=10cm CCD He-Ne laser ( λ = 632.8nm ) PC Fig. 2-1 Experimental setup. Procedures: 2-1. Set up the experiment as shown in Fig Align the optical components till the light from the hydrogen lamp and the laser beam go through the same light path. It is easier to align the system by observing the laser beam path (Another use of the laser beam is as a wavelength reference). Also make sure that the prism is at the minimum deviation and the light spot is well focused on the CCD chip Observe the spectra lines on the PC screen and find the hydrogen lines listed in Table 1 by using the laser spot as a reference Carefully adjust the distance of the CCD and the lens until the first two lines (i.e and/or nm) are best focused. Record the image by using a proper exposure time (to see the faint spectral lines at shorter wavelength a large enough exposure time ~20 second or more is needed) and save the image Repeat 2-4 until the last few lines are focused well and record another image. Note: In order to record good images and the faint spectral lines (e.g nm) of hydrogen, a black card box is needed to block stray light, so that large enough exposure time, say 20 second or larger can be used. Requirements and Information for data analysis: 1. It is well known that refractive index of dielectric material, such as glass, is a function of wavelength, which is given, to a good approximation, by, Cauchy equation n A B λ 2 g = + /, where n g is the refractive index, both A and B are constant for a given substance and λ is the wavelength. From this equation, with relative small difference of wavelength, there will be a slightly larger separation of the spectra lines in the shorter wavelength region because of larger dispersion. Actually, this was observed in the experimental results. a) Assume that the angular position of the spectra line is proportional to its n value (in fact, a good approximation). Because n= Kθ and θ d, where d is the position of spectral lines, 3
4 the relationship of d and λ is then: md A B λ 2 = + /, where m is an integer. Let m = 1, Assume that two spectral line are exactly equal to their accepted values and use Cauchy s equation to obtain A and B and thus the values of the other spectral lines. Part 3 The red spectral lines of hydrogen and deuterium Background: The basic grating equation is sinα + sinθ = mnλ, whereα is the angle between the incident light and the normal to the grating, θ is the angle between the diffracted light and the normal to the grating, m is the order number and n is the number of grooves per millimeter. When a parallel beam of polychromatic light is incident on a grating then the light is dispersed so that each wavelength satisfies the grating equation. As a result, blazing grating is often used to analyze atomic spectral lines. The energies of corresponding levels in hydrogen and deuterium differ by approximately 0.25 % because of the different reduced masses of these two atoms. Precise measurements of Balmer emission spectra for these atoms suggested that the red lines of hydrogen and deuterium are at nm and nm, respectively. In this experiment, the spectral lines of hydrogen and deuterium will be observed and their two red spectral lines will be recorded and analyzed. Experimental setup: White Screen Hydrogen lamp Slit ~13m Blazing grating Beam splitter Deuterium lamp He-Ne laser (for alignment) Lens (f= 50cm) CCD camera PC Fig Experimental setup. Procedures: 3-1. Set up the experiment as shown in Fig Align the components till the reflected light from the white screen and the laser beam passes through the same optical path. It is easier to align the system by observing the laser beam path Adjust the position of the CCD camera such that the laser spot can be clearly seen on the PC screen. Then slightly move the CCD camera toward or away from the lens so that the laser spot was well focused on the CCD screen Block off the laser beam and unblock the two spectral lamps First identify, roughly, the position of the hydrogen and deuterium read lines by bare eye by looking into the lens Put the CCD to the place identified by eyes where red spectral lines can be observed. Carefully adjust the distance of the CCD and the lens until the two red lines from the two lamps 4
5 are best focused. Record the image by using a proper exposure time (~800 ms or more if needed). Block the light from the slit and record another image as the background. Requirements: Image of the two red spectral lines. Estimated FWHM of the spectral lines. Estimated spectral resolution of the system. Part 4 Studies of the solar spectrum Background: The solar spectrum is a continuum spectrum with thousands of dark absorption lines superposed on it. These lines are called the Fraunhofer lines, and the solar spectrum is sometimes called the Fraunhofer spectrum. These lines are produced primarily in the photosphere of the sun. And the following table is a list of the most prominent Fraunhofer lines. Table 2. A list of the most prominent Fraunhofer lines Lines Due To Wavelengths (nm) A - (band) O B - (band) O C H 6563 a - (band) O D - 1, 2 Na 5896 & 5890 E Fe 5270 b - 1, 2 Mg 5184 & 5173 c Fe 4958 F H 4861 d Fe 4668 e Fe 4384 f H 4340 G Fe & Ca 4308 g Ca 4227 h H 4102 H Ca 3968 K Ca 3934 In this part of the experiment, part of the solar spectrum that contains the D-1, 2, (and possibly calcium line near nm, and the hydrogen line near nm) Fraunhofer lines will be recorded. Note: in an emission spectrum, this pair of intense yellow lines (wavelengths of and nm) is the most significant feature of the sodium spectrum. 5
6 Experimental setup: Sunlight White screen Monochromator ~15cm Entrance slit L1, F=15cm ~10cm Sodium lamp Exit ~27cm L2, F=10 cm ~16cm PC CCD camera Fig. 4-1 Experimental setup. Procedures: 4-1. Set up the experiment as shown in Fig Align the system to make sure that: (a) The sunlight as well as the sodium lamp properly light the white screen put near the window. (b) The incident light of the monochromator is normal to the entrance slit so that the incident light can be cast on the concave mirror in the monochromator properly. (c) Use a black card box to block the stray light so that long exposure time can be used Turn on the sodium lamp and use a large slit (~1 mm) first so that it is easy to align L1, L2 and the CCD. Adjust the monochromator to the wavelength of ~595 nm and then slightly move the CCD closer (or further) to the lens till sharp sodium lines (the double lines of and nm) appear on the computer screen Adjust the entrance slit to about 0.1 mm and use an appropriate exposure time so that sharp sodium lines appear on the computer screen without over exposed Block the sodium lamp and increase the exposure to about 20 s, record the image when two sharp dark lines at the same positions of those of the double sodium lines can be seen on the computer screen (Proc. 4-4). Requirements: Image of the sodium absorption lines. Fraunhofer spectrum of the region that you have recorded (light intensity versus wavelength). You abundance of elements (that is larger than %) on the surface of the sun is listed in the Appendix. Try to reconstruct the Fraunhofer lines near the spectral region(s) that you have recorded. (Use the information available on the Web site: 6
7 Appendix 1 Data Processing -- Extracting the Spectra You have to use the PC connected to LAN in Rm 115) A1-1. A1-2. Use Photoshop to open the data file (in JPEG format) to be analysed. If the Raman lines are not exactly vertical, rotate the image such that they are. A1-3. Click the icon once and then point the mouse to the picture to select, say, ~200 lines of pixels. A1-4. Invoke File and then select New. A1-5. Invoke Edit and then Paste the selected portion to this new file. A1-6. Save this new file with a name that you like (say yyyy) with an extension.raw. A1-7. Minimize Photoshop and then double click the icon Labview. A1-8. Several choices should appear on the screen. Select Open Vi and then select Programs and then Main and eventually Convert.vi A1-9. When Convert.vi is running, you can click the Load button once and load the file yyyy.raw. Then signal averaging will be carried out with a spectrum appear on the PC monitor. A1-10. Click the save button to save the result in ASCII format with an extension.dat Appendix 2 UV105 and UV107 Exposure Time Control Function Keys F1 through F8 are used to select or modify exposure times F1 <shift> F1 F5 <shift> F5 F6 <shift> F6 F7 <shift> F7 F8 sets the exposure time to the default exposure time of 100 milliseconds. prompts the user to enter a new exposure time in milliseconds. increments the present exposure time by 1 second. decrements the present exposure time by 1 second. increments the present exposure time by 0.1 second. decrements the present exposure time by 0.1 second. increments the present exposure time by 0.01 second. decrements the present exposure time by 0.01 second. increments the present exposure time by 1 millisecond. 7
8 <shift> F8 decrements the present exposure time by 1 millisecond. Appendix 3 UV105 and UV107 Single Key-Stroke Commands Commands which control camera operation (a)nti-blooming (i)nterlace (l)ive camera image Toggles anti-blooming mode off for highest dynamic range, and on for blooming reduction and lower dark current. Available only when image is live. Toggles interlace mode on and off (available only when image is live ). Two separate image frames are required for each interlaced image. Toggles live camera image mode on and off. Utility Commands (b)ias (h)elp (p)cx (q)uit (t)iff Displays a numerical indication of image brightness. Three numbers are displayed: the minimum brightness level, the mode of the brightness levels, and maximum brightness level. Displays help screens. Saves current image as a PCX file. The user is prompted for the name of the PCX file to be created. Terminates UV105 or UV107. Saves current images as a TIFF (Tag Image File Format) file. The user is prompted for the name of the TIFF file to be created. 8
9 Appendix 4 Element Atomic Abundance (%) Element Atomic Abundance (%) Number Number 9
ATOMIC SPECTRA. Apparatus: Optical spectrometer, spectral tubes, power supply, incandescent lamp, bottles of dyed water, elevating jack or block.
1 ATOMIC SPECTRA Objective: To measure the wavelengths of visible light emitted by atomic hydrogen and verify the measured wavelengths against those predicted by quantum theory. To identify an unknown
More informationWAVELENGTH OF LIGHT - DIFFRACTION GRATING
PURPOSE In this experiment we will use the diffraction grating and the spectrometer to measure wavelengths in the mercury spectrum. THEORY A diffraction grating is essentially a series of parallel equidistant
More informationO6: The Diffraction Grating Spectrometer
2B30: PRACTICAL ASTROPHYSICS FORMAL REPORT: O6: The Diffraction Grating Spectrometer Adam Hill Lab partner: G. Evans Tutor: Dr. Peter Storey 1 Abstract The calibration of a diffraction grating spectrometer
More informationGRID AND PRISM SPECTROMETERS
FYSA230/2 GRID AND PRISM SPECTROMETERS 1. Introduction Electromagnetic radiation (e.g. visible light) experiences reflection, refraction, interference and diffraction phenomena when entering and passing
More informationAP Physics B Ch. 23 and Ch. 24 Geometric Optics and Wave Nature of Light
AP Physics B Ch. 23 and Ch. 24 Geometric Optics and Wave Nature of Light Name: Period: Date: MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) Reflection,
More informationProcedure: Geometrical Optics. Theory Refer to your Lab Manual, pages 291 294. Equipment Needed
Theory Refer to your Lab Manual, pages 291 294. Geometrical Optics Equipment Needed Light Source Ray Table and Base Three-surface Mirror Convex Lens Ruler Optics Bench Cylindrical Lens Concave Lens Rhombus
More informationTHE BOHR QUANTUM MODEL
THE BOHR QUANTUM MODEL INTRODUCTION When light from a low-pressure gas is subject to an electric discharge, a discrete line spectrum is emitted. When light from such a low-pressure gas is examined with
More information6) How wide must a narrow slit be if the first diffraction minimum occurs at ±12 with laser light of 633 nm?
Test IV Name 1) In a single slit diffraction experiment, the width of the slit is 3.1 10-5 m and the distance from the slit to the screen is 2.2 m. If the beam of light of wavelength 600 nm passes through
More informationInterference. Physics 102 Workshop #3. General Instructions
Interference Physics 102 Workshop #3 Name: Lab Partner(s): Instructor: Time of Workshop: General Instructions Workshop exercises are to be carried out in groups of three. One report per group is due by
More information1051-232 Imaging Systems Laboratory II. Laboratory 4: Basic Lens Design in OSLO April 2 & 4, 2002
05-232 Imaging Systems Laboratory II Laboratory 4: Basic Lens Design in OSLO April 2 & 4, 2002 Abstract: For designing the optics of an imaging system, one of the main types of tools used today is optical
More information1 Laboratory #5: Grating Spectrometer
SIMG-215-20061: LABORATORY #5 1 Laboratory #5: Grating Spectrometer 1.1 Objective: To observe and measure the spectra of different light sources. 1.2 Materials: 1. OSA optics kit. 2. Nikon digital camera
More informationStudy Guide for Exam on Light
Name: Class: Date: Study Guide for Exam on Light Multiple Choice Identify the choice that best completes the statement or answers the question. 1. Which portion of the electromagnetic spectrum is used
More informationExperiment #12: The Bohr Atom. Equipment: Spectroscope Hydrogen and Helium Gas Discharge Tubes, Holder, and Variac Flashlight
Experiment #12: The Bohr Atom Purpose: To observe the visible spectrum of hydrogen and helium and verify the Bohr model of the hydrogen atom. Equipment: Spectroscope Hydrogen and Helium Gas Discharge Tubes,
More informationP R E A M B L E. Facilitated workshop problems for class discussion (1.5 hours)
INSURANCE SCAM OPTICS - LABORATORY INVESTIGATION P R E A M B L E The original form of the problem is an Experimental Group Research Project, undertaken by students organised into small groups working as
More informationTheremino System Theremino Spectrometer Technology
Theremino System Theremino Spectrometer Technology theremino System - Theremino Spectrometer Technology - August 15, 2014 - Page 1 Operation principles By placing a digital camera with a diffraction grating
More informationLaboratory #3 Guide: Optical and Electrical Properties of Transparent Conductors -- September 23, 2014
Laboratory #3 Guide: Optical and Electrical Properties of Transparent Conductors -- September 23, 2014 Introduction Following our previous lab exercises, you now have the skills and understanding to control
More informationPhysical Science Study Guide Unit 7 Wave properties and behaviors, electromagnetic spectrum, Doppler Effect
Objectives: PS-7.1 Physical Science Study Guide Unit 7 Wave properties and behaviors, electromagnetic spectrum, Doppler Effect Illustrate ways that the energy of waves is transferred by interaction with
More informationHow To Understand Light And Color
PRACTICE EXAM IV P202 SPRING 2004 1. In two separate double slit experiments, an interference pattern is observed on a screen. In the first experiment, violet light (λ = 754 nm) is used and a second-order
More informationBasic Optics System OS-8515C
40 50 30 60 20 70 10 80 0 90 80 10 20 70 T 30 60 40 50 50 40 60 30 C 70 20 80 10 90 90 0 80 10 70 20 60 50 40 30 Instruction Manual with Experiment Guide and Teachers Notes 012-09900B Basic Optics System
More informationChapter 17: Light and Image Formation
Chapter 17: Light and Image Formation 1. When light enters a medium with a higher index of refraction it is A. absorbed. B. bent away from the normal. C. bent towards from the normal. D. continues in the
More informationILLUSTRATIVE EXAMPLE: Given: A = 3 and B = 4 if we now want the value of C=? C = 3 + 4 = 9 + 16 = 25 or 2
Forensic Spectral Anaylysis: Warm up! The study of triangles has been done since ancient times. Many of the early discoveries about triangles are still used today. We will only be concerned with the "right
More informationAtoms Absorb & Emit Light
Atoms Absorb & Emit Light Spectra The wavelength of the light that an element emits or absorbs is its fingerprint. Atoms emit and absorb light First Test is Thurs, Feb 1 st About 30 multiple choice questions
More informationLight as a Wave. The Nature of Light. EM Radiation Spectrum. EM Radiation Spectrum. Electromagnetic Radiation
The Nature of Light Light and other forms of radiation carry information to us from distance astronomical objects Visible light is a subset of a huge spectrum of electromagnetic radiation Maxwell pioneered
More information- the. or may. scales on. Butterfly wing. magnified about 75 times.
Lecture Notes (Applications of Diffraction) Intro: - the iridescent colors seen in many beetles is due to diffraction of light rays hitting the small groovess of its exoskeleton - these ridges are only
More informationDiffraction of Laser Light
Diffraction of Laser Light No Prelab Introduction The laser is a unique light source because its light is coherent and monochromatic. Coherent light is made up of waves, which are all in phase. Monochromatic
More informationSolution Derivations for Capa #14
Solution Derivations for Capa #4 ) An image of the moon is focused onto a screen using a converging lens of focal length (f = 34.8 cm). The diameter of the moon is 3.48 0 6 m, and its mean distance from
More informationBlackbody Radiation References INTRODUCTION
Blackbody Radiation References 1) R.A. Serway, R.J. Beichner: Physics for Scientists and Engineers with Modern Physics, 5 th Edition, Vol. 2, Ch.40, Saunders College Publishing (A Division of Harcourt
More informationFrom lowest energy to highest energy, which of the following correctly orders the different categories of electromagnetic radiation?
From lowest energy to highest energy, which of the following correctly orders the different categories of electromagnetic radiation? From lowest energy to highest energy, which of the following correctly
More informationPHYS 222 Spring 2012 Final Exam. Closed books, notes, etc. No electronic device except a calculator.
PHYS 222 Spring 2012 Final Exam Closed books, notes, etc. No electronic device except a calculator. NAME: (all questions with equal weight) 1. If the distance between two point charges is tripled, the
More informationwaves rays Consider rays of light from an object being reflected by a plane mirror (the rays are diverging): mirror object
PHYS1000 Optics 1 Optics Light and its interaction with lenses and mirrors. We assume that we can ignore the wave properties of light. waves rays We represent the light as rays, and ignore diffraction.
More informationLab 9: The Acousto-Optic Effect
Lab 9: The Acousto-Optic Effect Incoming Laser Beam Travelling Acoustic Wave (longitudinal wave) O A 1st order diffracted laser beam A 1 Introduction qb d O 2qb rarefractions compressions Refer to Appendix
More informationEfficiency, Dispersion and Straylight Performance Tests of Immersed Gratings for High Resolution Spectroscopy in the Near Infra-red
Changing the economics of space Efficiency, Dispersion and Straylight Performance Tests of Immersed Gratings for High Resolution Spectroscopy in the Near Infra-red J. Fernandez-Saldivar 1, F. Culfaz 1,
More informationEXPERIMENT 11 UV/VIS Spectroscopy and Spectrophotometry: Spectrophotometric Analysis of Potassium Permanganate Solutions.
EXPERIMENT 11 UV/VIS Spectroscopy and Spectrophotometry: Spectrophotometric Analysis of Potassium Permanganate Solutions. Outcomes After completing this experiment, the student should be able to: 1. Prepare
More information9/16 Optics 1 /11 GEOMETRIC OPTICS
9/6 Optics / GEOMETRIC OPTICS PURPOSE: To review the basics of geometric optics and to observe the function of some simple and compound optical devices. APPARATUS: Optical bench, lenses, mirror, target
More informationAcousto-optic modulator
1 of 3 Acousto-optic modulator F An acousto-optic modulator (AOM), also called a Bragg cell, uses the acousto-optic effect to diffract and shift the frequency of light using sound waves (usually at radio-frequency).
More informationLight and its effects
Light and its effects Light and the speed of light Shadows Shadow films Pinhole camera (1) Pinhole camera (2) Reflection of light Image in a plane mirror An image in a plane mirror is: (i) the same size
More informationC) D) As object AB is moved from its present position toward the left, the size of the image produced A) decreases B) increases C) remains the same
1. For a plane mirror, compared to the object distance, the image distance is always A) less B) greater C) the same 2. Which graph best represents the relationship between image distance (di) and object
More informationLIGHT SECTION 6-REFRACTION-BENDING LIGHT From Hands on Science by Linda Poore, 2003.
LIGHT SECTION 6-REFRACTION-BENDING LIGHT From Hands on Science by Linda Poore, 2003. STANDARDS: Students know an object is seen when light traveling from an object enters our eye. Students will differentiate
More informationUsing the Spectrophotometer
Using the Spectrophotometer Introduction In this exercise, you will learn the basic principals of spectrophotometry and and serial dilution and their practical application. You will need these skills to
More informationReflection and Refraction
Equipment Reflection and Refraction Acrylic block set, plane-concave-convex universal mirror, cork board, cork board stand, pins, flashlight, protractor, ruler, mirror worksheet, rectangular block worksheet,
More informationProblem Set 6 UV-Vis Absorption Spectroscopy. 13-1. Express the following absorbances in terms of percent transmittance:
Problem Set 6 UV-Vis Absorption Spectroscopy 13-1. Express the following absorbances in terms of percent transmittance: a 0.051 b 0.918 c 0.379 d 0.261 e 0.485 f 0.072 A = log P o /P = log1/t = - log T
More informationDiffraction of a Circular Aperture
Diffraction of a Circular Aperture Diffraction can be understood by considering the wave nature of light. Huygen's principle, illustrated in the image below, states that each point on a propagating wavefront
More informationRevision problem. Chapter 18 problem 37 page 612. Suppose you point a pinhole camera at a 15m tall tree that is 75m away.
Revision problem Chapter 18 problem 37 page 612 Suppose you point a pinhole camera at a 15m tall tree that is 75m away. 1 Optical Instruments Thin lens equation Refractive power Cameras The human eye Combining
More informationChemistry 111 Lab: Intro to Spectrophotometry Page E-1
Chemistry 111 Lab: Intro to Spectrophotometry Page E-1 SPECTROPHOTOMETRY Absorption Measurements & their Application to Quantitative Analysis study of the interaction of light (or other electromagnetic
More informationPhysics 10. Lecture 29A. "There are two ways of spreading light: to be the candle or the mirror that reflects it." --Edith Wharton
Physics 10 Lecture 29A "There are two ways of spreading light: to be the candle or the mirror that reflects it." --Edith Wharton Converging Lenses What if we wanted to use refraction to converge parallel
More informationSSO Transmission Grating Spectrograph (TGS) User s Guide
SSO Transmission Grating Spectrograph (TGS) User s Guide The Rigel TGS User s Guide available online explains how a transmission grating spectrograph (TGS) works and how efficient they are. Please refer
More informationRealization of a UV fisheye hyperspectral camera
Realization of a UV fisheye hyperspectral camera Valentina Caricato, Andrea Egidi, Marco Pisani and Massimo Zucco, INRIM Outline Purpose of the instrument Required specs Hyperspectral technique Optical
More informationUV/VIS/IR SPECTROSCOPY ANALYSIS OF NANOPARTICLES
UV/VIS/IR SPECTROSCOPY ANALYSIS OF NANOPARTICLES SEPTEMBER 2012, V 1.1 4878 RONSON CT STE K SAN DIEGO, CA 92111 858-565 - 4227 NANOCOMPOSIX.COM Note to the Reader: We at nanocomposix have published this
More informationReview of the isotope effect in the hydrogen spectrum
Review of the isotope effect in the hydrogen spectrum 1 Balmer and Rydberg Formulas By the middle of the 19th century it was well established that atoms emitted light at discrete wavelengths. This is in
More informationAutomatic and Objective Measurement of Residual Stress and Cord in Glass
Automatic and Objective Measurement of Residual Stress and Cord in Glass GlassTrend - ICG TC15/21 Seminar SENSORS AND PROCESS CONTROL 13-14 October 2015, Eindhoven Henning Katte, ilis gmbh copyright ilis
More informationGeometric Optics Converging Lenses and Mirrors Physics Lab IV
Objective Geometric Optics Converging Lenses and Mirrors Physics Lab IV In this set of lab exercises, the basic properties geometric optics concerning converging lenses and mirrors will be explored. The
More informationExperiment #5: Qualitative Absorption Spectroscopy
Experiment #5: Qualitative Absorption Spectroscopy One of the most important areas in the field of analytical chemistry is that of spectroscopy. In general terms, spectroscopy deals with the interactions
More informationEXPERIMENT 6 OPTICS: FOCAL LENGTH OF A LENS
EXPERIMENT 6 OPTICS: FOCAL LENGTH OF A LENS The following website should be accessed before coming to class. Text reference: pp189-196 Optics Bench a) For convenience of discussion we assume that the light
More informationSpectroscopy. Biogeochemical Methods OCN 633. Rebecca Briggs
Spectroscopy Biogeochemical Methods OCN 633 Rebecca Briggs Definitions of Spectrometry Defined by the method used to prepare the sample 1. Optical spectrometry Elements are converted to gaseous atoms or
More informationEXPERIMENT O-6. Michelson Interferometer. Abstract. References. Pre-Lab
EXPERIMENT O-6 Michelson Interferometer Abstract A Michelson interferometer, constructed by the student, is used to measure the wavelength of He-Ne laser light and the index of refraction of a flat transparent
More informationSTAAR Science Tutorial 30 TEK 8.8C: Electromagnetic Waves
Name: Teacher: Pd. Date: STAAR Science Tutorial 30 TEK 8.8C: Electromagnetic Waves TEK 8.8C: Explore how different wavelengths of the electromagnetic spectrum such as light and radio waves are used to
More informationMCAL Spectrophotometry. Spectrophotometry
MCAL Spectrophotometry Instruments include: Cary 50 UV-vis Spectrophotometer Eclipse Spectrofluorometer HPLC Diode Array and Fluorescence ICP-OES with CCD detection Spectrophotometry The instruments all
More information12.1 What is Refraction pg. 515. Light travels in straight lines through air. What happens to light when it travels from one material into another?
12.1 What is Refraction pg. 515 Light travels in straight lines through air. What happens to light when it travels from one material into another? Bending Light The light traveling from an object in water
More informationSpectrophotometry and the Beer-Lambert Law: An Important Analytical Technique in Chemistry
Spectrophotometry and the Beer-Lambert Law: An Important Analytical Technique in Chemistry Jon H. Hardesty, PhD and Bassam Attili, PhD Collin College Department of Chemistry Introduction: In the last lab
More informationRodenstock Photo Optics
Rogonar Rogonar-S Rodagon Apo-Rodagon N Rodagon-WA Apo-Rodagon-D Accessories: Modular-Focus Lenses for Enlarging, CCD Photos and Video To reproduce analog photographs as pictures on paper requires two
More informationA concise guide to Safety Glasses, the different standards and the effects of light on the eye. Contents. Links. Year of publication: 2010
A concise guide to Safety Glasses, the different standards and the effects of light on the eye Year of publication: 2010 Produced by the leading supplier of Safety Glasses in the UK. All Rights Reserved.
More informationScanners and How to Use Them
Written by Jonathan Sachs Copyright 1996-1999 Digital Light & Color Introduction A scanner is a device that converts images to a digital file you can use with your computer. There are many different types
More informationIntroduction to microstructure
Introduction to microstructure 1.1 What is microstructure? When describing the structure of a material, we make a clear distinction between its crystal structure and its microstructure. The term crystal
More informationTHE NATURE OF LIGHT AND COLOR
THE NATURE OF LIGHT AND COLOR THE PHYSICS OF LIGHT Electromagnetic radiation travels through space as electric energy and magnetic energy. At times the energy acts like a wave and at other times it acts
More information2) A convex lens is known as a diverging lens and a concave lens is known as a converging lens. Answer: FALSE Diff: 1 Var: 1 Page Ref: Sec.
Physics for Scientists and Engineers, 4e (Giancoli) Chapter 33 Lenses and Optical Instruments 33.1 Conceptual Questions 1) State how to draw the three rays for finding the image position due to a thin
More informationClassroom Exercise ASTR 390 Selected Topics in Astronomy: Astrobiology A Hertzsprung-Russell Potpourri
Classroom Exercise ASTR 390 Selected Topics in Astronomy: Astrobiology A Hertzsprung-Russell Potpourri Purpose: 1) To understand the H-R Diagram; 2) To understand how the H-R Diagram can be used to follow
More informationUsing light scattering method to find The surface tension of water
Experiment (8) Using light scattering method to find The surface tension of water The aim of work: The goals of this experiment are to confirm the relationship between angular frequency and wave vector
More informationPHYSICS PAPER 1 (THEORY)
PHYSICS PAPER 1 (THEORY) (Three hours) (Candidates are allowed additional 15 minutes for only reading the paper. They must NOT start writing during this time.) ---------------------------------------------------------------------------------------------------------------------
More information2 Spectrophotometry and the Analysis of Riboflavin
2 Spectrophotometry and the Analysis of Riboflavin Objectives: A) To become familiar with operating the Platereader; B) to learn how to use the Platereader in determining the absorption spectrum of a compound
More informationRAY OPTICS II 7.1 INTRODUCTION
7 RAY OPTICS II 7.1 INTRODUCTION This chapter presents a discussion of more complicated issues in ray optics that builds on and extends the ideas presented in the last chapter (which you must read first!)
More informationFig.1. The DAWN spacecraft
Introduction Optical calibration of the DAWN framing cameras G. Abraham,G. Kovacs, B. Nagy Department of Mechatronics, Optics and Engineering Informatics Budapest University of Technology and Economics
More informationScience In Action 8 Unit C - Light and Optical Systems. 1.1 The Challenge of light
1.1 The Challenge of light 1. Pythagoras' thoughts about light were proven wrong because it was impossible to see A. the light beams B. dark objects C. in the dark D. shiny objects 2. Sir Isaac Newton
More informationLBS-300 Beam Sampler for C-mount Cameras. YAG Focal Spot Analysis Adapter. User Notes
LBS-300 Beam Sampler for C-mount Cameras P/N SP90183, SP90184, SP90185 and SP90186 YAG Focal Spot Analysis Adapter P/N SP90187, SP90188, SP90189, SP90190, SP90191 User Notes Ophir-Spiricon Inc. 60 West
More informationImproved predictive modeling of white LEDs with accurate luminescence simulation and practical inputs
Improved predictive modeling of white LEDs with accurate luminescence simulation and practical inputs TracePro Opto-Mechanical Design Software s Fluorescence Property Utility TracePro s Fluorescence Property
More informationPhysics 116. Nov 4, 2011. Session 22 Review: ray optics. R. J. Wilkes Email: ph116@u.washington.edu
Physics 116 Session 22 Review: ray optics Nov 4, 2011 R. J. Wilkes Email: ph116@u.washington.edu ! Exam 2 is Monday!! All multiple choice, similar to HW problems, same format as Exam 1!!! Announcements
More informationConvex Mirrors. Ray Diagram for Convex Mirror
Convex Mirrors Center of curvature and focal point both located behind mirror The image for a convex mirror is always virtual and upright compared to the object A convex mirror will reflect a set of parallel
More informationPhysics 441/2: Transmission Electron Microscope
Physics 441/2: Transmission Electron Microscope Introduction In this experiment we will explore the use of transmission electron microscopy (TEM) to take us into the world of ultrasmall structures. This
More informationHarmonic oscillations of spiral springs Springs linked in parallel and in series
.3.26 Related topics Spring constant, Hooke s Law, oscillations, limit of elasticity, parallel springs, serial springs, use of an interface. Principle and task The spring constant D is determined for different
More informationCOOKBOOK. for. Aristarchos Transient Spectrometer (ATS)
NATIONAL OBSERVATORY OF ATHENS Institute for Astronomy, Astrophysics, Space Applications and Remote Sensing HELMOS OBSERVATORY COOKBOOK for Aristarchos Transient Spectrometer (ATS) P. Boumis, J. Meaburn,
More informationTS-E24mm f/3.5l TS-E45mm f/2.8 TS-E90mm f/2.8 Instructions
TS-E24mm f/3.5l TS-E45mm f/2.8 TS-E90mm f/2.8 ENG Instructions Thank you for purchasing a Canon product. Canon s TS-E lenses are tilt-shift lenses designed for EOS cameras. The tilt-shift mechanism enables
More informationUser guide for Cary 5000 absorption spectrometer with external DRA 1800 attachment.
User guide for Cary 5000 absorption spectrometer with external DRA 1800 attachment. (last updated 03/17/2016) This guide is for use of the Cary 5000 with the DRA only. For use without the DRA as a standard
More informationSpectroscopy Using the Tracker Video Analysis Program
Spectroscopy Using the Tracker Video Analysis Program Douglas Brown Cabrillo College Aptos CA 95003 dobrown@cabrillo.edu Spectroscopy has important applications in many fields and deserves more attention
More informationExperiment 5. Lasers and laser mode structure
Northeastern University, PHYS5318 Spring 2014, 1 1. Introduction Experiment 5. Lasers and laser mode structure The laser is a very important optical tool that has found widespread use in science and industry,
More informationRefraction of Light at a Plane Surface. Object: To study the refraction of light from water into air, at a plane surface.
Refraction of Light at a Plane Surface Object: To study the refraction of light from water into air, at a plane surface. Apparatus: Refraction tank, 6.3 V power supply. Theory: The travel of light waves
More informationFTIR Instrumentation
FTIR Instrumentation Adopted from the FTIR lab instruction by H.-N. Hsieh, New Jersey Institute of Technology: http://www-ec.njit.edu/~hsieh/ene669/ftir.html 1. IR Instrumentation Two types of instrumentation
More informationChapter 6 Telescopes: Portals of Discovery. How does your eye form an image? Refraction. Example: Refraction at Sunset.
Chapter 6 Telescopes: Portals of Discovery 6.1 Eyes and Cameras: Everyday Light Sensors Our goals for learning:! How does your eye form an image?! How do we record images? How does your eye form an image?
More informationAtomic Structure: Chapter Problems
Atomic Structure: Chapter Problems Bohr Model Class Work 1. Describe the nuclear model of the atom. 2. Explain the problems with the nuclear model of the atom. 3. According to Niels Bohr, what does n stand
More informationTHE COMPOUND MICROSCOPE
THE COMPOUND MICROSCOPE In microbiology, the microscope plays an important role in allowing us to see tiny objects that are normally invisible to the naked eye. It is essential for students to learn how
More informationWaves Sound and Light
Waves Sound and Light r2 c:\files\courses\1710\spr12\wavetrans.doc Ron Robertson The Nature of Waves Waves are a type of energy transmission that results from a periodic disturbance (vibration). They are
More information1 of 9 2/9/2010 3:38 PM
1 of 9 2/9/2010 3:38 PM Chapter 23 Homework Due: 8:00am on Monday, February 8, 2010 Note: To understand how points are awarded, read your instructor's Grading Policy. [Return to Standard Assignment View]
More informationWhat s in the Mix? Liquid Color Spectroscopy Lab (Randy Landsberg & Bill Fisher)
What s in the Mix? Liquid Color Spectroscopy Lab (Randy Landsberg & Bill Fisher) Introduction: There is more to a color than a name. Color can tell us lots of information. In this lab you will use a spectrophotometer
More informationReview Vocabulary spectrum: a range of values or properties
Standards 7.3.19: Explain that human eyes respond to a narrow range of wavelengths of the electromagnetic spectrum. 7.3.20: Describe that something can be seen when light waves emitted or reflected by
More informationSynthetic Sensing: Proximity / Distance Sensors
Synthetic Sensing: Proximity / Distance Sensors MediaRobotics Lab, February 2010 Proximity detection is dependent on the object of interest. One size does not fit all For non-contact distance measurement,
More informationCONFOCAL LASER SCANNING MICROSCOPY TUTORIAL
CONFOCAL LASER SCANNING MICROSCOPY TUTORIAL Robert Bagnell 2006 This tutorial covers the following CLSM topics: 1) What is the optical principal behind CLSM? 2) What is the spatial resolution in X, Y,
More informationAlpy 600 User Guide. Olivier Thizy (olivier.thizy@shelyak.com) François Cochard (francois.cochard@shelyak.com)
Alpy 600 User Guide Olivier Thizy (olivier.thizy@shelyak.com) François Cochard (francois.cochard@shelyak.com) DC0016A : april 2013 Alpy 600 spectroscope User Guide Olivier Thizy (olivier.thizy@shelyak.com)
More information5. The Nature of Light. Does Light Travel Infinitely Fast? EMR Travels At Finite Speed. EMR: Electric & Magnetic Waves
5. The Nature of Light Light travels in vacuum at 3.0. 10 8 m/s Light is one form of electromagnetic radiation Continuous radiation: Based on temperature Wien s Law & the Stefan-Boltzmann Law Light has
More informationAlignement of a ring cavity laser
Alignement of a ring cavity laser 1 Introduction This manual describes a procedure to align the cavity of our Ti:Sapphire ring laser and its injection with an Argon-Ion pump laser beam. The setup is shown
More informationHoward Eskildsen often uploads some of his wonderful and exquisite solar
Solar Images Taken with Calcium K-Line Filters Howard L. Cohen January 2014 (Rev. March 2015) Howard Eskildsen s beautiful images of the Sun uploaded to the AAC website may appear strange and unfamiliar
More informationExperiment 3 Lenses and Images
Experiment 3 Lenses and Images Who shall teach thee, unless it be thine own eyes? Euripides (480?-406? BC) OBJECTIVES To examine the nature and location of images formed by es. THEORY Lenses are frequently
More informationHolography 1 HOLOGRAPHY
Holography 1 HOLOGRAPHY Introduction and Background The aesthetic appeal and commercial usefulness of holography are both related to the ability of a hologram to store a three-dimensional image. Unlike
More information