Experiment 11. Grating constant of diffraction grating

Size: px
Start display at page:

Download "Experiment 11. Grating constant of diffraction grating"

Transcription

1 Experiment 11. Grating constant of diffraction grating 1. Purpose Measure light source s wavelength by using diffraction grating, those grating constant is already known, in order to understand diffraction phenomenon. With this light source, measure unknown diffraction grating s grating constant. 2. Principle Figure 1 illustrates light, which has λ wavelength, passes through glass plate of diffraction grating (G) and m th diffraction light tilted to ф angle. Optical pass difference between nearest linear light is Δ=dsinф Figure 1. where all diffracted light show constructive interference. It makes light intensity maximum. The d is grating constant and m is number of diffracted light. Therefore, if we know grating constant d while measuring diffraction angle ф, we could know wavelength of light source and vise versa

2 3. Equipment and set up Equipment Quantity Laser Diode 1 Light Sensor 1 Rotary Motion Sensor 1 Optics Bench 1 1M Rotation plate 2 Diffraction grating 1 Known grating constant Diffraction grating 1 Unknown grating constant 4. Experiment procedure Caution - Use diffraction grating carefully. - Use Light sensor under limit sensitivity of light intensity. 1-1) Install Data studio program (1) Connect Science Workshop interface into computer and turn on. (2) Connect light sensor and rotary motion sensor to Analog Channel A and Digital Channel, respectively

3 1-2) Equipment and Setup As shown below Figure, Put light sensor at the end of optical bench and laser sensor onto rotation plate. Put rotary motion sensor at the center of rotation plate in order to measure rotation angle. Since ratio of motion sensor to rotation plate is not 1:1, we must rotate rotation plate to 180º for getting correction ratio. Meanwhile, Put sensitivity of light sensor to 1 to control intensity of rotational light. 2) Wavelength measurement of laser diode (1) Put laser diode on optical bench and diffraction grating onto rotation plate as shown above Figure. Attach rotation plate on rotary motion sensor. (2) Put slit in front of light sensor for measuring intensity of passed light precisely. (3) Set up beginning stage by watching quantity of light passing through light sensor to be 0 th diffraction angle. (4) Run Data Studio for connecting light sensor and rotary motion sensor (5) Choose Light Sensor graph located on the lower right side menu. Click x-axis on graph and invert graph as intensity of light vs angle. (6) Rotate rotation plate and observe intensity of light dependence on angle. (7) Read angle when intensity of light show large value after 0 degree and get constant each diffraction angle. (8) Read until 3 rd diffraction angle appears. ( Measure light intensity with increasing sensitivity up to

4 when you have difficulties reading 2 nd diffraction angle. ) (9) Move initial position of diffraction plate and rotate rotation plate opposite direction. Repeat (6)-(8) process and measure angle until 3 rd diffraction angle appears. (10) Record results on Table 1. Calculate average values of each diffraction angle. Calculate wavelength of laser diode by using already known grating constant. 3) Measurement of unknown grating constant - 4 -

5 5. Results Diffraction grating experiment DARA SHEET Table 1. laser diode wavelength measurement (θ m and θ m represents different direction angle) Grating number per mm (n) Grating constant (1mm/n) Diffraction number 1 st (m=1) 2 nd (m=2) 3 rd (m=3) θ m θ m 2Φ m = θ m - θ m Φ m Λ m [mm] Wavelength of laser diode : Λ=(Λ 1 +Λ 2 +Λ 3 )/3 [μm] Λ m =(sin Φ m )/mm [μm] Table 2. Measurement of unknown grating constant Wavelength of laser diode [mm] Diffraction number 1 st (m=1) 2 nd (m=2) 3 rd (m=3) θ m θ m 2Φ m Φ m N Grating number : n=(n 1 +n 2 +n 3 )/3 n=(sin Φ m )/ Λ m m - 5 -

6 6. Questions 1) Why do we do experiments with putting slit in front of laser diode? 2) We user monochromatic light which is emitted from laser diode. But, the light what we see usually is white light which is composed of several wavelengths. What if we use this light as laser diode? Which do we add equipment for doing experiment? And how do we install? 3) Which circumstances are happened when grating constant is smaller than wavelength of laser diode? 4) What kind of laser diode do we need in order to investigate diffraction by passing through grating structure having atom-size grating constant? - 6 -

Polarization of Light

Polarization of Light Polarization of Light References Halliday/Resnick/Walker Fundamentals of Physics, Chapter 33, 7 th ed. Wiley 005 PASCO EX997A and EX999 guide sheets (written by Ann Hanks) weight Exercises and weights

More information

Diffraction of Laser Light

Diffraction 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 information

Interference. Physics 102 Workshop #3. General Instructions

Interference. 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 information

THE BOHR QUANTUM MODEL

THE 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 information

6) How wide must a narrow slit be if the first diffraction minimum occurs at ±12 with laser light of 633 nm?

6) 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 information

Experiment 5: Magnetic Fields of a Bar Magnet and of the Earth

Experiment 5: Magnetic Fields of a Bar Magnet and of the Earth MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.02 Spring 2005 Experiment 5: Magnetic Fields of a Bar Magnet and of the Earth OBJECTIVES 1. To examine the magnetic field associated with a

More information

P R E A M B L E. Facilitated workshop problems for class discussion (1.5 hours)

P 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 information

The Phenomenon of Photoelectric Emission:

The Phenomenon of Photoelectric Emission: The Photoelectric Effect. The Wave particle duality of light Light, like any other E.M.R (electromagnetic radiation) has got a dual nature. That is there are experiments that prove that it is made up of

More information

Solution Derivations for Capa #14

Solution 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 information

Experiment #2: Determining Sugar Content of a Drink. Objective. Introduction

Experiment #2: Determining Sugar Content of a Drink. Objective. Introduction Experiment #2: Determining Sugar Content of a Drink Objective How much sugar is there in your drink? In this experiment, you will measure the amount of sugar dissolved in a soft drink by using two different

More information

Interferometers. OBJECTIVES To examine the operation of several kinds of interferometers. d sin = n (1)

Interferometers. OBJECTIVES To examine the operation of several kinds of interferometers. d sin = n (1) Interferometers The true worth of an experimenter consists in his pursuing not only what he seeks in his experiment, but also what he did not seek. Claude Bernard (1813-1878) OBJECTIVES To examine the

More information

PHYA2. General Certificate of Education Advanced Subsidiary Examination June 2010. Mechanics, Materials and Waves

PHYA2. General Certificate of Education Advanced Subsidiary Examination June 2010. Mechanics, Materials and Waves Centre Number Surname Candidate Number For Examiner s Use Other Names Candidate Signature Examiner s Initials Physics A Unit 2 For this paper you must have: a ruler a calculator a Data and Formulae Booklet.

More information

ILLUSTRATIVE EXAMPLE: Given: A = 3 and B = 4 if we now want the value of C=? C = 3 + 4 = 9 + 16 = 25 or 2

ILLUSTRATIVE 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 information

Diffraction and Young s Single Slit Experiment

Diffraction and Young s Single Slit Experiment Diffraction and Young s Single Slit Experiment Developers AB Overby Objectives Preparation Background The objectives of this experiment are to observe Fraunhofer, or far-field, diffraction through a single

More information

1 of 9 2/9/2010 3:38 PM

1 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 information

Friday 18 January 2013 Morning

Friday 18 January 2013 Morning Friday 18 January 2013 Morning AS GCE PHYSICS B (ADVANCING PHYSICS) G492/01 Understanding Processes / Experimentation and Data Handling *G411640113* Candidates answer on the Question Paper. OCR supplied

More information

ε: Voltage output of Signal Generator (also called the Source voltage or Applied

ε: Voltage output of Signal Generator (also called the Source voltage or Applied Experiment #10: LR & RC Circuits Frequency Response EQUIPMENT NEEDED Science Workshop Interface Power Amplifier (2) Voltage Sensor graph paper (optional) (3) Patch Cords Decade resistor, capacitor, and

More information

SGS: Das Scanning Grating Spektrometer Ein kleines, günstiges Spektrometermodul auf Basis eines dispersiven Mikrosystems

SGS: Das Scanning Grating Spektrometer Ein kleines, günstiges Spektrometermodul auf Basis eines dispersiven Mikrosystems the leading supplier of Micro Scanning Devices Your Micro Optical Solution IPHT-Workshop 11.-12.03.08 We move the light for you! SGS: Das Scanning Grating Spektrometer Ein kleines, günstiges Spektrometermodul

More information

Inductors in AC Circuits

Inductors in AC Circuits Inductors in AC Circuits Name Section Resistors, inductors, and capacitors all have the effect of modifying the size of the current in an AC circuit and the time at which the current reaches its maximum

More information

1 Laboratory #5: Grating Spectrometer

1 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 information

4.4 WAVE CHARACTERISTICS 4.5 WAVE PROPERTIES HW/Study Packet

4.4 WAVE CHARACTERISTICS 4.5 WAVE PROPERTIES HW/Study Packet 4.4 WAVE CHARACTERISTICS 4.5 WAVE PROPERTIES HW/Study Packet Required: READ Hamper pp 115-134 SL/HL Supplemental: Cutnell and Johnson, pp 473-477, 507-513 Tsokos, pp 216-242 REMEMBER TO. Work through all

More information

Setting up the DeskCNC controller.

Setting up the DeskCNC controller. 1) Determine the steps to linear motion ratios for each axis. 2 2) Determine Maximum velocity (speed). 3 3) Setting up the software Machine Tab 4 4) Setting up the software DeskCNC Setup Tab 5 5) Setting

More information

Fraunhofer Diffraction

Fraunhofer Diffraction Physics 334 Spring 1 Purpose Fraunhofer Diffraction The experiment will test the theory of Fraunhofer diffraction at a single slit by comparing a careful measurement of the angular dependence of intensity

More information

O6: The Diffraction Grating Spectrometer

O6: 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 information

Boardworks AS Physics

Boardworks AS Physics Boardworks AS Physics Vectors 24 slides 11 Flash activities Prefixes, scalars and vectors Guide to the SI unit prefixes of orders of magnitude Matching powers of ten to their SI unit prefixes Guide to

More information

Simple Harmonic Motion

Simple Harmonic Motion Simple Harmonic Motion 1 Object To determine the period of motion of objects that are executing simple harmonic motion and to check the theoretical prediction of such periods. 2 Apparatus Assorted weights

More information

WAVELENGTH OF LIGHT - DIFFRACTION GRATING

WAVELENGTH 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 information

Physics 111 Homework Solutions Week #9 - Tuesday

Physics 111 Homework Solutions Week #9 - Tuesday Physics 111 Homework Solutions Week #9 - Tuesday Friday, February 25, 2011 Chapter 22 Questions - None Multiple-Choice 223 A 224 C 225 B 226 B 227 B 229 D Problems 227 In this double slit experiment we

More information

Optical Fibres. Introduction. Safety precautions. For your safety. For the safety of the apparatus

Optical Fibres. Introduction. Safety precautions. For your safety. For the safety of the apparatus Please do not remove this manual from from the lab. It is available at www.cm.ph.bham.ac.uk/y2lab Optics Introduction Optical fibres are widely used for transmitting data at high speeds. In this experiment,

More information

INTERFERENCE OF SOUND WAVES

INTERFERENCE OF SOUND WAVES 1/2016 Sound 1/8 INTERFERENCE OF SOUND WAVES PURPOSE: To measure the wavelength, frequency, and propagation speed of ultrasonic sound waves and to observe interference phenomena with ultrasonic sound waves.

More information

Lab 9: The Acousto-Optic Effect

Lab 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 information

PHOTOELECTRIC EFFECT AND DUAL NATURE OF MATTER AND RADIATIONS

PHOTOELECTRIC EFFECT AND DUAL NATURE OF MATTER AND RADIATIONS PHOTOELECTRIC EFFECT AND DUAL NATURE OF MATTER AND RADIATIONS 1. Photons 2. Photoelectric Effect 3. Experimental Set-up to study Photoelectric Effect 4. Effect of Intensity, Frequency, Potential on P.E.

More information

3.5.4.2 One example: Michelson interferometer

3.5.4.2 One example: Michelson interferometer 3.5.4.2 One example: Michelson interferometer mirror 1 mirror 2 light source 1 2 3 beam splitter 4 object (n object ) interference pattern we either observe fringes of same thickness (parallel light) or

More information

Experiment: Static and Kinetic Friction

Experiment: Static and Kinetic Friction PHY 201: General Physics I Lab page 1 of 6 OBJECTIVES Experiment: Static and Kinetic Friction Use a Force Sensor to measure the force of static friction. Determine the relationship between force of static

More information

AP 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 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 information

INFITEC - A NEW STEREOSCOPIC VISUALISATION TOOL BY WAVELENGTH MULTIPLEX IMAGING

INFITEC - A NEW STEREOSCOPIC VISUALISATION TOOL BY WAVELENGTH MULTIPLEX IMAGING INFITEC - A NEW STEREOSCOPIC VISUALISATION TOOL BY WAVELENGTH MULTIPLEX IMAGING Helmut Jorke, Markus Fritz INFITEC GmbH, Lise-Meitner-Straße 9, 89081 Ulm info@infitec.net Phone +49 731 550299 56 Fax _

More information

Solution 1: Algorithm Positioning

Solution 1: Algorithm Positioning Model No: OEAFP Series All-Fiber Pipeline Security System Solutions Solution 1: Algorithm Positioning Application conditions Applicable for outdoor long-distance oil-gas pipeline security monitoring without

More information

Experiment 2: Conservation of Momentum

Experiment 2: Conservation of Momentum Experiment 2: Conservation of Momentum Learning Goals After you finish this lab, you will be able to: 1. Use Logger Pro to analyze video and calculate position, velocity, and acceleration. 2. Use the equations

More information

Passive Remote Sensing of Clouds from Airborne Platforms

Passive Remote Sensing of Clouds from Airborne Platforms Passive Remote Sensing of Clouds from Airborne Platforms Why airborne measurements? My instrument: the Solar Spectral Flux Radiometer (SSFR) Some spectrometry/radiometry basics How can we infer cloud properties

More information

Physics 30 Worksheet # 14: Michelson Experiment

Physics 30 Worksheet # 14: Michelson Experiment Physics 30 Worksheet # 14: Michelson Experiment 1. The speed of light found by a Michelson experiment was found to be 2.90 x 10 8 m/s. If the two hills were 20.0 km apart, what was the frequency of the

More information

Refractive Index Measurement Principle

Refractive Index Measurement Principle Refractive Index Measurement Principle Refractive index measurement principle Introduction Detection of liquid concentrations by optical means was already known in antiquity. The law of refraction was

More information

Lab 7: Rotational Motion

Lab 7: Rotational Motion Lab 7: Rotational Motion Equipment: DataStudio, rotary motion sensor mounted on 80 cm rod and heavy duty bench clamp (PASCO ME-9472), string with loop at one end and small white bead at the other end (125

More information

Diffraction of a Circular Aperture

Diffraction 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 information

Holography 1 HOLOGRAPHY

Holography 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

GRID AND PRISM SPECTROMETERS

GRID 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 information

EXPERIMENT O-6. Michelson Interferometer. Abstract. References. Pre-Lab

EXPERIMENT 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 information

Acousto-optic modulator

Acousto-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 information

Small Optical Encoder Modules 480lpi Digital Output. Features. Applications VCC 3 CHANNEL A 2 CHANNEL B 4 GND 1

Small Optical Encoder Modules 480lpi Digital Output. Features. Applications VCC 3 CHANNEL A 2 CHANNEL B 4 GND 1 HEDS-9730, HEDS-9731 Small Optical Encoder Modules 480lpi Digital Output Data Sheet Description The HEDS-973X is a high performance incremental encoder module. When operated in conjunction with either

More information

INTERFERENCE OF SOUND WAVES

INTERFERENCE OF SOUND WAVES 2011 Interference - 1 INTERFERENCE OF SOUND WAVES The objectives of this experiment are: To measure the wavelength, frequency, and propagation speed of ultrasonic sound waves. To observe interference phenomena

More information

How Reed Switches are used with a Permanent Magnet

How Reed Switches are used with a Permanent Magnet How Reed Switches are used with a Permanent Magnet Using Reed Switches in a sensing environment, one generally uses a magnet for actuation. It is important to understand this interaction clearly for proper

More information

DIFFRACTION AND INTERFERENCE

DIFFRACTION AND INTERFERENCE DIFFRACTION AND INTERFERENCE In this experiment you will emonstrate the wave nature of light by investigating how it bens aroun eges an how it interferes constructively an estructively. You will observe

More information

Laboratory #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 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 information

PUMPED Nd:YAG LASER. Last Revision: August 21, 2007

PUMPED Nd:YAG LASER. Last Revision: August 21, 2007 PUMPED Nd:YAG LASER Last Revision: August 21, 2007 QUESTION TO BE INVESTIGATED: How can an efficient atomic transition laser be constructed and characterized? INTRODUCTION: This lab exercise will allow

More information

OPERATION MANUAL INFRARED THERMOMETER

OPERATION MANUAL INFRARED THERMOMETER OPERATION MANUAL INFRARED THERMOMETER Features: Precise non-contact measurements Built-in laser pointer Automatic selection range and Resolution to 0.1ºor 1º / switchable button Automatic Data Hold & Auto

More information

Physics 41, Winter 1998 Lab 1 - The Current Balance. Theory

Physics 41, Winter 1998 Lab 1 - The Current Balance. Theory Physics 41, Winter 1998 Lab 1 - The Current Balance Theory Consider a point at a perpendicular distance d from a long straight wire carrying a current I as shown in figure 1. If the wire is very long compared

More information

STATIC AND KINETIC FRICTION

STATIC AND KINETIC FRICTION STATIC AND KINETIC FRICTION LAB MECH 3.COMP From Physics with Computers, Vernier Software & Technology, 2000. INTRODUCTION If you try to slide a heavy box resting on the floor, you may find it difficult

More information

Lab 1: Introduction to PSpice

Lab 1: Introduction to PSpice Lab 1: Introduction to PSpice Objectives A primary purpose of this lab is for you to become familiar with the use of PSpice and to learn to use it to assist you in the analysis of circuits. The software

More information

Stereoscopic 3D Digital Theater System. Operator Manual (MI-2100)

Stereoscopic 3D Digital Theater System. Operator Manual (MI-2100) Stereoscopic 3D Digital Theater System Operator Manual (MI-2100) -1- All information contained in or disclosed by this document is confidential and propriety to masterimage Co., Ltd. (hereinafter referred

More information

Using the Spectrophotometer

Using 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 information

Basic Optics System OS-8515C

Basic 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 information

ATOMIC SPECTRA. Apparatus: Optical spectrometer, spectral tubes, power supply, incandescent lamp, bottles of dyed water, elevating jack or block.

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 information

Bio 321 Lightmicroscopy Electronmicrosopy Image Processing

Bio 321 Lightmicroscopy Electronmicrosopy Image Processing Bio 321 Lightmicroscopy Electronmicrosopy Image Processing Urs Ziegler Center for Microscopy and Image Analysis Light microscopy (Confocal Laser Scanning Microscopy) Light microscopy (Confocal Laser Scanning

More information

FREE FALL. Introduction. Reference Young and Freedman, University Physics, 12 th Edition: Chapter 2, section 2.5

FREE FALL. Introduction. Reference Young and Freedman, University Physics, 12 th Edition: Chapter 2, section 2.5 Physics 161 FREE FALL Introduction This experiment is designed to study the motion of an object that is accelerated by the force of gravity. It also serves as an introduction to the data analysis capabilities

More information

1 de 13. Kit de 37 sensores compatibles con Arduino

1 de 13. Kit de 37 sensores compatibles con Arduino 1 de 13 Kit de 37 sensores compatibles con Arduino 2 de 13 Item Picture Description KY001: Temperature This module measures the temperature and reports it through the 1-wire bus digitally to the Arduino.

More information

WHITE PAPER. Are More Pixels Better? www.basler-ipcam.com. Resolution Does it Really Matter?

WHITE PAPER. Are More Pixels Better? www.basler-ipcam.com. Resolution Does it Really Matter? WHITE PAPER www.basler-ipcam.com Are More Pixels Better? The most frequently asked question when buying a new digital security camera is, What resolution does the camera provide? The resolution is indeed

More information

INTRODUCTION FIGURE 1 1. Cosmic Rays. Gamma Rays. X-Rays. Ultraviolet Violet Blue Green Yellow Orange Red Infrared. Ultraviolet.

INTRODUCTION FIGURE 1 1. Cosmic Rays. Gamma Rays. X-Rays. Ultraviolet Violet Blue Green Yellow Orange Red Infrared. Ultraviolet. INTRODUCTION Fibre optics behave quite different to metal cables. The concept of information transmission is the same though. We need to take a "carrier" signal, identify a signal parameter we can modulate,

More information

LBS-300 Beam Sampler for C-mount Cameras. YAG Focal Spot Analysis Adapter. User Notes

LBS-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 information

PHYSICS PAPER 1 (THEORY)

PHYSICS 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 information

How To Understand Light And Color

How 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 information

Alignement of a ring cavity laser

Alignement 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 information

Rutgers Analytical Physics 750:228, Spring 2016 ( RUPHY228S16 )

Rutgers Analytical Physics 750:228, Spring 2016 ( RUPHY228S16 ) 1 of 13 2/17/2016 5:28 PM Signed in as Weida Wu, Instructor Help Sign Out Rutgers Analytical Physics 750:228, Spring 2016 ( RUPHY228S16 ) My Courses Course Settings University Physics with Modern Physics,

More information

Atomic Force Microscope

Atomic Force Microscope Atomic Force Microscope (Veeco Nanoman) User Manual Basic Operation 4 th Edition Aug 2012 NR System Startup If the system is currently ON To start the NanoScope software, double-click the NanoScope startup

More information

A NEW LOOK AT RISLEY PRISMS. By Craig Schwarze Senior Systems Engineer OPTRA Inc.

A NEW LOOK AT RISLEY PRISMS. By Craig Schwarze Senior Systems Engineer OPTRA Inc. As seen in Photonics Spectra June 2006: A NEW LOOK AT RISLEY PRISMS By Craig Schwarze Senior Systems Engineer OPTRA Inc. Introduction With laser beams finding more and more applications that require aiming

More information

Laser Diode Gas Sensors

Laser Diode Gas Sensors Laser Diode Gas Sensors Photonic Sensors Swiss Laser Net Workshop Biel 17.09.09 Thomas Hessler Overview Leister and ist photonic activities TDLS detection principle TDLS product plattform Applications

More information

A Guide to Acousto-Optic Modulators

A Guide to Acousto-Optic Modulators A Guide to Acousto-Optic Modulators D. J. McCarron December 7, 2007 1 Introduction Acousto-optic modulators (AOMs) are useful devices which allow the frequency, intensity and direction of a laser beam

More information

Automatisierte, hochpräzise Optikmontage Lösungen für die Industrie

Automatisierte, hochpräzise Optikmontage Lösungen für die Industrie Automatisierte, hochpräzise Optikmontage Lösungen für die Industrie Alexander Steinecker, CSEM Trends in Micro Nano, HSLU, Horw, 5. Dezember 2013 High power laser sources Motivation Laser manufacturing

More information

L-LAS-TB-CL serie. laser light curtains for inline measuring tasks

L-LAS-TB-CL serie. laser light curtains for inline measuring tasks L-LAS-TB-CL serie laser light curtains for inline measuring tasks Maximum distance 2.000 mm Measurement range 6 up to 98 mm Resolution up to 4 µm up to 1,5 khz scan rate 0-10 V or 4-20 ma analogue output

More information

Proposed experiment to test the non-locality hypothesis in transient light-interference phenomena

Proposed experiment to test the non-locality hypothesis in transient light-interference phenomena Proposed experiment to test the non-locality hypothesis in transient light-interference phenomena Masanori Sato Honda Electronics Co., Ltd., 20 Oyamazuka, Oiwa-cho, Toyohashi, Aichi 441-3193, Japan Abstract

More information

4. CAMERA ADJUSTMENTS

4. CAMERA ADJUSTMENTS 4. CAMERA ADJUSTMENTS Only by the possibility of displacing lens and rear standard all advantages of a view camera are fully utilized. These displacements serve for control of perspective, positioning

More information

Mechanics. Determining the gravitational constant with the gravitation torsion balance after Cavendish. LD Physics Leaflets P1.1.3.1.

Mechanics. Determining the gravitational constant with the gravitation torsion balance after Cavendish. LD Physics Leaflets P1.1.3.1. Mechanics Measuring methods Determining the gravitational constant LD Physics Leaflets P1.1.3.1 Determining the gravitational constant with the gravitation torsion balance after Cavendish Measuring the

More information

Experiment #5: Qualitative Absorption Spectroscopy

Experiment #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 information

6/2016 E&M forces-1/8 ELECTRIC AND MAGNETIC FORCES. PURPOSE: To study the deflection of a beam of electrons by electric and magnetic fields.

6/2016 E&M forces-1/8 ELECTRIC AND MAGNETIC FORCES. PURPOSE: To study the deflection of a beam of electrons by electric and magnetic fields. 6/016 E&M forces-1/8 ELECTRIC AND MAGNETIC FORCES PURPOSE: To study the deflection of a beam of electrons by electric and magnetic fields. APPARATUS: Electron beam tube, stand with coils, power supply,

More information

Measuring index of refraction

Measuring index of refraction Grzegorz F. Wojewoda Zespół Szkół Ogólnokształcących nr 1 Bydgoszcz, Poland Logo designed by Armella Leung, www.armella.fr.to Translation: Małgorzata Czart Measuring index of refraction The advent of low-cost

More information

Laser diffuse reflection light scanner with background suppression. Dimensioned drawing

Laser diffuse reflection light scanner with background suppression. Dimensioned drawing Specifications and description HRTL 3B Laser diffuse reflection light scanner with background suppression Dimensioned drawing We reserve the right to make changes DS_HRTL3B_en.fm en 01-2010/12 50114049

More information

Vandal-Proof IR Dome Camera

Vandal-Proof IR Dome Camera Vandal-Proof IR Dome Camera Instruction Manual VER.:1.0, NO.:040118 Thank you very much for purchasing our product. Before operating this product, please read this instruction manual carefully to ensure

More information

Refraction 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. 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 information

Tube Control Measurement, Sorting Modular System for Glass Tube

Tube Control Measurement, Sorting Modular System for Glass Tube Tube Control Measurement, Sorting Modular System for Glass Tube Tube Control is a modular designed system of settled instruments and modules. It comprises measuring instruments for the tube dimensions,

More information

WOOD WEAR TESTING USING TRIBOMETER

WOOD WEAR TESTING USING TRIBOMETER WOOD WEAR TESTING USING TRIBOMETER Prepared by Duanjie Li, PhD 6 Morgan, Ste156, Irvine CA 92618 P: 949.461.9292 F: 949.461.9232 nanovea.com Today's standard for tomorrow's materials. 2015 NANOVEA INTRO

More information

Using light scattering method to find The surface tension of water

Using 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 information

Mercury TM 1500P PCB-Mount Digital Encoders

Mercury TM 1500P PCB-Mount Digital Encoders Mercury TM 1500P PCB-Mount Digital Encoders Factory Set Resolution to 0.50μm Reflective Linear and Rotary Encoders Sensor the size of a Dime Resolution Factory Set: x4, x8, x20, or x40 Linear: 5μm, 2.5μm,

More information

Pre-lab Quiz/PHYS 224 Magnetic Force and Current Balance. Your name Lab section

Pre-lab Quiz/PHYS 224 Magnetic Force and Current Balance. Your name Lab section Pre-lab Quiz/PHYS 224 Magnetic Force and Current Balance Your name Lab section 1. What do you investigate in this lab? 2. Two straight wires are in parallel and carry electric currents in opposite directions

More information

PRECISION INTERFEROMETER

PRECISION INTERFEROMETER Includes Teacher's Notes and Typical Experiment Results Instruction Manual and Experiment Guide for the PASCO scientific Models OS-9255A thru OS-9258A 012-07137A 5/99 PRECISION INTERFEROMETER 1990 PASCO

More information

LOCATION DEPENDENCY OF POSITIONING ERROR IN A 3-AXES CNC MILLING MACHINE

LOCATION DEPENDENCY OF POSITIONING ERROR IN A 3-AXES CNC MILLING MACHINE th International & 26 th All India Manufacturing Technology, Design and Research Conference (AIMTDR 214) December 12 th 14 th, 214, IIT Guwahati, Assam, India LOCATION DEPENDENCY OF POSITIONING ERROR IN

More information

Physics 441/2: Transmission Electron Microscope

Physics 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 information

AP PHYSICS C Mechanics - SUMMER ASSIGNMENT FOR 2016-2017

AP PHYSICS C Mechanics - SUMMER ASSIGNMENT FOR 2016-2017 AP PHYSICS C Mechanics - SUMMER ASSIGNMENT FOR 2016-2017 Dear Student: The AP physics course you have signed up for is designed to prepare you for a superior performance on the AP test. To complete material

More information

Experiment 4 ~ Newton s Second Law: The Atwood Machine

Experiment 4 ~ Newton s Second Law: The Atwood Machine xperiment 4 ~ Newton s Second Law: The twood Machine Purpose: To predict the acceleration of an twood Machine by applying Newton s 2 nd Law and use the predicted acceleration to verify the equations of

More information

5.1 The First Law: The Law of Inertia

5.1 The First Law: The Law of Inertia The First Law: The Law of Inertia Investigation 5.1 5.1 The First Law: The Law of Inertia How does changing an object s inertia affect its motion? Newton s first law states that objects tend to keep doing

More information

Size Of the Image Nature Of the Image At Infinity At the Focus Highly Diminished, Point Real and Inverted

Size Of the Image Nature Of the Image At Infinity At the Focus Highly Diminished, Point Real and Inverted CHAPTER-10 LIGHT REFLECTION AND REFRACTION Light rays; are; electromagnetic in nature, and do not need material medium for Propagation Speed of light in vacuum in 3*10 8 m/s When a light ray falls on a

More information

Experiment 5. Lasers and laser mode structure

Experiment 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 information