DSP Analysis of Digital Vector Slope Gauge Data Produced by Ocean Wave Simulation

Size: px
Start display at page:

Download "DSP Analysis of Digital Vector Slope Gauge Data Produced by Ocean Wave Simulation"

Transcription

1 DSP Analysis of Digital Vector Slope Gauge Data Produced by Ocean Wave Simulation EECS Introduction to Research Prof. Earl Schweppe,, Instructor Evan L. Bryson

2 Overview Ocean Wave Behavior The Vector Slope Gauge (VSG) VSG History VSG Function Ocean Wave Data Simulation Off-line Processing Future Work

3 Overview Ocean Wave Behavior The Vector Slope Gauge (VSG) VSG History VSG Function Ocean Wave Data Simulation Off-line Processing Future Work

4 Ocean Wave Behavior Spectrum Wavelength, period, and velocity Deep water vs. shallow water waves Sea = linear sum of waves Orbital velocity

5 Ocean Wave Spectrum (From Kampion, 1997)

6 Wave Velocity vs. Wavelength and Period (From Kampion, 1997)

7 Simple Wavefront Description Height of ocean wave at time t and position (x,y): h( x, y, t) = Acos( Ωt + κx cosα + κy sinα + φ) where Ω = κ = L = T = α = φ = 2π = angular frequency (rad/sec) T 2π = wave number (rad/m) L wavelength (m) wave period (sec) wave approach direction phase

8 Superposition of Waves Complex Sea = Superposition of many wavefronts Individual wavefronts are approximately sinusoidal in deep ocean Wavefronts change shape near shore as water depth decreases Single wavefront is rare in nature Wavefronts are initiated by winds over the ocean at other locations (From Bascom, 1964)

9 (From Kampion, 1997)

10 Orbital Velocity (From Kampion, 1997) (From Bascom, 1964)

11 Overview Ocean Wave Behavior The Vector Slope Gauge (VSG) VSG History VSG Function Ocean Wave Data Simulation Off-line Processing Future Work

12 VSG History Version 1 Analog VSG Tested in the North Sea in 1990 Version 2 Improvement of Version 1 Tested at Duck Pier in 1995 Version 3 Digital VSG No ocean surface data available

13 VSG Function VSG z y axis is radar look direction Θ is incidence angle H is height above mean ocean surface H Θ y x

14 Typical VSG Beam Pattern on Ocean Surface Beam 3 Beam 2 Beam 1 ~ 1 meter ~ 1 meter

15 Frequency Format of VSG Radar Signal Sweep Cycle Upsweep Downsweep F Bandwidth Beam 1 Beam 2 Beam 3 T

16 Instantaneous IF Output and Return for Range Measurement Radar Signals Transmitted Signal Returned Signal F Intermediate Frequency Signal (Difference Frequency) T (Adapted from Ulaby, Moore, and Fung, Fig. 7.25, p. 513)

17 Instantaneous IF Output and Return for Range and Doppler Measurement Radar Signals Transmitted Signal Returned Signal F Intermediate Frequency Signal (Difference Frequency) T (Adapted from Ulaby, Moore, and Fung, Fig. 7.25, p. 513)

18 Instantaneous Frequencies for Point Target Magnified View of a Portion of the Signal Transmitted Signal F F Returned Signal T T (Adapted from Ulaby, Moore, and Fung, Fig. 7.25, p. 513)

19 VSG Parameters Range Sweep repetition frequency Single (Up or Down) sweep time Sweep rate Minimum DSP sample rate R f T B = = sweep f t f smin hvsg = cosθ = c fif 4B R = 1 2f B T B sweep = 2 f IF = 10 cos( 45) = 8 3 (3 10 ) (60010 ) µs = 1.0MHz = m 4000Hz = 4.76Mhz/ µ sec

20 Overview Ocean Wave Behavior The Vector Slope Gauge (VSG) VSG History VSG Function Ocean Wave Data Simulation Off-line Processing Future Work

21 Ocean Wave Data Simulation for Digital VSG Characterize simple ocean surfaces Flat surface (calm sea) Single wavefront Multiple wave fronts Add Doppler shift to surfaces Convert ranges + Doppler to frequencies Digital sampling of frequencies Scale and shift Convert to 12-bit unsigned integers Create data files in digital VSG format

22 Ocean Wave Data Simulation WaveSim7.m RangeEst.m slrangemod.m slopepoimod.m Save2Slopes.m VSG Parameters slopeab2.m SlopeOut.txt Wavesim7.m Range IF SampGen.m Sampled IF Ocean Wave Parameters NsPerSweep.m VSGOutput.m VSGOut.bin

23 Digital VSG Data Format MSB LSB not used (always 0) Beam # Up/Down 0 = Up 1 = Down 00 = Beam 1 01 = Beam 2 10 = Beam 3 11 not used Data 12 bit unsigned integer

24 Overview Ocean Wave Behavior The Vector Slope Gauge (VSG) VSG History VSG Function Ocean Wave Data Simulation Off-line Processing Future Work

25 Off-line Processing Current Vector Slope Gauge Concept VSG Raw VSG Data Data Storage Hard Disk Delay Data Preparation Data Processing and Calculations Printer Output of Results

26 DSP Algorithm Ocean Project Data Beam 1 Up Data Beam 1 Down PSD PSD BPF BPF Calculate f eff, u Calculate f eff, d Storage Buffer Storage Buffer Calculate f avg, u Calculate f avg, d + + _ + Scale to Velocity Scale to Range f d1 1 R 1 R 1 R 2 R 3 Calculate Vector Slope Look Angle Data Beam 2 Up Data Beam 2 Down PSD PSD BPF BPF Calculate f eff, u Calculate f eff, d Storage Buffer Storage Buffer Calculate f avg, u Calculate f avg, d + + _ + Scale to Velocity Scale to Range f d2 2 R 2 f d1 f d2 f d3 Calculate f d, avg Data Beam 3 Up Data Beam 3 Down PSD PSD BPF BPF Calculate f eff, u Calculate f eff, d Storage Buffer Storage Buffer Calculate f avg, u Calculate f avg, d + + _ + Scale to Velocity Scale to Range f d3 3 R 3 Adapted from DSP Algorithm for Ocean Radar Project, Gary W. Hamilton II

27 DSP of Stored Ocean Wave Data DSP2.m VSG Parameters VSGOut.bin DSP2.m GetTimeSeries2.m FindPSD.m Upsweep Downsweep Shift and Scale FindEffFreq.m evanslope.m Sum Average Frequency Difference Average Frequency Slopes Sx, Sy Range Doppler

28 Overview Ocean Wave Behavior The Vector Slope Gauge (VSG) VSG History VSG Function Ocean Wave Data Simulation Off-line Processing Future Work

29 Future Work Collect ocean data on digital VSG Comparison to Duck Pier results Orbital velocity measurement Real-time DSP Adaptation to shipboard environment

30 Real-Time Vector Slope Gauge Concept VSG Raw VSG Data DSP Board On-Screen Results DSP Program

31 (Kampion, 1997) University of Kansas

Workhorse ADCP Multi- Directional Wave Gauge Primer

Workhorse ADCP Multi- Directional Wave Gauge Primer Acoustic Doppler Solutions Workhorse ADCP Multi- Directional Wave Gauge Primer Brandon Strong October, 2000 Principles of ADCP Wave Measurement The basic principle behind wave the measurement, is that

More information

Chapter 37. Wave Optics

Chapter 37. Wave Optics Chapter 37 Wave Optics Wave Optics Wave optics is a study concerned with phenomena that cannot be adequately explained by geometric (ray) optics. Sometimes called physical optics These phenomena include:

More information

NAME:... REFRACTION. Page 1

NAME:... REFRACTION.   Page 1 NAME:... REFRACTION 1. A ray of red light enters a semi-circular glass block normal to the curved surface. Which diagram correctly shows the partial reflection and refraction of the ray? www.kcpe-kcse.com

More information

14 Chapter. Interference and Diffraction

14 Chapter. Interference and Diffraction 14 Chapter Interference and Diffraction 14.1 Superposition of Waves... 14-14.1.1 Interference Conditions for Light Sources... 14-4 14. Young s Double-Slit Experiment... 14-4 Example 14.1: Double-Slit Experiment...

More information

Let s review the four equations we now call Maxwell s equations. (Gauss s law for magnetism) (Faraday s law)

Let s review the four equations we now call Maxwell s equations. (Gauss s law for magnetism) (Faraday s law) Electromagnetic Waves Let s review the four equations we now call Maxwell s equations. E da= B d A= Q encl ε E B d l = ( ic + ε ) encl (Gauss s law) (Gauss s law for magnetism) dφ µ (Ampere s law) dt dφ

More information

MEASUREMENT OF THE WAVELENGTH WITH APPLICATION OF A DIFFRACTION GRATING AND A SPECTROMETER

MEASUREMENT OF THE WAVELENGTH WITH APPLICATION OF A DIFFRACTION GRATING AND A SPECTROMETER Warsaw University of Technology Faculty of Physics Physics Laboratory I P Irma Śledzińska 4 MEASUREMENT OF THE WAVELENGTH WITH APPLICATION OF A DIFFRACTION GRATING AND A SPECTROMETER 1. Fundamentals Electromagnetic

More information

Development of Real Time Wave Simulation Technique

Development of Real Time Wave Simulation Technique Development of Real Time Wave Simulation Technique Ben T. Nohara, Member Masami Matsuura, Member Summary The research of ocean s has been important, not changing since the Age of Great Voyages, because

More information

1 Laboratory #4: Division-of-Wavefront Interference

1 Laboratory #4: Division-of-Wavefront Interference 1051-455-0073, Physical Optics 1 Laboratory #4: Division-of-Wavefront Interference 1.1 Theory Recent labs on optical imaging systems have used the concept of light as a ray in goemetrical optics to model

More information

Experiment 6. Snell s Law. Use Snell s Law to determine the index of refraction of Lucite.

Experiment 6. Snell s Law. Use Snell s Law to determine the index of refraction of Lucite. Experiment 6 Snell s Law 6.1 Objectives Use Snell s Law to determine the index of refraction of Lucite. Observe total internal reflection and calculate the critical angle. Explain the basis of how optical

More information

Problem Solving 10: Double-Slit Interference

Problem Solving 10: Double-Slit Interference MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of hysics roblem Solving 10: Double-Slit Interference OBJECTIVES 1. To introduce the concept of interference. 2. To find the conditions for constructive

More information

The Light Field. Last lecture: Radiometry and photometry

The Light Field. Last lecture: Radiometry and photometry The Light Field Last lecture: Radiometry and photometry This lecture: Light field = radiance function on rays Conservation of radiance Measurement equation Throughput and counting rays Irradiance calculations

More information

FRESNEL DIFFRACTION AND PARAXIAL WAVE EQUATION. A. Fresnel diffraction

FRESNEL DIFFRACTION AND PARAXIAL WAVE EQUATION. A. Fresnel diffraction 19 IV. FRESNEL DIFFRACTION AND PARAXIAL WAVE EQUATION A. Fresnel diffraction Any physical optical beam is of finite transverse cross section. Beams of finite cross section may be described in terms of

More information

16. Holography. Dennis Gabor (1947) Nobel Prize in Physics (1971)

16. Holography. Dennis Gabor (1947) Nobel Prize in Physics (1971) 16. Holography Dennis Gabor (1947) Nobel Prize in Physics (1971) Photography Records intensity distribution of light. Does not record direction. Two-dimensional image. Holography = whole + writing Records

More information

dq dt I = Irradiance or Light Intensity is Flux Φ per area A (W/m 2 ) Φ =

dq dt I = Irradiance or Light Intensity is Flux Φ per area A (W/m 2 ) Φ = Radiometry (From Intro to Optics, Pedrotti -4) Radiometry is measurement of Emag radiation (light) Consider a small spherical source Total energy radiating from the body over some time is Q total Radiant

More information

MILLIMETER WAVE INDUSTRIAL DISTANCE SENSOR FMCW 94/10/X

MILLIMETER WAVE INDUSTRIAL DISTANCE SENSOR FMCW 94/10/X 46 Robezu str. LV-1004 Riga Latvia Phone: +371-7-065-100, Fax: +371-7-065-102 Mm-wave Division in St. Petersburg, Russia Phone: +7-812-326-5924, Fax: +7-812-326-1060 MILLIMETER WAVE INDUSTRIAL DISTANCE

More information

Chapter 37. Interference of Light Waves

Chapter 37. Interference of Light Waves Chapter 37 Interference of Light Waves Wave Optics Wave optics is a study concerned with phenomena that cannot be adequately explained by geometric (ray) optics These phenomena include: Interference Diffraction

More information

PHYS 202 Notes, Week 8

PHYS 202 Notes, Week 8 PHYS 202 Notes, Week 8 Greg Christian March 8 & 10, 2016 Last updated: 03/10/2016 at 12:30:44 This week we learn about electromagnetic waves and optics. Electromagnetic Waves So far, we ve learned about

More information

HALF YEARLY EXAMINATIONS 2015/2016. Answer ALL questions showing your working Where necessary give your answers correct to 2 decimal places.

HALF YEARLY EXAMINATIONS 2015/2016. Answer ALL questions showing your working Where necessary give your answers correct to 2 decimal places. Track 3 GIRLS SECONDARY, MRIEHEL HALF YEARLY EXAMINATIONS 2015/2016 FORM: 4 PHYSICS Time: 1½ hrs Name: Class: Answer ALL questions showing your working Where necessary give your answers correct to 2 decimal

More information

UNIQUE SCIENCE ACADEMY

UNIQUE SCIENCE ACADEMY 1 UNIQUE SIENE EMY Test (Unit 1-15) Name :... Paper: Physics ate : 27.05.2011 ode: 5054 lass: II Time llowed: 5Minutes Maximum Marks: 25 1 Theory Section: [Total 16 Marks] Fig.1.1 shows three wavefronts

More information

Contours of slopes of a rippled water surface

Contours of slopes of a rippled water surface Contours of slopes of a rippled water surface Charles Cox* and Xin Zhang Scripps Institution of Oceanography, UCSD 0213, La Jolla, California 9209, USA *cscox@ucsd.edu Abstract: The appearance of a horizontal

More information

Comparison of Wind Retrievals from a. Scanning LIDAR and a Vertically Profiling LIDAR for Wind Energy Remote Sensing Applications

Comparison of Wind Retrievals from a. Scanning LIDAR and a Vertically Profiling LIDAR for Wind Energy Remote Sensing Applications Comparison of Wind Retrievals from a Headline Scanning LIDAR and a Vertically Profiling LIDAR for Wind Energy Remote Sensing Applications PAUL T. QUELET1, JULIE K. LUNDQUIST1,2 1University of Colorado,

More information

A simulator of sea clutter from X-band radar at low grazing angles

A simulator of sea clutter from X-band radar at low grazing angles A simulator of sea clutter from X-band radar at low grazing angles Guillaume Sicot, Nicolas Thomas Actimar 36 quai de la douane 29200 Brest - France Email: guillaume.sicot@actimar.fr Jean-Marc Le Caillec

More information

Chapter 37 HW Q: 2, 4, 7, 10, P: 4, 8, 13, 19, 21, 28, 31, 36, 42, 59, 62

Chapter 37 HW Q: 2, 4, 7, 10, P: 4, 8, 13, 19, 21, 28, 31, 36, 42, 59, 62 Chapter 37 HW Q: 2, 4, 7, 10, P: 4, 8, 13, 19, 21, 28, 31, 36, 42, 59, 62 Wave Interference y = y 1 +y 2 = 2A cos (φ/2) sin (kx - ωt + φ/2) Δφ Resultant Amplitude: 2Acos 2 Constructive Interference: Δ

More information

Section 9.1 Angles, Arcs, & Their Measures (Part I)

Section 9.1 Angles, Arcs, & Their Measures (Part I) Week 1 Handout MAC 1114 Professor Niraj Wagh J Section 9.1 Angles, Arcs, & Their Measures (Part I) Basic Terminology Line: Two distinct points A and B determine a line called line AB. Segment: The portion

More information

Diffraction. Introduction: Diffraction is bending of waves around an obstacle (barrier) or spreading of waves passing through a narrow slit.

Diffraction. Introduction: Diffraction is bending of waves around an obstacle (barrier) or spreading of waves passing through a narrow slit. Introduction: Diffraction is bending of waves around an obstacle (barrier) or spreading of waves passing through a narrow slit. Diffraction amount depends on λ/a proportion If a >> λ diffraction is negligible

More information

Light. Form of Electromagnetic Energy Only part of Electromagnetic Spectrum that we can really see

Light. Form of Electromagnetic Energy Only part of Electromagnetic Spectrum that we can really see Light Form of Electromagnetic Energy Only part of Electromagnetic Spectrum that we can really see Facts About Light The speed of light, c, is constant in a vacuum. Light can be: REFLECTED ABSORBED REFRACTED

More information

Diffraction Diffraction occurs when light waves pass through an aperture Huygen's Principal: each point on wavefront acts as source of another wave

Diffraction Diffraction occurs when light waves pass through an aperture Huygen's Principal: each point on wavefront acts as source of another wave Diffraction Diffraction occurs when light waves pass through an aperture Huygen's Principal: each point on wavefront acts as source of another wave If light coming from infinity point source at infinity

More information

PHYS 3410/6750: Modern Optics Midterm #2

PHYS 3410/6750: Modern Optics Midterm #2 Name: PHYS 3410/6750: Modern Optics Midterm #2 Wednesday 16 November 2011 Prof. Bolton Only pen or pencil are allowed. No calculators or additional materials. PHYS 3410/6750 Fall 2011 Midterm #2 2 Problem

More information

College Physics 150. Chapter 25 Interference and Diffraction

College Physics 150. Chapter 25 Interference and Diffraction College Physics 50 Chapter 5 Interference and Diffraction Constructive and Destructive Interference The Michelson Interferometer Thin Films Young s Double Slit Experiment Gratings Diffraction Resolution

More information

Answer Notes Marks 1 (a) MP1. pitch is frequency; allow it for pitch

Answer Notes Marks 1 (a) MP1. pitch is frequency; allow it for pitch (a) MP. pitch is frequency; allow it for pitch MP. any one of: whether sound/note sounds high or low; high sound has high frequency ORA; ignore references to amplitude, wavelength allow vibrates more often

More information

RADIANCE IN THE OCEAN: EFFECTS OF WAVE SLOPE AND RAMAN SCATTERING NEAR THE SURFACE AND AT DEPTHS THROUGH THE ASYMPTOTIC REGION

RADIANCE IN THE OCEAN: EFFECTS OF WAVE SLOPE AND RAMAN SCATTERING NEAR THE SURFACE AND AT DEPTHS THROUGH THE ASYMPTOTIC REGION RADIANCE IN THE OCEAN: EFFECTS OF WAVE SLOPE AND RAMAN SCATTERING NEAR THE SURFACE AND AT DEPTHS THROUGH THE ASYMPTOTIC REGION A Thesis by JULIE MARIE SLANKER Submitted to the Office of Graduate Studies

More information

dq dt I = Irradiance or Light Intensity is Flux Φ per area A (W/m 2 ) Φ =

dq dt I = Irradiance or Light Intensity is Flux Φ per area A (W/m 2 ) Φ = Radiometry (From Intro to Optics, Pedrotti -4) Radiometry is measurement of Emag radiation (light) Consider a small spherical source Total energy radiating from the body over some time is Q total Radiant

More information

Wave properties The wave speed A two-dimensional traveling wave is a disturbance of a medium, which can be expressed

Wave properties The wave speed A two-dimensional traveling wave is a disturbance of a medium, which can be expressed Wave phenomena: ripple tank experiments References: PASCO Instruction Manual and Experiment Guide for Ripple Generator and Ripple Tank System G. Kuwabara, T. Hasegawa, K. Kono: Water waves in a ripple

More information

Stable simulations of illumination patterns caused by focusing of sunlight by water waves

Stable simulations of illumination patterns caused by focusing of sunlight by water waves Stable simulations of illumination patterns caused by focusing of sunlight by water waves Sjoerd de Ridder ABSTRACT Illumination patterns of underwater sunlight have fascinated various researchers in the

More information

3 - SYNTHETIC APERTURE RADAR (SAR) SUMMARY David Sandwell, SIO 239, January, 2008

3 - SYNTHETIC APERTURE RADAR (SAR) SUMMARY David Sandwell, SIO 239, January, 2008 1 3 - SYNTHETIC APERTURE RADAR (SAR) SUMMARY David Sandwell, SIO 239, January, 2008 Fraunhoffer diffraction To understand why a synthetic aperture in needed for microwave remote sensing from orbital altitude

More information

2017 Summer Course on Optical Oceanography and Ocean Color Remote Sensing. Apparent Optical Properties and the BRDF

2017 Summer Course on Optical Oceanography and Ocean Color Remote Sensing. Apparent Optical Properties and the BRDF 2017 Summer Course on Optical Oceanography and Ocean Color Remote Sensing Curtis Mobley Apparent Optical Properties and the BRDF Delivered at the Darling Marine Center, University of Maine July 2017 Copyright

More information

E x Direction of Propagation. y B y

E x Direction of Propagation. y B y x E x Direction of Propagation k z z y B y An electromagnetic wave is a travelling wave which has time varying electric and magnetic fields which are perpendicular to each other and the direction of propagation,

More information

4D Technology Corporation

4D Technology Corporation 4D Technology Corporation Dynamic Laser Interferometry for Company Profile Disk Shape Characterization DiskCon Asia-Pacific 2006 Chip Ragan chip.ragan@4dtechnology.com www.4dtechnology.com Interferometry

More information

Laser Diffraction and Interference

Laser Diffraction and Interference Laser Diffraction and Interference Objective 1. To determine the wavelength of laser light from a thin wire diffraction pattern.. Compare the thickness of the wire with the single-slit width that form

More information

DETERMINISTIC 3D RADIATION TRANSPORT SIMULATION FOR DOSE DISTRIBUTION AND ORGAN DOSE EVALUATION IN DIAGNOSTIC CT

DETERMINISTIC 3D RADIATION TRANSPORT SIMULATION FOR DOSE DISTRIBUTION AND ORGAN DOSE EVALUATION IN DIAGNOSTIC CT DETERMINISTIC 3D RADIATION TRANSPORT SIMULATION FOR DOSE DISTRIBUTION AND ORGAN DOSE EVALUATION IN DIAGNOSTIC CT Monica Ghita,, Glenn Sjoden, Manuel Arreola, Ahmad Al-Basheer Basheer, Choonsik Lee, Wesley

More information

Femtosecond Single Shot Autocorrelator. Model ASF-20 INSTRUCTION MANUAL

Femtosecond Single Shot Autocorrelator. Model ASF-20 INSTRUCTION MANUAL 1 Femtosecond Single Shot Autocorrelator Model ASF-20 INSTRUCTION MANUAL 2 The Single Shot Autocorrelator (SSA) Model ASF-20 was designed to monitor the pulsewidth of both oscillators and amplifiers of

More information

A SPECTRAL ANALYSIS OF SINGLE ANTENNA INTERFEROMETRY. Craig Stringham

A SPECTRAL ANALYSIS OF SINGLE ANTENNA INTERFEROMETRY. Craig Stringham A SPECTRAL ANALYSIS OF SINGLE ANTENNA INTERFEROMETRY Craig Stringham Microwave Earth Remote Sensing Laboratory Brigham Young University 459 CB, Provo, UT 84602 March 18, 2013 ABSTRACT This paper analyzes

More information

SS4 - Spatial array processing

SS4 - Spatial array processing Doctoral Program on Electrical Engineering and Communications Sérgio M. Jesus (sjesus@ualg.pt) Universidade do Algarve, PT-8005-139 Faro, Portugal www.siplab.fct.ualg.pt 24 February 2010 thanks to Paulo

More information

To determine the wavelength of laser light using single slit diffraction

To determine the wavelength of laser light using single slit diffraction 9 To determine the wavelength of laser light using single slit diffraction pattern 91 Apparatus: Helium-Neon laser or diode laser, a single slit with adjustable aperture width, optical detector and power

More information

Section Parametrized Surfaces and Surface Integrals. (I) Parametrizing Surfaces (II) Surface Area (III) Scalar Surface Integrals

Section Parametrized Surfaces and Surface Integrals. (I) Parametrizing Surfaces (II) Surface Area (III) Scalar Surface Integrals Section 16.4 Parametrized Surfaces and Surface Integrals (I) Parametrizing Surfaces (II) Surface Area (III) Scalar Surface Integrals MATH 127 (Section 16.4) Parametrized Surfaces and Surface Integrals

More information

Experiment 8 Wave Optics

Experiment 8 Wave Optics Physics 263 Experiment 8 Wave Optics In this laboratory, we will perform two experiments on wave optics. 1 Double Slit Interference In two-slit interference, light falls on an opaque screen with two closely

More information

FINDING THE INDEX OF REFRACTION - WebAssign

FINDING THE INDEX OF REFRACTION - WebAssign Name: Book: Period: Due Date: Lab Partners: FINDING THE INDEX OF REFRACTION - WebAssign Purpose: The theme in this lab is the interaction between light and matter. Matter and light seem very different

More information

LIGHT: Two-slit Interference

LIGHT: Two-slit Interference LIGHT: Two-slit Interference Objective: To study interference of light waves and verify the wave nature of light. Apparatus: Two red lasers (wavelength, λ = 633 nm); two orange lasers (λ = 612 nm); two

More information

Physics 210 Medical Physics Midterm Exam Fall 2012 October 12, 2012

Physics 210 Medical Physics Midterm Exam Fall 2012 October 12, 2012 Physics 210 Medical Physics Midterm Exam Fall 2012 October 12, 2012 Name Problem 1 /32 Problem 2 /32 Problem 3 /24 Total /88 I affirm that I have carried out my academic endeavors with full academic honesty.

More information

MODELING OF THREE-DIMENSIONAL PROPAGATION ON A COASTAL WEDGE WITH A SEDIMENT SUPPORTING SHEAR

MODELING OF THREE-DIMENSIONAL PROPAGATION ON A COASTAL WEDGE WITH A SEDIMENT SUPPORTING SHEAR MODELING OF THREE-DIMENSIONAL PROPAGATION ON A COASTAL WEDGE WITH A SEDIMENT SUPPORTING SHEAR Piotr Borejko Vienna University of Technology, Karlsplatz 13/E26/3, 14 Vienna, Austria Fax: + 43 1 588 1 21

More information

LIGHT. Speed of light Law of Reflection Refraction Snell s Law Mirrors Lenses

LIGHT. Speed of light Law of Reflection Refraction Snell s Law Mirrors Lenses LIGHT Speed of light Law of Reflection Refraction Snell s Law Mirrors Lenses Light = Electromagnetic Wave Requires No Medium to Travel Oscillating Electric and Magnetic Field Travel at the speed of light

More information

Physical Optics. You can observe a lot just by watching. Yogi Berra ( )

Physical Optics. You can observe a lot just by watching. Yogi Berra ( ) Physical Optics You can observe a lot just by watching. Yogi Berra (1925-2015) OBJECTIVES To observe some interference and diffraction phenomena with visible light. THEORY In a previous experiment you

More information

Control of Light. Emmett Ientilucci Digital Imaging and Remote Sensing Laboratory Chester F. Carlson Center for Imaging Science 8 May 2007

Control of Light. Emmett Ientilucci Digital Imaging and Remote Sensing Laboratory Chester F. Carlson Center for Imaging Science 8 May 2007 Control of Light Emmett Ientilucci Digital Imaging and Remote Sensing Laboratory Chester F. Carlson Center for Imaging Science 8 May 007 Spectro-radiometry Spectral Considerations Chromatic dispersion

More information

Electricity & Optics

Electricity & Optics Physics 24100 Electricity & Optics Lecture 27 Chapter 33 sec. 7-8 Fall 2017 Semester Professor Koltick Clicker Question Bright light of wavelength 585 nm is incident perpendicularly on a soap film (n =

More information

Ripple Tank. Refraction and Dispersion

Ripple Tank. Refraction and Dispersion Ripple Tank Refraction and Dispersion There is a distinct relationship between frequency, wave velocity, and wavelength. If you know any two, you can determine the third simply by using the formula v =

More information

newfasant US User Guide

newfasant US User Guide newfasant US User Guide Software Version: 6.2.10 Date: April 15, 2018 Index 1. FILE MENU 2. EDIT MENU 3. VIEW MENU 4. GEOMETRY MENU 5. MATERIALS MENU 6. SIMULATION MENU 6.1. PARAMETERS 6.2. DOPPLER 7.

More information

3. For an incoming ray of light vacuum wavelength 589 nm, fill in the unknown values in the following table.

3. For an incoming ray of light vacuum wavelength 589 nm, fill in the unknown values in the following table. Homework Set 15A: Mirrors and Lenses 1. Find the angle of refraction for a ray of light that enters a bucket of water from air at an angle of 25 degrees to the normal. 2. A ray of light of vacuum wavelength

More information

Single-point current meter designed for very long-term deployments

Single-point current meter designed for very long-term deployments Single-point current meter designed for very long-term deployments With all the features and capabilities of the standard Aquadopp, the deepwater current meter has been used and proven by oceanographers

More information

Lecture 39. Chapter 37 Diffraction

Lecture 39. Chapter 37 Diffraction Lecture 39 Chapter 37 Diffraction Interference Review Combining waves from small number of coherent sources double-slit experiment with slit width much smaller than wavelength of the light Diffraction

More information

Chapter 26 Geometrical Optics

Chapter 26 Geometrical Optics Chapter 26 Geometrical Optics 26.1 The Reflection of Light 26.2 Forming Images With a Plane Mirror 26.3 Spherical Mirrors 26.4 Ray Tracing and the Mirror Equation 26.5 The Refraction of Light 26.6 Ray

More information

Which row could be correct for the colours seen at X, at Y and at Z?

Which row could be correct for the colours seen at X, at Y and at Z? 1 The ray diagram shows the image of an formed by a converging lens. converging lens image 50 cm What is the focal length of the lens? 40 cm 72 cm 40 cm 50 cm 72 cm 90 cm 2 The diagram shows the dispersion

More information

Polarized Downwelling Radiance Distribution Camera System

Polarized Downwelling Radiance Distribution Camera System Polarized Downwelling Radiance Distribution Camera System Kenneth J. Voss Physics Department, University of Miami Coral Gables, Fl. 33124 phone: (305) 284-2323 ext 2 fax: (305) 284-4222 email: voss@physics.miami.edu

More information

Model REEF-SS ASF-200

Model REEF-SS ASF-200 1 Femtosecond Single Shot Autocorrelator Model REEF-SS ASF-200 INSTRUCTION MANUAL 4119 Twilight Ridge, San Diego, CA 92130 USA Tel::858.876.3133 Fax::858.630.2376 2 The Single Shot Autocorrelator (SSA)

More information

Textbook Assignment #1: DUE Friday 5/9/2014 Read: PP Do Review Questions Pg 388 # 1-20

Textbook Assignment #1: DUE Friday 5/9/2014 Read: PP Do Review Questions Pg 388 # 1-20 Page 1 of 38 Page 2 of 38 Unit Packet Contents Unit Objectives Notes 1: Waves Introduction Guided Practice: Waves Introduction (CD pp 89-90) Independent Practice: Speed of Waves Notes 2: Interference and

More information

University Physics (Prof. David Flory) Chapt_37 Monday, August 06, 2007

University Physics (Prof. David Flory) Chapt_37 Monday, August 06, 2007 Name: Date: 1. If we increase the wavelength of the light used to form a double-slit diffraction pattern: A) the width of the central diffraction peak increases and the number of bright fringes within

More information

GLOBAL navigation satellite system reflectometry

GLOBAL navigation satellite system reflectometry 1064 IEEE GEOCIENCE AND REMOTE ENING LETTER, VOL. 13, NO. 8, AUGUT 2016 On the patial Resolution of GN Reflectometry Maria Paola Clarizia, Member, IEEE, and Christopher. Ruf, Fellow, IEEE Abstract A method

More information

PSI Precision, accuracy and validation aspects

PSI Precision, accuracy and validation aspects PSI Precision, accuracy and validation aspects Urs Wegmüller Charles Werner Gamma Remote Sensing AG, Gümligen, Switzerland, wegmuller@gamma-rs.ch Contents Aim is to obtain a deeper understanding of what

More information

Chapter 38 Wave Optics (II)

Chapter 38 Wave Optics (II) Chapter 38 Wave Optics (II) Initiation: Young s ideas on light were daring and imaginative, but he did not provide rigorous mathematical theory and, more importantly, he is arrogant. Progress: Fresnel,

More information

Downloaded from UNIT 06 Optics

Downloaded from   UNIT 06 Optics 1 Mark UNIT 06 Optics Q1: A partially plane polarised beam of light is passed through a polaroid. Show graphically the variation of the transmitted light intensity with angle of rotation of the Polaroid.

More information

Fig The light rays that exit the prism enter longitudinally into an astronomical telescope adjusted for infinite distance.

Fig The light rays that exit the prism enter longitudinally into an astronomical telescope adjusted for infinite distance. Romanian Master of Physics 07 Problem I Reflection and refraction of light A. An interesting prism The main section of a glass prism, situated in air n '.00, has the form of a rhomb with. A thin yellow

More information

Light and refractive index

Light and refractive index 17 Fig. 7.1 shows a ray of light incident on a rectangular glass block at point X. W P X air glass Q R S Fig. 7.1 The ray of light is refracted at X. On Fig. 7.1, (a) draw the normal at X, [1] (b) draw

More information

Advanced modelling of gratings in VirtualLab software. Site Zhang, development engineer Lignt Trans

Advanced modelling of gratings in VirtualLab software. Site Zhang, development engineer Lignt Trans Advanced modelling of gratings in VirtualLab software Site Zhang, development engineer Lignt Trans 1 2 3 4 Content Grating Order Analyzer Rigorous Simulation of Holographic Generated Volume Grating Coupled

More information

Th LHR5 08 Multi-modal Surface Wave Inversion and Application to North Sea OBN Data

Th LHR5 08 Multi-modal Surface Wave Inversion and Application to North Sea OBN Data Th LHR5 08 Multi-modal Surface Wave Inversion and pplication to North Sea ON Data S. Hou (CGG), D. Zheng (CGG), X.G. Miao* (CGG) & R.R. Haacke (CGG) SUMMRY Surface-wave inversion (SWI) for S-wave velocity

More information

Review of Trigonometry

Review of Trigonometry Worksheet 8 Properties of Trigonometric Functions Section Review of Trigonometry This section reviews some of the material covered in Worksheets 8, and The reader should be familiar with the trig ratios,

More information

MICHELSON S INTERFEROMETER

MICHELSON S INTERFEROMETER MICHELSON S INTERFEROMETER Objectives: 1. Alignment of Michelson s Interferometer using He-Ne laser to observe concentric circular fringes 2. Measurement of the wavelength of He-Ne Laser and Na lamp using

More information

Interference Effects. 6.2 Interference. Coherence. Coherence. Interference. Interference

Interference Effects. 6.2 Interference. Coherence. Coherence. Interference. Interference Effects 6.2 Two-Slit Thin film is a general property of waves. A condition for is that the wave source is coherent. between two waves gives characteristic patterns due to constructive and destructive.

More information

Waves-Refraction. 5. A change in the speed of a wave as it enters a new medium produces a change in 1. frequency 2. period 3. wavelength 4.

Waves-Refraction. 5. A change in the speed of a wave as it enters a new medium produces a change in 1. frequency 2. period 3. wavelength 4. 1. In which way does blue light change as it travels from diamond into crown glass? 1. Its frequency decreases. 2. Its frequency increases. 3. Its speed decreases. 4. Its speed increases. Base your answers

More information

The sources must be coherent. This means they emit waves with a constant phase with respect to each other.

The sources must be coherent. This means they emit waves with a constant phase with respect to each other. CH. 24 Wave Optics The sources must be coherent. This means they emit waves with a constant phase with respect to each other. The waves need to have identical wavelengths. Can t be coherent without this.

More information

ISAR IMAGING OF MULTIPLE TARGETS BASED ON PARTICLE SWARM OPTIMIZATION AND HOUGH TRANSFORM

ISAR IMAGING OF MULTIPLE TARGETS BASED ON PARTICLE SWARM OPTIMIZATION AND HOUGH TRANSFORM J. of Electromagn. Waves and Appl., Vol. 23, 1825 1834, 2009 ISAR IMAGING OF MULTIPLE TARGETS BASED ON PARTICLE SWARM OPTIMIZATION AND HOUGH TRANSFORM G.G.Choi,S.H.Park,andH.T.Kim Department of Electronic

More information

first name (print) last name (print) brock id (ab17cd) (lab date)

first name (print) last name (print) brock id (ab17cd) (lab date) (ta initials) first name (print) last name (print) brock id (ab17cd) (lab date) Experiment 3 Refraction of light In this Experiment you will learn that the bending of light crossing the boundary of two

More information

Capturing light. Source: A. Efros

Capturing light. Source: A. Efros Capturing light Source: A. Efros Review Pinhole projection models What are vanishing points and vanishing lines? What is orthographic projection? How can we approximate orthographic projection? Lenses

More information

Reflectance & Lighting

Reflectance & Lighting Reflectance & Lighting Computer Vision I CSE5A Lecture 6 Last lecture in a nutshell Need for lenses (blur from pinhole) Thin lens equation Distortion and aberrations Vignetting CS5A, Winter 007 Computer

More information

Wave Hydro Dynamics Prof. V. Sundar Department of Ocean Engineering Indian Institute of Technology, Madras

Wave Hydro Dynamics Prof. V. Sundar Department of Ocean Engineering Indian Institute of Technology, Madras Wave Hydro Dynamics Prof. V. Sundar Department of Ocean Engineering Indian Institute of Technology, Madras Module No. # 06 Wave Theories and Testing Facilities Lecture No. # 01 Finite Amplitude Wave Theories

More information

Physics 11 - Waves Extra Practice Questions

Physics 11 - Waves Extra Practice Questions Physics - Waves xtra Practice Questions. Wave motion in a medium transfers ) energy, only ) mass, only. both mass and energy. neither mass nor energy. single vibratory disturbance that moves from point

More information

Lasers PH 645/ OSE 645/ EE 613 Summer 2010 Section 1: T/Th 2:45-4:45 PM Engineering Building 240

Lasers PH 645/ OSE 645/ EE 613 Summer 2010 Section 1: T/Th 2:45-4:45 PM Engineering Building 240 Lasers PH 645/ OSE 645/ EE 613 Summer 2010 Section 1: T/Th 2:45-4:45 PM Engineering Building 240 John D. Williams, Ph.D. Department of Electrical and Computer Engineering 406 Optics Building - UAHuntsville,

More information

SAFT DATA PROCESSING APPLIED TO LASER-ULTRASONIC INSPECTION

SAFT DATA PROCESSING APPLIED TO LASER-ULTRASONIC INSPECTION SAFT DATA PROCESSING APPLIED TO LASER-ULTRASONIC INSPECTION A. Blouin, D. Levesque, C. Neron, F. Enguehard, D. Drolet, and I-P. Monchalin National Research Council of Canada, Industrial Materials Institute,

More information

The influence of coherent waves on the remotely sensed reflectance

The influence of coherent waves on the remotely sensed reflectance The influence of coherent waves on the remotely sensed reflectance J. Ronald V. Zaneveld and Emmanuel Boss College of Ocean and Atmospheric Sciences, Oregon State University, Corvallis OR 97330 zaneveld@oce.orst.edu,

More information

PHYS 3410/3411/6750/6751: Modern Optics Midterm #2

PHYS 3410/3411/6750/6751: Modern Optics Midterm #2 Name: PHYS 3410/3411/6750/6751: Modern Optics Midterm #2 Wednesday 17 November 2010 Prof. Bolton Only pen or pencil are allowed. No calculators or additional materials. PHYS 3410/3411/6750/6751 Midterm

More information

Memorandum. Clint Slatton Prof. Brian Evans Term project idea for Multidimensional Signal Processing (EE381k)

Memorandum. Clint Slatton Prof. Brian Evans Term project idea for Multidimensional Signal Processing (EE381k) Memorandum From: To: Subject: Date : Clint Slatton Prof. Brian Evans Term project idea for Multidimensional Signal Processing (EE381k) 16-Sep-98 Project title: Minimizing segmentation discontinuities in

More information

D&S Technical Note 09-2 D&S A Proposed Correction to Reflectance Measurements of Profiled Surfaces. Introduction

D&S Technical Note 09-2 D&S A Proposed Correction to Reflectance Measurements of Profiled Surfaces. Introduction Devices & Services Company 10290 Monroe Drive, Suite 202 - Dallas, Texas 75229 USA - Tel. 214-902-8337 - Fax 214-902-8303 Web: www.devicesandservices.com Email: sales@devicesandservices.com D&S Technical

More information

UNIT VI OPTICS ALL THE POSSIBLE FORMULAE

UNIT VI OPTICS ALL THE POSSIBLE FORMULAE 58 UNIT VI OPTICS ALL THE POSSIBLE FORMULAE Relation between focal length and radius of curvature of a mirror/lens, f = R/2 Mirror formula: Magnification produced by a mirror: m = - = - Snell s law: 1

More information

Physics 123 Optics Review

Physics 123 Optics Review Physics 123 Optics Review I. Definitions & Facts concave converging convex diverging real image virtual image real object virtual object upright inverted dispersion nearsighted, farsighted near point,

More information

UNSTEADY FLOW IN OPEN CHANNELS

UNSTEADY FLOW IN OPEN CHANNELS UNSTEADY FLOW IN OPEN CHANNELS Definition in free surface flow of water is classified as steady or unsteady flow. The flow of water in rivers, canals, reservoirs, lakes, pools, and free- surface flow in

More information

WavesMon v3.08 User s Guide

WavesMon v3.08 User s Guide WavesMon v3.08 User s Guide P/N 957-6232-00 (November 2011) 2011 Teledyne RD Instruments, Inc. All rights reserved. Table of Contents 1 Introduction... 1 1.1 How to Contact Teledyne RD Instruments... 1

More information

Stevens High School AP Physics II Work for Not-school

Stevens High School AP Physics II Work for Not-school 1. Gravitational waves are ripples in the fabric of space-time (more on this in the next unit) that travel at the speed of light (c = 3.00 x 10 8 m/s). In 2016, the LIGO (Laser Interferometry Gravitational

More information

Th ELI1 12 Joint Crossline Reconstruction and 3D Deghosting of Shallow Seismic Events from Multimeasurement Streamer Data

Th ELI1 12 Joint Crossline Reconstruction and 3D Deghosting of Shallow Seismic Events from Multimeasurement Streamer Data Th ELI1 12 Joint Crossline Reconstruction and 3D Deghosting of Shallow Seismic Events from Multimeasurement Streamer Data Y.I. Kamil* (Schlumberger), M. Vassallo (Schlumberger), W. Brouwer (Schlumberger),

More information

Interference of Light

Interference of Light Interference of Light Review: Principle of Superposition When two or more waves interact they interfere. Wave interference is governed by the principle of superposition. The superposition principle says

More information

Phys 102 Lecture 17 Introduction to ray optics

Phys 102 Lecture 17 Introduction to ray optics Phys 102 Lecture 17 Introduction to ray optics 1 Physics 102 lectures on light Light as a wave Lecture 15 EM waves Lecture 16 Polarization Lecture 22 & 23 Interference & diffraction Light as a ray Lecture

More information

Interference. Electric fields from two different sources at a single location add together. The same is true for magnetic fields at a single location.

Interference. Electric fields from two different sources at a single location add together. The same is true for magnetic fields at a single location. Interference Electric fields from two different sources at a single location add together. The same is true for magnetic fields at a single location. Thus, interacting electromagnetic waves also add together.

More information

Chapter 32 Light: Reflection and Refraction. Copyright 2009 Pearson Education, Inc.

Chapter 32 Light: Reflection and Refraction. Copyright 2009 Pearson Education, Inc. Chapter 32 Light: Reflection and Refraction Units of Chapter 32 The Ray Model of Light Reflection; Image Formation by a Plane Mirror Formation of Images by Spherical Mirrors Index of Refraction Refraction:

More information