Purpose  To analyze, through theoretical and experimental methods, the relative luminescence of a series of images produced by multiple reflections in.

Slides:



Advertisements
Similar presentations
Interference and Diffraction
Advertisements

The Wave Nature of Light
Diffraction and Interference Physics Light Light has Wave properties Light can Diffract Light can Interfere – Constructively – Destructively.
AP Physics Mr. Jean March 30 th, The plan: Review of slit patterns & interference of light particles. Quest Assignment #2 Polarizer More interference.
Introduction Secondary electron secondary electron detector The electron beam interaction with near surface specimen atoms will make a signal which results.
Chapter 24 Wave Optics.
Lecture 15 Interference Chp. 36 Opening Demo Topics –Interference is due to the wave nature of light –Hyugens principle, Coherence –Change in wavelength.
1 Laser Beam Coherence Purpose: To determine the frequency separation between the axial modes of a He-Ne Laser All sources of light, including lasers,
Radiator study status Y. Horii, Y. Koga, N. Kiribe, … (Nagoya University, Japan) 1 B2GM, 6 th July.
Copyright © 2009 Pearson Education, Inc. Chapter 32 Light: Reflection and Refraction.
Diffraction through a single slit
Modern Optics Lab Lab 5 Part 1: Experiments involving Light Polarization  Measuring light transmission through a dichroic material (“polarizer sheet”)
Chapter 37 - Interference and Diffraction
Results Theory Abstract Evaluation of Scintillation Index and Intensity of Partially Coherent Laser Light MIDN 4/C Meredith L. Lipp and MIDN 4/C Kathryn.
Two identical resistors are wired in series. An electrical current runs through the combination. If the current through the first resistor is I 1, then.
An unpolarized beam of light is incident on a pane of glass (n = 1
Chapter 7 Light.
It is against the honor code to “click” for someone else-violators will loose all clicker pts. HITT RF Remote Login Procedure: 1. PRESS AND HOLD THE DOWN.
Applying Colour Theory to Visual Design.  Color Theory is the art of mixing colors to achieve desired effects.  The way colors are combined can be used.
Review Questions – Unit What happens when red light shines on a prism? a. it changes the color of the light into blue and green b. it changes the.
Lesson#23 Topic: Simple Circuits Objectives: (After this class I will be able to) 1. Explain the difference between wiring light bulbs in series and in.
To view the slide show with animations Press F5 on the top of the keyboard Security Alert – press OK (we have checked the photos) Then to step forwards.
Mirror and Lens Notes.
Light and Optics.
Spectrophotometer Prof.Dr. Moustafa M. Mohamed Vice Dean Faculty of Allied Medical Science Pharos University in Alexandria, EGYPT.
Reading Quiz Light can be polarized because:
1 Atomic Absorption Spectroscopy Lecture Emission in Flames There can be significant amounts of emission produced in flames due to presence of flame.
Diffraction is the bending of waves around obstacles or the edges of an opening. Huygen’s Principle - Every point on a wave front acts as a source of tiny.
Interference Applications Physics 202 Professor Lee Carkner Lecture 25.
Interference in Thin Films, final
Thin Film Interference II. Thin Film Whiteboard I! White light is incident upon a type I thin film from above, as shown below. Then, the thickness of.
Ch 16 Interference. Diffraction is the bending of waves around obstacles or the edges of an opening. Huygen’s Principle - Every point on a wave front.
ResourcesChapter menu Bellringer What do you think light is? Is light made of matter? Can light travel through space? Explain your answers in your lab.
Light at a Distance Jessica, Charlie, Courtney, and Ashley.
Lecture 24 Interference of Light.
Text book pages Do 7.1 – 7.3 in your workbooks
Physics 1C Lecture 27A. Interference Treating light as a particle (geometrical optics) helped us to understand how images are formed by lenses and mirrors.
Higher Physics – Unit Waves. a a λ λ crest trough Wave Theory All waves transmit energy. The energy of a wave depends on its amplitude. a = amplitude.
Conditions for Interference
Version 0.10 (c) 2007 CELEST VISI  N BRIGHTNESS CONTRAST CLASSROOM PRESENTATION PRE-EXPERIMENT How many black dots can you count?
Like other waves, light waves can add constructively and destructively as shown above. Examples: –Colors seen in soap bubbles –Colors seen in a thin film.
Reading Quiz Sometimes a thin layer of oil on top of a puddle of water produces a rainbow pattern of colors. This is a result of: the interference properties.
Radiative forcing of climate by historical land cover change H. Damon Matthews, Andrew J. Weaver, Michael Eby, and Katrin J. Meissner Cory Martin Atmospheric.
Physical optics Done by P G LOGAN. Physical optics Physical optics deals with phenomena that depend on the wave nature of light. There are three types.
Physics 102: Lecture 21, Slide 1 Diffraction, Gratings, Resolving Power Physics 102: Lecture 21.
Basics Reflection Mirrors Plane mirrors Spherical mirrors Concave mirrors Convex mirrors Refraction Lenses Concave lenses Convex lenses.
Series and Parallel Circuits
Chapter 24 Wave Optics. Young’s Double Slit Experiment Thomas Young first demonstrated interference in light waves from two sources in Light is.
Chapter 16 Fundamentals of Light Understand sources of light and how light illuminates the universe around us. Chapter 16 In this chapter you will:
Chemical Effects The energy of light can chemically change the surfaces of materials absorbing it. Light changes the chemistry of the eye’s retina, so.
Intro Video: Interference of Waves Questions From Reading Activity?
LONGITUDINAL COUPLED-BUNCH OSCILLATIONS IN THE RECYCLER RING PRESENTED BY: MUHED RANA UNIVERSITY OF MARYLAND, BALTIMORE COUNTY (UMBC), BALTIMORE, MD SUPERVISOR:
LIGHT BASICS. Illumination The human eye can detect changes in size, brightness, position, color of an object. We can tell the difference between shadows.
Version 0.10 (c) 2007 CELEST VISI  N BRIGHTNESS CONTRAST CLASSROOM PRESENTATION PRE-EXPERIMENT How many black dots can you count?
Properties of Light GLY 4200 Fall, 2017.
Mrs. Gilford’s Art Class
FRAUNHOFFER DIFFRACTION AT DOUBLE SLIT
Voltage Divider.
Phys102 Lecture 25 The Wave Nature of Light; Interference
Primary and secondary light
Reflection, Transmission, Absorption, part 2
Phys102 Lecture 25 The Wave Nature of Light; Interference
Interference.
Volume 34, Issue 5, Pages (May 2002)
Experiment Report Format
Volume 34, Issue 5, Pages (May 2002)
Diffraction and Interference
Key Areas covered Irradiance and the inverse square law.
Voltage Divider.
Presentation transcript:

Purpose  To analyze, through theoretical and experimental methods, the relative luminescence of a series of images produced by multiple reflections in a decorative glass lamp The number of visible images can be used to measure the sensitivity range of the eye

Background  Glass oil lamp from Curry Club Restaurant, East Setauket  Inner walls of the glass have a partially reflective coating  Dimensions: 6.5in x 3in x 3in  Glass walls are 0.25in thick and have a brown tint 6.5 in 3 in 0.25 in 11 images

Background (cont.) 2nd image 3rd image 4th image  When the flame is viewed at eye level, a series of flame images can be seen  Each consecutive image is dimmer than the last and images can be seen in a dark room  The nth image is produced by n-1 reflections  The reflectance of the inner wall determines the relative brightness of the image 1st image Top View

Procedure - Part 1 Outer Surface Inner Surface  An He-Ne laser and a photo detector were used to measure I 1, I 2, I 3, and I 4 to calculate the reflectance of the inner and outer surface and the absorption (t)  Incoming light split between absorption, reflection, and transmission I1I1 I4I4 I2I2 I3I3 I5I5 I6I6 I7I7 I8I8 R o = I 2 / I 1 R i = I 7 / I 6 t = I 6 / I 5

Measured Intensity Values First Run Second Run Ratio*Average I1I1 245 mA mA I2I2 7.9 mA mA I3I μA μA I4I μA μA * Ratio of second run to first run. The second run values are lower because the laser power decreased after warm-up but are consistent with the first run.

 The values of R i, R o, and t were derived from a set of equations that contained the measured values of I 1, I 2, I 3, and I 4.  t = 1-a and a = absorption ratio  I 5 = I 1 - I 2  I 6 = t*I 5 = t*(I 1 - I 2 )  I 7 = I 6 - I 3 = t*(I 1 - I 2 )-I 3  I 8 = t*I 7 = I 4 + I 8 *(I 2 /I 1 )  t 2 *(I 1 - I 2 )-t*I 3 - I 4 /(1 - (I 2 /I 1 )) = 0  R o = I 2 /I 1  R i = I 7 /I 6 = 1 - I 3 /(t*(I 1 - I 2 )) Analysis and Results Results: R o = 3.2% t = 40.8% R i = 42.5%

Procedure - Part 2  Laser beam allowed to travel through the lamp  5 visible spots  Photo detector used to measure their intensities in Volts using a 100 kΩ resistor & iris used to isolate the images  The ratio of the spot intensities is R i 2  R i 2 = % Laser Lamp 5 spots of decreasing intensity IrisPhoto Detector

Discussion / Conclusion  The reflectance of the inner surface of the glass lamp (R i ) equals the relative luminescence between the flame images  R i was measured using two independent methods and the 2 values are in very good agreement  R i = 43.0 ± 0.5%  This value predicts the relative luminescence of the candle flame as shown in the graph below  The nth image is approximately (0.43) n times as bright as the first image  The 11 th image is 10, 760 times brighter than the first  Therefore, the human eye can perceive a range of about 10,000 in intensity at a single instant

Future Study  Testing human visual sensitivity  Determining an optimum reflection-transmittance ratio (applications for sunglasses, tinted glass, etc.)  Analyzing or designing “one-way” mirrors  Analyzing laser cavities