Dispersive power. of Prism
|
|
- Raymond York
- 6 years ago
- Views:
Transcription
1 Dispersive power of Pris 1
2 Dispersive Power of Pris Experient No. Object : To deterine the dispersive power of the aterial of a pris by spectroeter. Apparatus : Spectroeter, pris, spirit level, reading lens and ercury lap. Forula : Where The dispersive power of the aterial of a pris is given by v 1) efractive index of the aterial of a pris for extree violet colour V efractive index of the aterial of a pris for extree red colour efractive index of the aterial of a pris for yellow (ean) colour position. efractive index is given by sin( A ) / 2 sin( A/ 2) Where A Angle of pris Angle of iniu deviation Procedure : To obtain pure spectru by spectroeter the following adjustents ust be ade : The axis of the telescope and that of colliator sut intersect the central axis of rotation of telescope. 2
3 The pris table is leveled with the help of spirit level. The slit of the colliator is ade narrow, vertical and syetrical on both sides. Note the lest count of vernier scales. Adjustent of the telescope. i) Turn the telescope towards a white wall and the distance between its objective and the eyepiece is so adjusted that the field of view becoes copletely luinous. Now the eyepiece is displaced inside the tube till the cross-wire becoes distinctly visible. ii) Now the telescope with objective is directed towards a distant tree or pole and they are viewed through the telescope. The distance between the objective and the eye piece is adjusted with the help of rack and pinion arrangeent such that a distinct and clear iage of the object is seen. Thus the telescope is ready to focus all the parallel rays at the cross wire. Adjustent of Colliator : Place the ercury lap in front of the slit of colliator and align the telescope with the colliator such that the iage of the slit is seen through telescope. Thej distance between the slit and the lens of the colliator is adjusted with the help of its rack and pinion arrangeent until a distinct iage is seen through the telescope. In this position the light rays coing out of the colliator will be parallel to each other. Adjustent of Pris table : The height of the pris table is adjusted in such a way that the light rays coing out of the colliator fall axiu on the refracting surface of the pris when it is placed on the pris table. Schuster s ethod : There is another ethod of adjusting the telescope and the colliator for parallel rays. This ethod is called Schuster s ethod. The ethod is as follows : i) First of all pris table is adjusted at the sae height of the colliator and telescope. ii) iii) iv) Now the pris is placed on the pris table in such a position that its one of the refracting surface faces the colliator. The light eerging fro the other refracting surface of the pris is viewed through the telescope. The pris table and the telescope both are then rotated slowly and siultaneously so that the spectral lines always reain the cross-wire. A state is reached when on rotating the pris table further, the direction of rotation of the spectral lines reserved. This position is the position of iniu deviation. Now, keeping the telescope fixed, the pris table is rotated through a sall angle. The spectral lines are seen to be blurred. The telescope is adjusted with the help of rack and pinion arrangeent so that spectral lines becoe distinct and clear. v) table is rotated through a sall angle in the colliator is adjusted with the help of a rack and pinion arrangeent so that spectral lines becoe distinct and clear. 3
4 vi) The ethod described in steps (iv) and (v) are repeated attain and again till the spectral lines becoe distinct and clear through out the entire rotation of the telescope. In this position the spectroeter will be set for parallel rays coing out of the colliator, focusing parallel rays by telescope at its cross-wire and the pris in the position of angle of iniu deviation. Measureent of the angle of iniu deviation : i) Follow the procedure as given in steps (i), (ii), and (iii) of the Schuster s ethod. ii) iii) iv) Now fix the vertical cross-wire on one of the extree spectral line of the spectru with the help of tangent screw of the telescope. Note the reading of both the verniers on the ain scale. Siilarly fix the vertical cross wire on the ean line (yellow line) and extree spectral line on the other end of the spectru and in each position note the reading of both the verniers on the ain scale. The position of the pris table is kept fixed and the pris is reoved. The telescope is rotated till the direct iage of the slit is viewed at its vertical cross-wire. The position of the telescope is noted by the reading of both the verniers. v) The difference of readings in steps (ii), (iii) with (iv) is calculated for both the circular verniers. The ean of these two differences will be angle of iniu deviation. Measureent of the angle of Pris A : i) Place the pris on the pris table with its angle of pris A towards the colliator and with its refracting edge A at its centre. In this position soe of the light falling on each refracting surface AB and AC will be reflected and can be received by the telescope. ii) iii) iv) The telescope is oved to one side to receive the light reflected fro the refracting surface AB and the iage of the slit is focused at the vertical cross-wire. The reading of two verniers are noted on the ain scale. Now the telescope is oved to another side to receive the light reflected fro the refracting surface AD and the iage of slit is focused again at the vertical cross-wire. The reading of two verniers are noted again on the ain scale. The difference of readings in steps (ii) and (iii) is calculated for both the verniers. The ean of these two differences will be twice the angle of pris. Therefore, half of this angle gives the angle of pris. The refractive index and then dispersive power of the pris are calculated fro these observations. 4
5 Figure: Observations : One division of ain scale x.. Nuber of vernier divisions n.. Least count of the vernier n x.. For iniu deviation : eading in the S.No. Colour Circular Scale iniu deviation position 1. ed V 1 2. ellow V 1 3. Violet V 1 eading in the position of direct iage.s. c.s. Total a.s. c.s. Total b a - b Mean 5
6 S.No. For Angle of Pris A : eading for eading for reflection Vernier eflection fro face fro fact AC AB.s. c.s. Total a.s. c.s. Total a Difference a - b Mean Value 2A Mean Value A 1. V 1 2. V 1 Calculation : Angle of pris A Angle of iniu deviation for extree violet colour V sin( A ) / 2 for violet V sin A / 2 Angle of iniu deviation for extree red colour for ed sin( A ) / 2 sin A / 2 Angle of iniu deviation for extree red colour sin( A ) / 2 for ellow sin A / 2 Dispersive power of aterial of a pris V a esult : The dispersive power of aterial of a pris Standard value for the flint glass Crown Glass % error Sources of Error : The slit ay not be vertical and narrow. The edge of slit and pris ay not be perfectly vertical. The axis of rotation of the telescope ay not pass through the centre of circular scale. While taking observations, telescope and pris table are not fixed. 6
7 Pris is not clean. Precautions : The slit should be as narrow as possible but the knife edge s of the slit should not touch each other. The telescope and the colliator should be separately set for parallel rays. The height of the pris table should be so adjusted that the axiu light ust fall on the entire surface of the pris. While taking observations the telescope and the pris table ust be claped. The reading lens should be used for taking readings on both the verniers. Viva-Voce : What is the use of collilator in the spectroeter? The colliator akes the light rays coing fro the light source parallel to each other. Why are lines and circles drawn on the pris table? For placing the grating or pris properly on the pris table. Why do you take readings fro both the verniers? This is done in order to eliinate the error arising due to non coincidence of the axis of rotation of the pris table or the telescope with the centre of the circular ain scale. * * * 7
8 8
Determination of Cauchy s Contants
8. Determination of Cauchy s Contants 8.1 Objective: To determine Cauchy s Constants using a prism and spectrometer. Apparatus: Glass prism, spectrometer and mercury vapour lamp. 8. Theory: The wavelength
More informationEXPERIMENT NO. 6. OBJECT: To determine the wavelength of any three lines of mercury light by diffraction grating in1 st and 2 nd order spectrum.
EXPEIMENT NO. 6 OBJECT: To determine the wavelength of any three lines of mercury light by diffraction grating in1 st and 2 nd order spectrum. APPAATUS: A diffraction grating, Spectrometer, spirit level,
More informationTHE DIFFRACTION GRATING SPECTROMETER
Purpose Theory THE DIFFRACTION GRATING SPECTROMETER a. To study diffraction of light using a diffraction grating spectrometer b. To measure the wavelengths of certain lines in the spectrum of the mercury
More informationTo determine the wavelengths of light emitted by a mercury vapour lamp by using a diffraction grating.
12. Diffraction grating OBJECT To determine the wavelengths of light emitted by a mercury vapour lamp by using a diffraction grating. INTRODUCTION: Consider a light beam transmitted through an aperture
More informationDISPERSION OF A GLASS PRISM
PH2 page 1 DISPERSION OF A GLASS PRISM OBJECTIVE The objective of this experiment is to analyze the emission spectrum of helium and to analyze the dispersion of a glass prism by measuring the index of
More informationEXPERIMENT NO. 8. OBJECT: To determine the wavelength of sodium light by method.
EXPERIMENT NO. 8 OBJECT: To determine the wavelength of sodium light by method. Fresnel s APPARATUS: Optical bench with four uprights, a sodium lamp, Fresnel s, a convex lens and micrometer eyepiece. DIAGRAM:
More informationDispersion of light by a prism
Dispersion of light by a prism Aim: (i) To calculate refractive index µ of a prism for various wavelengths (λ) of Hg and to find dispersive power of the material of the prism (ii) To plot µ-/λ curve and
More informationPh 3455/MSE 3255 Experiment 2: Atomic Spectra
Ph 3455/MSE 3255 Experiment 2: Atomic Spectra Background Reading: Tipler, Llewellyn pp. 163-165 Apparatus: Spectrometer, sodium lamp, hydrogen lamp, mercury lamp, diffraction grating, watchmaker eyeglass,
More informationDISPERSION AND SPECTRA CHAPTER 20
CHAPTER 20 DISPERSION AND SPECTRA 20.1 DISPERSION As mentioned earlier, the refractive index of a material depends slightly on the wavelength of light. The relation between the two may be approximately
More informationThe Quantum Model of the Hydrogen Atom
Physics 109 Science 1 Experiment 1 1 The Quantum Model of the Hydrogen Atom In this experiment you will use a spectrometer to determine the wavelengths of the visible lines of atomic hydrogen. The goal
More informationUNIT-5 EM WAVES UNIT-6 RAY OPTICS
UNIT-5 EM WAVES 2 Marks Question 1. To which regions of electromagnetic spectrum do the following wavelengths belong: (a) 250 nm (b) 1500 nm 2. State any one property which is common to all electromagnetic
More informationEXPERIMENT 5:Determination of the refractive index (µ) of the material of a prism using sprectometer
EXPERIMENT 5:Determination of the refractive index (µ) of the material of a prism using sprectometer Debangshu Mukherjee B.Sc Physics,1st year Chennai Mathematical Institute 17.10.008 1 Aim of Experiment
More informationChapter 4. Dispersion of Glass. 4.1 Introduction. 4.2 Apparatus
Chapter 4 Dispersion of Glass 4.1 Introduction This experiment will develop skills in choosing a suitable fit for data and plotting the resulting curve. Curve fitting will count for a big chunk of the
More informationPractical Physics "C"
The Islaic University of Gaza Faculty of Science Departent of Physics Practical Physics "C" PHYS 101 By Staff of Physics 01 1 Experient (1) Refraction of the Light and Snell's Law Objective 1. To verify
More informationDETERMINATION OF ELASTIC CONSTANTS CORNU S METHOD
DETEMINATION OF ELASTIC CONSTANTS CONU S METHOD Ai: To deterine the elastic constants of the given aterial by Cornu s interference ethod. Apparatus: A glass or perspe plate is placed syetrically on two
More informationExperiment #4: Optical Spectrometer and the Prism Deviation
Experiment #4: Optical Spectrometer and the Prism Deviation Carl Adams October 2, 2011 1 Purpose In the first part of this lab you will set up and become familiar with an optical spectrometer. In the second
More informationPhysics 24, Spring 2007 Lab 2 - Complex Spectra
Physics 24, Spring 2007 Lab 2 - Complex Spectra Theory The optical spectra of isolated atoms consist of discrete, unequally spaced lines. This fact could not be understood on the basis of classical atomic
More informationAtomic Spectra HISTORY AND THEORY
Atomic Spectra HISTORY AND THEORY When atoms of a gas are excited (by high voltage, for instance) they will give off light. Each element (in fact, each isotope) gives off a characteristic atomic spectrum,
More informationExperiment #5: Cauchy s Formula
Experiment #5: Cauchy s Formula Carl Adams October 14, 2011 1 Purpose This experiment is a continuation of Experiment #4. It is assumed you have an aligned spectrometer. 2 Safety/Protocol 1. The gas discharge
More informationWebreview - Ch 27 Quantum Physics Practice Test
Please do write on practice test. ID A Webreview - Ch 27 Quantu Physics Practice Test Multiple Choice Identify the choice that best copletes the stateent or answers the question. 1. Planck's quantu theory
More informationMA304 Differential Geometry
MA304 Differential Geoetry Hoework 4 solutions Spring 018 6% of the final ark 1. The paraeterised curve αt = t cosh t for t R is called the catenary. Find the curvature of αt. Solution. Fro hoework question
More informationFor more sample papers visit :
PHYSICS (THEORY) (Three hours) For more sample papers visit : www.4ono.com Answer all questions in Part I and six questions from Part II, choosing two questions from each of the Sections A, B and C. All
More informationLAB 10: OPTICAL MATERIALS AND DISPERSION I
OPTI 202L - Geometrical and Instrumental Optics Lab LAB 10: OPTICAL MATERIALS AND DISPERSION I 10-1 Measuring the refractive index of a material is one of the most fundamental optical measurements, and
More informationPC1144 Physics IV. Atomic Spectra
PC1144 Physics IV Atomic Spectra 1 Objectives Investigate how well the visible light wavelengths of hydrogen predicted by the Bohr theory agree with experimental values. Determine an experimental value
More informationDispersion of Glass Introduction Apparatus Theory
Dispersion of Glass Introduction This experiment will develop skills in aligning and using a spectrometer to measure dispersion of glass, and choosing a suitable fit for data and plotting the resulting
More informationInternational Mathematical Olympiad. Preliminary Selection Contest 2009 Hong Kong. Outline of Solutions
International Matheatical Olypiad Preliinary Selection ontest 009 Hong Kong Outline of Solutions nswers:. 03809. 0 3. 0. 333. 00099 00. 37 7. 3 8. 3 9. 3 0. 8 3. 009 00. 3 3. 3. 89. 8077. 000 7. 30 8.
More informationWater a) 48 o b) 53 o c) 41.5 o d) 44 o. Glass. PHYSICS 223 Exam-2 NAME II III IV
PHYSICS 3 Exa- NAME. In the figure shown, light travels fro aterial I, through three layers of other aterials with surfaces parallel to one another, and then back into another layer of aterial I. The refractions
More informationDispersion and resolving power of the prism and grating spectroscope (Item No.: P )
Dispersion and resolving power of the prism and grating spectroscope (Item No.: P2210300) Curricular Relevance Area of Expertise: Physics Education Level: University Topic: Light and Optics Subtopic: Diffraction
More informationLaboratory #29: Spectrometer
INDIANA UNIVERSITY, DEPARTMENT OF PHYSICS, P309 LABORATORY Laboratory #29: Spectrometer Goal: Learn to adjust an optical spectrometer, use a transmission grating to measure known spectral lines of mercury,
More informationOptics. Measuring the line spectra of inert gases and metal vapors using a prism spectrometer. LD Physics Leaflets P
Optics Spectrometer Prism spectrometer LD Physics Leaflets P5.7.1.1 Measuring the line spectra of inert gases and metal vapors using a prism spectrometer Objects of the experiment Adjusting the prism spectrometer.
More information8.1 Force Laws Hooke s Law
8.1 Force Laws There are forces that don't change appreciably fro one instant to another, which we refer to as constant in tie, and forces that don't change appreciably fro one point to another, which
More informationMAKE SURE TA & TI STAMPS EVERY PAGE BEFORE YOU START
Laboratory Section: Last Revised on Deceber 15, 2014 Partners Naes: Grade: EXPERIMENT 8 Electron Beas 0. Pre-Laboratory Work [2 pts] 1. Nae the 2 forces that are equated in order to derive the charge to
More information12 th Annual Johns Hopkins Math Tournament Saturday, February 19, 2011 Power Round-Poles and Polars
1 th Annual Johns Hopkins Math Tournaent Saturday, February 19, 011 Power Round-Poles and Polars 1. Definition and Basic Properties 1. Note that the unit circles are not necessary in the solutions. They
More information2. Electric Current. E.M.F. of a cell is defined as the maximum potential difference between the two electrodes of the
2. Electric Current The net flow of charges through a etallic wire constitutes an electric current. Do you know who carries current? Current carriers In solid - the electrons in outerost orbit carries
More informationn(λ) = c/v(λ). Figure 1: Dispersion curves for some common optical glass types.
Physics 2310 Lab 2: The Dispersion of Optical Glass Dr. Michael Pierce (Univ. of Wyoming) Based on a lab by Dr. M. Kruger (Univ. of Missouri, Kansas City) Purpose: The purpose of this lab is to introduce
More informationOPTICAL INSTRUMENTS VERY SHORT ANSWER QUESTIONS
OPTICAL INSTRUMENTS VERY SHORT ANSWER QUESTIONS Q-1. The difference in the focal lengths of the two lenses is larger in which case microscope or telescope? Q-2. What is the formula for angular magnification
More informationLab 5: Spectroscopy & the Hydrogen Atom Phy248 Spring 2009
Lab 5: Spectroscopy & the Hydrogen Atom Phy248 Spring 2009 Name Section Return this spreadsheet to your TA that will use it to score your lab. To receive full credit you must use complete sentences and
More informationInstruments and Related Topics
1. Traveling Microscope The traveling microscope [Fig.1] is an instrument well-suited for the purpose of measuring small vertical or horizontal distances with high accuracy. It consists of a compound microscope
More informationQuiz 5 PRACTICE--Ch12.1, 13.1, 14.1
Nae: Class: Date: ID: A Quiz 5 PRACTICE--Ch2., 3., 4. Multiple Choice Identify the choice that best copletes the stateent or answers the question.. A bea of light in air is incident at an angle of 35 to
More informationAIPMT / NEET (Physics, Chemistry and Biology) Code A/P/W. Time: 3 hrs Total Marks: 720
AIPMT / NEET - 06 (Physics, Cheistry and Biology) Code A/P/W Tie: hrs Total Marks: 70 General Instructions:. The Answer sheet is inside this Text booklet. When you are directed to open the text booklet,
More informationNORTHERN ILLINOIS UNIVERSITY PHYSICS DEPARTMENT. Physics 211 E&M and Quantum Physics Spring Lab #9: Diffraction Spectroscopy
NORTHERN ILLINOIS UNIVERSITY PHYSICS DEPARTMENT Physics 211 E&M and Quantum Physics Spring 2018 Lab #9: Diffraction Spectroscopy Lab Writeup Due: Mon/Wed/Thu/Fri, April 30/ May 2/3/4, 2018 Background All
More informationDETECTION OF NONLINEARITY IN VIBRATIONAL SYSTEMS USING THE SECOND TIME DERIVATIVE OF ABSOLUTE ACCELERATION
DETECTION OF NONLINEARITY IN VIBRATIONAL SYSTEMS USING THE SECOND TIME DERIVATIVE OF ABSOLUTE ACCELERATION Masaki WAKUI 1 and Jun IYAMA and Tsuyoshi KOYAMA 3 ABSTRACT This paper shows a criteria to detect
More informationRydberg constant from atomic spectra of gases
Page 1 of 8 Rydberg constant from atomic spectra of gases Objective - Calibrating a prism spectrometer to convert the scale readings in wavelengths of spectral lines. - Observing the Balmer series of atomic
More informationUSEFUL HINTS FOR SOLVING PHYSICS OLYMPIAD PROBLEMS. By: Ian Blokland, Augustana Campus, University of Alberta
1 USEFUL HINTS FOR SOLVING PHYSICS OLYMPIAD PROBLEMS By: Ian Bloland, Augustana Capus, University of Alberta For: Physics Olypiad Weeend, April 6, 008, UofA Introduction: Physicists often attept to solve
More information72. (30.2) Interaction between two parallel current carrying wires.
7. (3.) Interaction between two parallel current carrying wires. Two parallel wires carrying currents exert forces on each other. Each current produces a agnetic field in which the other current is placed.
More informationLecture #8-3 Oscillations, Simple Harmonic Motion
Lecture #8-3 Oscillations Siple Haronic Motion So far we have considered two basic types of otion: translation and rotation. But these are not the only two types of otion we can observe in every day life.
More informationEasy Evaluation Method of Self-Compactability of Self-Compacting Concrete
Easy Evaluation Method of Self-Copactability of Self-Copacting Concrete Masanori Maruoka 1 Hiroi Fujiwara 2 Erika Ogura 3 Nobu Watanabe 4 T 11 ABSTRACT The use of self-copacting concrete (SCC) in construction
More informationa a a a a a a m a b a b
Algebra / Trig Final Exa Study Guide (Fall Seester) Moncada/Dunphy Inforation About the Final Exa The final exa is cuulative, covering Appendix A (A.1-A.5) and Chapter 1. All probles will be ultiple choice
More informationPHYSICS ADVANCED LABORATORY I UNIVERSAL GRAVITATIONAL CONSTANT Spring 2001 (additions for Spring 2005 on last page)
PHYSICS 334 - ADVANCED LABOATOY I UNIVESAL GAVITATIONAL CONSTANT Spring 001 (aitions for Spring 005 on last page) Purposes: Deterine the value of the universal gravitation constant G. Backgroun: Classical
More informationPart I: How Dense Is It? Fundamental Question: What is matter, and how do we identify it?
Part I: How Dense Is It? Fundaental Question: What is atter, and how do we identify it? 1. What is the definition of atter? 2. What do you think the ter ass per unit volue eans? 3. Do you think that a
More informationCHAPTER 37. Answer to Checkpoint Questions
1010 CHAPTER 37 DIFFRACTION CHAPTER 37 Answer to Checkpoint Questions 1. (a) expan; (b) expan. (a) secon sie axiu; (b) :5 3. (a) re; (b) violet 4. iinish 5. (a) increase; (b) sae 6. (a) left; (b) less
More informationEngineering Physics 1 Prof. G.D. Vermaa Department of Physics Indian Institute of Technology-Roorkee
Engineering Physics 1 Prof. G.D. Vermaa Department of Physics Indian Institute of Technology-Roorkee Module-04 Lecture-02 Diffraction Part - 02 In the previous lecture I discussed single slit and double
More informationEXPERIMENT 14. The Atomic Spectrum of Hydrogen
Name: Laboratory Section: Laboratory Section Date: Partners Names: Grade: Last Revised on March 18, 2003 EXPERIMENT 14 The Atomic Spectrum of Hydrogen 0. Pre-Laboratory Work [2 pts] 1. You will be using
More informationTAP 413-2: Measuring the charge to mass ratio for an electron
TAP 413-: Measuring the charge to ass ratio for an electron Using circular otion Using a agnetic field to drive an electron round in a circle can give inforation about the acceleration. The agnetic force
More informationNEET PHYSICS PAPER CODE : PP NEET-2018 ( ) PHYSICS
NEET PHYSICS PAPER CODE : PP NEET-8 (6-5-8) PHYSICS Q. An e wave is propagating in a ediu with a Ans. () velocity v v î. The instantaneous oscillating electric field of this e wave is along +y axis. Then
More informationElectromagnetic Waves
Electroagnetic Waves Physics 4 Maxwell s Equations Maxwell s equations suarize the relationships between electric and agnetic fields. A ajor consequence of these equations is that an accelerating charge
More informationThe accelerated expansion of the universe is explained by quantum field theory.
The accelerated expansion of the universe is explained by quantu field theory. Abstract. Forulas describing interactions, in fact, use the liiting speed of inforation transfer, and not the speed of light.
More informationHyperbolic Horn Helical Mass Spectrometer (3HMS) James G. Hagerman Hagerman Technology LLC & Pacific Environmental Technologies April 2005
Hyperbolic Horn Helical Mass Spectroeter (3HMS) Jaes G Hageran Hageran Technology LLC & Pacific Environental Technologies April 5 ABSTRACT This paper describes a new type of ass filter based on the REFIMS
More informationIn this chapter we will start the discussion on wave phenomena. We will study the following topics:
Chapter 16 Waves I In this chapter we will start the discussion on wave phenoena. We will study the following topics: Types of waves Aplitude, phase, frequency, period, propagation speed of a wave Mechanical
More informationDISPERSION VERY SHORT ANSWER QUESTIONS. Two identical prisms made of the same material placed with their based on opposite sides (of the
DISPERSION VERY SHORT ANSWER QUESTIONS Q-1. What will be the spectrum of sun during a total solar eclipse? Q-2. Why the secondary rainbow is always fainter than the primary rainbow? Q-3. Two identical
More informationLab 10: Spectroscopy & the Hydrogen Atom Phy208 Fall 2008
Lab 10: Spectroscopy & the Hydrogen Atom Phy208 Fall 2008 Name Section This sheet is the lab document your TA will use to score your lab. It is to be turned in at the end of lab. To receive full credit
More informationPHYSICS PAPER 1 (THEORY) (Three hours)
PHYSICS PAPER 1 (THEORY) (Three hours) (Candidates are allowed additional 15 minutes for only reading the paper. They must OT start writing during this time.) ---------------------------------------------------------------------------------------------------------------------
More informationQuestion number 1 to 8 carries 2 marks each, 9 to 16 carries 4 marks each and 17 to 18 carries 6 marks each.
IIT-JEE5-PH-1 FIITJEE Solutions to IITJEE 5 Mains Paper Tie: hours Physics Note: Question nuber 1 to 8 carries arks each, 9 to 16 carries 4 arks each and 17 to 18 carries 6 arks each. Q1. whistling train
More informationPhysics 23 Fall 1998 Lab 4 - The Hydrogen Spectrum
Physics 3 Fall 998 Lab 4 - The Hydrogen Spectrum Theory In the late 800's, it was known that when a gas is excited by means of an electric discharge and the light emitted is viewed through a diffraction
More informationChapter 8 Deflection. Structural Mechanics 2 Dept of Architecture
Chapter 8 Deflection Structural echanics Dept of rchitecture Outline Deflection diagras and the elastic curve Elastic-bea theory The double integration ethod oent-area theores Conjugate-bea ethod 8- Deflection
More informationn(a B) = n(a - B) + n(a B) + n(b- A) 50 = n(b- A) n(b- A) = n(b- A) =15 Now,n(B) = n(a B) + n(b- A) = = 30
Answer Keys: 1 A A A 4 A 5 B 6 C 7 A 8 D 9 B 10 B 11 B 1 C 1 A 14 A 15 C 16 D 17 A 18 C 19 B 0 B 1 A B B 4 B 5 A 6 D 7 A 8 D 9 C 0 C 1 A C B 4 A 5 B 6 A 7 C 8 B 9 B 40 C 41 C 4 D 4 B 44 A 45 B 46 D 47
More informationIn this chapter, we consider several graph-theoretic and probabilistic models
THREE ONE GRAPH-THEORETIC AND STATISTICAL MODELS 3.1 INTRODUCTION In this chapter, we consider several graph-theoretic and probabilistic odels for a social network, which we do under different assuptions
More informationDesign and Experimental Research of Atomizer Based on Micro Abrasive Ultrasonic Polishing Bang-fu WANG, Yin ZHEN, Juan SONG and A-chun ZHU
217 3rd International Conference on Applied Mechanics and Mechanical Autoation (AMMA 217) ISBN: 978-1-6595-479- Design and Experiental Research of Atoizer Based on Micro Abrasive Ultrasonic Polishing Bang-fu
More informationProc. of the IEEE/OES Seventh Working Conference on Current Measurement Technology UNCERTAINTIES IN SEASONDE CURRENT VELOCITIES
Proc. of the IEEE/OES Seventh Working Conference on Current Measureent Technology UNCERTAINTIES IN SEASONDE CURRENT VELOCITIES Belinda Lipa Codar Ocean Sensors 15 La Sandra Way, Portola Valley, CA 98 blipa@pogo.co
More informationE. K. A. ADVANCED PHYSICS LABORATORY PHYSICS 3081, 4051 FRAUNHOFER DIFFRACTION
E. K. A. ADVANCED PHYSICS LABORATORY PHYSICS 3081, 4051 FRAUNHOFER DIFFRACTION References for Fraunhofer Diffraction 1. Jenkins and White Fundamentals of Optics. Chapters on Fraunhofer diffraction and
More informationProtokoll. Grundpraktikum II - Optical Spectroscopy
Protokoll Grundpraktikum II - Optical Spectroscopy 1 Elaboration 1.1 Optical Spectroscopy Student: Hauke Rasch, Martin Borchert Tutor: Madsen Date: 22.October2014 This experiment is about the fundamental
More informationPhysics Circular Motion: Energy and Momentum Conservation. Science and Mathematics Education Research Group
F FA ACULTY C U L T Y OF O F EDUCATION E D U C A T I O N Departent of Curriculu and Pedagogy Physics Circular Motion: Energy and Moentu Conservation Science and Matheatics Education Research Group Supported
More informationOBJECTIVES INTRODUCTION
M7 Chapter 3 Section 1 OBJECTIVES Suarize data using easures of central tendency, such as the ean, edian, ode, and idrange. Describe data using the easures of variation, such as the range, variance, and
More informationPHYS 102 Previous Exam Problems
PHYS 102 Previous Exa Probles CHAPTER 16 Waves Transverse waves on a string Power Interference of waves Standing waves Resonance on a string 1. The displaceent of a string carrying a traveling sinusoidal
More informationQuestion 1. [14 Marks]
6 Question 1. [14 Marks] R r T! A string is attached to the dru (radius r) of a spool (radius R) as shown in side and end views here. (A spool is device for storing string, thread etc.) A tension T is
More informationSIR C.R.REDDY COLLEGE OF ENGINEERING ELURU
SIR C.R.REDDY COLLEGE OF ENGINEERING ELURU-534007 METROLOGY LABORATORY MANUAL III/IV B.TECH (Mechanical): II SEMESTER DEPARTMENT OF MECHANICAL ENGINEERING DEPARTMENT OF MECHANICAL ENGINEERING METROLOGY
More informationInstruction Sheet Martin Henschke, Ballistic Pendulum art. no.:
Physics Educational Tools Dr. Martin Henschke Gerätebau Dieselstr. 8, 5374 Erftstadt, Gerany www.henschke-geraetebau.de/english/ Instruction Sheet Martin Henschke, 4-6-1 Ballistic Pendulu art. no.: 6573
More informationAny first year text, sections on atomic structure, spectral lines and spectrometers
Physics 33 Experiment 5 Atomic Spectra References Any first year text, sections on atomic structure, spectral lines and spectrometers Any modern physics text, eg F.K. Richtmeyer, E.H. Kennard and J.N.
More informationSpeed of Light in Glass
Experiment (1) Speed of Light in Glass Objective:- This experiment is used to determine the speed of propagation of light waves in glass. Apparatus:- Prism, spectrometer, Halogen lamp source. Theory:-
More informationPH 221-2A Fall Waves - I. Lectures Chapter 16 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition)
PH 1-A Fall 014 Waves - I Lectures 4-5 Chapter 16 (Halliday/Resnick/Walker, Fundaentals of Physics 9 th edition) 1 Chapter 16 Waves I In this chapter we will start the discussion on wave phenoena. We will
More informationCurious Bounds for Floor Function Sums
1 47 6 11 Journal of Integer Sequences, Vol. 1 (018), Article 18.1.8 Curious Bounds for Floor Function Sus Thotsaporn Thanatipanonda and Elaine Wong 1 Science Division Mahidol University International
More informationProbability and Stochastic Processes: A Friendly Introduction for Electrical and Computer Engineers Roy D. Yates and David J.
Probability and Stochastic Processes: A Friendly Introduction for Electrical and oputer Engineers Roy D. Yates and David J. Goodan Proble Solutions : Yates and Goodan,1..3 1.3.1 1.4.6 1.4.7 1.4.8 1..6
More informationPHYSICS ADVANCED LABORATORY I UNIVERSAL GRAVITATIONAL CONSTANT Spring 2001
PHYSICS 334 - ADVANCED LABOATOY I UNIVESAL GAVITATIONAL CONSTANT Spring 001 Purposes: Deterine the value of the universal gravitation constant G. Backgroun: Classical echanics topics-oents of inertia,
More informationHYDROGEN SPECTRUM. Figure 1 shows the energy level scheme for the hydrogen atom as calculated from equation. Figure 1 Figure 2
15 Jul 04 Hydrogen.1 HYDROGEN SPECTRUM In this experiment the wavelengths of the visible emission lines of hydrogen (Balmer series) will be measured and compared to the values predicted by Bohr s quantum
More informationPhysics 120 Final Examination
Physics 120 Final Exaination 12 August, 1998 Nae Tie: 3 hours Signature Calculator and one forula sheet allowed Student nuber Show coplete solutions to questions 3 to 8. This exaination has 8 questions.
More informationEinstein Classes, Unit No. 102, 103, Vardhman Ring Road Plaza, Vikas Puri Extn., Outer Ring Road New Delhi , Ph. : ,
1 O P T I C S 1. Define resolving power of a telescope & microscope and give the expression for its resolving power. 2. Explain briefly the formation of mirage in deserts. 3. The radii of curvature of
More informationLAB MECH8.COMP From Physics with Computers, Vernier Software & Technology, 2003.
LAB MECH8.COMP Fro Physics with Coputers, Vernier Software & Technology, 003. INTRODUCTION You have probably watched a ball roll off a table and strike the floor. What deterines where it will land? Could
More informationAtomic emission spectra experiment
Atomic emission spectra experiment Contents 1 Overview 1 2 Equipment 1 3 Measuring the grating spacing using the sodium D-lines 4 4 Measurement of hydrogen lines and the Rydberg Constant 5 5 Measurement
More informationNational 5 Summary Notes
North Berwick High School Departent of Physics National 5 Suary Notes Unit 3 Energy National 5 Physics: Electricity and Energy 1 Throughout the Course, appropriate attention should be given to units, prefixes
More informationUNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics
UNIVERSITY OF SASKATCHEWAN Departent of Physics and Engineering Physics 05 Saskatchewan High School Physics Scholarship Copetition May, 05 Tie allowed: 90 inutes This copetition is based on the Saskatchewan
More information= T. Oscillations and Waves. Example of an Oscillating System IB 12 IB 12
Oscillation: the vibration of an object Oscillations and Waves Eaple of an Oscillating Syste A ass oscillates on a horizontal spring without friction as shown below. At each position, analyze its displaceent,
More informationEmission Spectrum of Atomic Gases. Prelab Questions
Emission Spectrum of Atomic Gases Prelab Questions Before this coming to this lab, please review your text for the physics of the spectrum of visible light and of diffraction grating spectrometer.. Which
More informationProblem Set 14: Oscillations AP Physics C Supplementary Problems
Proble Set 14: Oscillations AP Physics C Suppleentary Probles 1 An oscillator consists of a bloc of ass 050 g connected to a spring When set into oscillation with aplitude 35 c, it is observed to repeat
More informationPearson Physics Level 30 Unit VI Forces and Fields: Chapter 12 Solutions
Concept Check (top) Pearson Physics Level 30 Unit VI Forces and Fields: Chapter 12 Solutions Student Book page 583 Concept Check (botto) The north-seeking needle of a copass is attracted to what is called
More informationThis is a repository copy of Analytical optimisation of electromagnetic design of a linear (tubular) switched reluctance motor.
This is a repository copy of Analytical optiisation of electroagnetic design of a linear (tubular) switched reluctance otor. White Rose Research Online URL for this paper: http://eprints.whiterose.ac.uk/907/
More informationInterference and Diffraction
Topics: What we are going to learn Wave behaviour of EM wave (In the case of light) Interference an iffraction Huygens' principle Interference of light fro ouble slit Thin fil Interferoeter iffraction
More informationBALLISTIC PENDULUM. EXPERIMENT: Measuring the Projectile Speed Consider a steel ball of mass
BALLISTIC PENDULUM INTRODUCTION: In this experient you will use the principles of conservation of oentu and energy to deterine the speed of a horizontally projected ball and use this speed to predict the
More informationlecture 37: Linear Multistep Methods: Absolute Stability, Part I lecture 38: Linear Multistep Methods: Absolute Stability, Part II
lecture 37: Linear Multistep Methods: Absolute Stability, Part I lecture 3: Linear Multistep Methods: Absolute Stability, Part II 5.7 Linear ultistep ethods: absolute stability At this point, it ay well
More informationQ5 We know that a mass at the end of a spring when displaced will perform simple m harmonic oscillations with a period given by T = 2!
Chapter 4.1 Q1 n oscillation is any otion in which the displaceent of a particle fro a fixed point keeps changing direction and there is a periodicity in the otion i.e. the otion repeats in soe way. In
More informationUNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics
UNIVERSITY OF SASKATCHEWAN Departent of Physics and Engineering Physics 017 Saskatchewan High School Physics Scholarship Copetition Wednesday May 10, 017 Tie allowed: 90 inutes This copetition is based
More information