Assignment Solutions- Dual Nature. September 19

Size: px
Start display at page:

Download "Assignment Solutions- Dual Nature. September 19"

Transcription

1 Assignment Solutions- Dual Nature September 9 03

2 CH 4 DUAL NATURE OF RADIATION & MATTER SOLUTIONS No. Constants used:, = 6.65 x 0-34 Js, e =.6 x 0-9 C, c = 3 x 0 8 m/s Answers Two metals A, B ave work functions ev and 4 ev respectively. Wic metal as a lower tresold wavelengt for poto electric effect? Given A < B ν o = i.e. C = λ o K λ o = K- constant B Since A < B, λ B < λ A Te de Broglie wave lengt associated wit an electron accelerated troug a potential difference V is λ. Wat will be its wavelengt, wen te acceleration potential is increased to 4V? For an electron, λe =.7 V Å i.e. λe V λ/ For a potential 4V, λe 4V λe = λe 3 A particle of a mass M at rest decays into particles of masses m and m aving nonzero velocities. Wat is te ratio of te de-broglie wavelengt of te two particles? Using te conservation of momentum, p + p = 0 i.e. p = p we know tat, λ = ; since p = p p ; λ = λ An electron, alpa particle and a proton ave te same K.E. Wic of tese particles as te sortest de Broglie wavelengt? Given : Ee = Eα = Ep ; also me < mp < mα Kinetic energy E = ½ m v ; E = m v m = p m : p = m E () 4 de-broglie s relation gives, λ = p = m E () α Since E is same for all te particles, () can be written as : λ = k m Since mass of α particle (mα) is greatest, it as te sortest de-broglie wavelengt.

3 5 Te tresold frequency of metal is 0. Wen te ligt of frequency 0 is incident on te metal plate, te maximum velocity of electrons emitted is v. Wen te frequency of te incident radiation is increased to 5 0, te maximum velocity of electrons emitted is v. Find te ratio of v to v. From Einstein s poto-electric equation, ν = o + ½ m v For te two cases, ν o = ν o + ½ m v ν o = ½ m v (3) Similarly, 4ν o = ½ m v (4) (4) / (3), we get, 4 = v v v : v = : : An alpa particle and a proton are accelerated tru te same potential difference. Calculate te ratio of linear momentum acquired by te two. We know tat, m p < m α ; but m α = 4m p -----(5) and q α = q p -----(6) Wen a carge q is accelerated troug a potential V, its kinetic energy E is given by : 6 E = qv (7) From () te momentum of te particle is p = m qv : p α = m α q α V p p = m p q p V From (5) and (6), we get, p α : p p = : Wen te ligt of wavelengt 400nm is incident on te catode of a potocell, te stopping potential recorded is 6 V. If te wave of incident ligt is increased to 600nm. Calculate te new stopping potential. From Einstein s poto-electric equation, ν = o + ev o (8) C λ = o + ev o (9) 7 For te two cases, () (0), we get, c e C λ = o + ev o (0) and C λ = o + ev o () λ λ = V o V o 4.96 V Substituting te values of, c, e, λ = 400nm, λ = 600nm and V o = 6V, V o = 4.96 V 3

4 8 9 0 If te intensity of radiation incident on a potocell is doubled, wat appens to te number of potoelectrons and energy of te potoelectrons? As intensity of radiation is increased, te number of potoelectrons increases, but energy of te potons remains te same. Energy will increase only wit increase in frequency of radiation, not wit increase in intensity. If te frequency of radiation incident on a potocell is doubled, wat appens to te number of potoelectrons and energy of te potoelectrons? Same as above. Ligt of two different frequencies wose potons ave energies ev and.5ev, respectively, successively illuminate a metal wose work function is 0.5 ev. Find te ratio of maximum speed of te emitted electrons. ν o = o + ½ m v ev = 0.5 ev + ½ m v 0.5 ev = ½ m v ().5eV = 0.5 ev + ½ m v ev = ½ m v () () / () we get, 4 = v v v : v = : A proton wen accelerated troug a potential difference of V volt as a de-broglie wavelengt λ. Wat sould be te potential required to accelerate an α particle in order to ave te same λ? Given λ α = λ p, Te de-broglie wavelengt of a carge accelerated troug a potential V is given by: Increases No Cange No Cange Increases : λ = m qv λ p = m p q p V ----() and λ α = m α q α V ---(3) V/8 volt But m α = 4m p, q α = q p and λ α = λ p (given) equating () and (3), we get, 3 V = V 8 Wen ligt of wavelengt 0.6mm falls on a potocell potoelectrons are emitted for wic te stopping potential is 0.5V. Wit ligt of wavelengt 0.04 mm te stopping potential canges to.5v. Find te work-function of te metal in electron-volts. If 5% of energy supplied to a bulb is irradiated as visible ligt, ow many quanta are emitted per second by a 00W bulb? Assume wavelengt of ligt is 5.6 x 0-5 cm. 00W = 00 J/s Only 5% is visible radiation. Ie 5 J/s Energy of one poton, E = ν or E = C λ (4) Energy of n potons = 5 J n = 5 C λ =.4 x 0 9 s -.4 x 0 9 s - 4

5 4 Wat is te ratio of te wavelengt of a poton and tat of an electron of te same energy? For a poton, E = C i.e. λ λ p = C ---(5) For an electron, λ E e = = ---(6) p me λ p λ e = c me E = c m E c m E Te grap below sows te variation of te max. kinetic energy of potoelectrons wit frequency of incident ligt. Find te tresold frequency and work function of te metal from te grap. E (ev) ν (x 0 4 Hz) 0 5 Hz 4 ev From Einstein s potoelectric equation, ν = o + ev -----(7) ev = ν - o ----(8) (equation for a straigt line wit slope = ) But ν o = o i.e. wen ν = ν o, ev = 0. From te grap ν o = 0 5 Hz From te grap and from (8) o = 4eV Eby P Kurien, mail@selltesell.com 5

ATOMIC PHYSICS PREVIOUS EAMCET QUESTIONS ENGINEERING

ATOMIC PHYSICS PREVIOUS EAMCET QUESTIONS ENGINEERING ATOMIC PHYSICS PREVIOUS EAMCET QUESTIONS ENGINEERING 9. Te work function of a certain metal is. J. Ten te maximum kinetic energy of potoelectrons emitted by incident radiation of wavelengt 5 A is: (9 E)

More information

Dual Nature of matter and radiation: m v 1 c

Dual Nature of matter and radiation: m v 1 c Dual Nature of matter and radiation: Potons: Electromagnetic radiation travels in space in te form discrete packets of energy called potons. Tese potons travel in straigt line wit te speed of ligt. Important

More information

DUAL NATURE OF RADIATION AND MATTER

DUAL NATURE OF RADIATION AND MATTER DUAL NATURE OF RADIATION AND MATTER Important Points: 1. J.J. Tomson and Sir William Crookes studied te discarge of electricity troug gases. At about.1 mm of Hg and at ig voltage invisible streams called

More information

QUESTIONS ) Of the following the graph which represents the variation of Energy (E) of the photon with the wavelength (λ) is E E 1) 2) 3) 4)

QUESTIONS ) Of the following the graph which represents the variation of Energy (E) of the photon with the wavelength (λ) is E E 1) 2) 3) 4) CET II PUC: PHYSICS: ATOMIC PHYSICS INTRODUCTION TO ATOMIC PHYSICS, PHOTOELECTRIC EFFECT DUAL NATURE OF MATTER, BOHR S ATOM MODEL SCATTERING OF LIGHT and LASERS QUESTIONS ) Wic of te following statements

More information

Test on Nuclear Physics

Test on Nuclear Physics Test on Nuclear Pysics Examination Time - 40 minutes Answer all questions in te spaces provided Tis wole test involves an imaginary element called Bedlum wic as te isotope notation sown below: 47 11 Bd

More information

Preview from Notesale.co.uk Page 2 of 42

Preview from Notesale.co.uk Page 2 of 42 1 PHYSICAL CHEMISTRY Dalton (1805) Tomson (1896) - Positive and negative carges Ruterford (1909) - Te Nucleus Bor (1913) - Energy levels Atomic Model : Timeline CATHODE RAYS THE DISCOVERY OF ELECTRON Scrödinger

More information

Physics Teach Yourself Series Topic 15: Wavelike nature of matter (Unit 4)

Physics Teach Yourself Series Topic 15: Wavelike nature of matter (Unit 4) Pysics Teac Yourself Series Topic 15: Wavelie nature of atter (Unit 4) A: Level 14, 474 Flinders Street Melbourne VIC 3000 T: 1300 134 518 W: tss.co.au E: info@tss.co.au TSSM 2017 Page 1 of 8 Contents

More information

UNIT-1 MODERN PHYSICS

UNIT-1 MODERN PHYSICS UNIT- MODERN PHYSICS Introduction to blackbody radiation spectrum: A body wic absorbs all radiation tat is incident on it is called a perfect blackbody. Wen radiation allowed to fall on suc a body, it

More information

M12/4/PHYSI/HPM/ENG/TZ1/XX. Physics Higher level Paper 1. Thursday 10 May 2012 (afternoon) 1 hour INSTRUCTIONS TO CANDIDATES

M12/4/PHYSI/HPM/ENG/TZ1/XX. Physics Higher level Paper 1. Thursday 10 May 2012 (afternoon) 1 hour INSTRUCTIONS TO CANDIDATES M12/4/PHYSI/HPM/ENG/TZ1/XX 22126507 Pysics Higer level Paper 1 Tursday 10 May 2012 (afternoon) 1 our INSTRUCTIONS TO CANDIDATES Do not open tis examination paper until instructed to do so. Answer all te

More information

Final exam: Tuesday, May 11, 7:30-9:30am, Coates 143

Final exam: Tuesday, May 11, 7:30-9:30am, Coates 143 Final exam: Tuesday, May 11, 7:30-9:30am, Coates 143 Approximately 7 questions/6 problems Approximately 50% material since last test, 50% everyting covered on Exams I-III About 50% of everyting closely

More information

nucleus orbital electron wave 2/27/2008 Quantum ( F.Robilliard) 1

nucleus orbital electron wave 2/27/2008 Quantum ( F.Robilliard) 1 r nucleus orbital electron wave λ /7/008 Quantum ( F.Robilliard) 1 Wat is a Quantum? A quantum is a discrete amount of some quantity. For example, an atom is a mass quantum of a cemical element te mass

More information

Problem Set 3: Solutions

Problem Set 3: Solutions University of Alabama Department of Pysics and Astronomy PH 253 / LeClair Spring 2010 Problem Set 3: Solutions 1. Te energy required to break one OO bond in ozone O 3, OOO) is about 500 kj/mol. Wat is

More information

38. Photons and Matter Waves

38. Photons and Matter Waves 38. Potons and Matter Waves Termal Radiation and Black-Body Radiation Color of a Tungsten filament as temperature increases Black Red Yellow Wite T Termal radiation : Te radiation depends on te temperature

More information

Tutorial 2 (Solution) 1. An electron is confined to a one-dimensional, infinitely deep potential energy well of width L = 100 pm.

Tutorial 2 (Solution) 1. An electron is confined to a one-dimensional, infinitely deep potential energy well of width L = 100 pm. Seester 007/008 SMS0 Modern Pysics Tutorial Tutorial (). An electron is confined to a one-diensional, infinitely deep potential energy well of widt L 00 p. a) Wat is te least energy te electron can ave?

More information

Contents. Theory Exercise Exercise Exercise Exercise Answer Key 28-29

Contents. Theory Exercise Exercise Exercise Exercise Answer Key 28-29 ATOMIC STRUCTURE Topic Contents Page No. Teory 0-04 Exercise - 05-4 Exercise - 5-9 Exercise - 3 0-3 Exercise - 4 4-7 Answer Key 8-9 Syllabus Bor model, spectrum of ydrogen atom, quantum numbers; Wave-particle

More information

Problem Set 4: Whither, thou turbid wave SOLUTIONS

Problem Set 4: Whither, thou turbid wave SOLUTIONS PH 253 / LeClair Spring 2013 Problem Set 4: Witer, tou turbid wave SOLUTIONS Question zero is probably were te name of te problem set came from: Witer, tou turbid wave? It is from a Longfellow poem, Te

More information

f a h f a h h lim lim

f a h f a h h lim lim Te Derivative Te derivative of a function f at a (denoted f a) is f a if tis it exists. An alternative way of defining f a is f a x a fa fa fx fa x a Note tat te tangent line to te grap of f at te point

More information

28 64 Ni is - g/mole Se (D)

28 64 Ni is - g/mole Se (D) EXERCISE-0 CHECK YOUR GRASP SELECT THE CORRECT ALTERNATIVE (ONLY ONE CORRECT ANSWER). Te element aving no neutron in te nucleus of its atom is - (A) ydrogen (B) nitrogen (C) elium (D) boron. Te particles

More information

Everything comes unglued

Everything comes unglued Blackbody Radiation Potoelectric Effect Wave-Particle Duality SPH4U Everyting comes unglued Te predictions of classical pysics (Newton s laws and Maxwell s equations) are sometimes completely, utterly

More information

Introduction. Learning Objectives. On completion of this chapter you will be able to:

Introduction. Learning Objectives. On completion of this chapter you will be able to: Introduction Learning Objectives On completion of tis capter you will be able to: 1. Define Compton Effect. 2. Derive te sift in incident ligt wavelengt and Compton wavelengt. 3. Explain ow te Compton

More information

= h. Geometrically this quantity represents the slope of the secant line connecting the points

= h. Geometrically this quantity represents the slope of the secant line connecting the points Section 3.7: Rates of Cange in te Natural and Social Sciences Recall: Average rate of cange: y y y ) ) ), ere Geometrically tis quantity represents te slope of te secant line connecting te points, f (

More information

CHAPTER 7 QUANTUM THEORY AND ATOMIC STRUCTURE

CHAPTER 7 QUANTUM THEORY AND ATOMIC STRUCTURE CHAPTER 7 QUANTUM THEORY AND ATOMIC STRUCTURE Te value for te speed of ligt will be 3.00x0 8 m/s except wen more significant figures are necessary, in wic cases,.9979x0 8 m/s will be used. TOOLS OF THE

More information

1. State whether the function is an exponential growth or exponential decay, and describe its end behaviour using limits.

1. State whether the function is an exponential growth or exponential decay, and describe its end behaviour using limits. Questions 1. State weter te function is an exponential growt or exponential decay, and describe its end beaviour using its. (a) f(x) = 3 2x (b) f(x) = 0.5 x (c) f(x) = e (d) f(x) = ( ) x 1 4 2. Matc te

More information

The structure of the atoms

The structure of the atoms Te structure of te atoms Atomos = indivisible University of Pécs, Medical Scool, Dept. Biopysics All tat exists are atoms and empty space; everyting else is merely tougt to exist. Democritus, 415 B.C.

More information

Main Points: 1. Limit of Difference Quotients. Prep 2.7: Derivatives and Rates of Change. Names of collaborators:

Main Points: 1. Limit of Difference Quotients. Prep 2.7: Derivatives and Rates of Change. Names of collaborators: Name: Section: Names of collaborators: Main Points:. Definition of derivative as limit of difference quotients. Interpretation of derivative as slope of grap. Interpretation of derivative as instantaneous

More information

2.2 Derivative. 1. Definition of Derivative at a Point: The derivative of the function f x at x a is defined as

2.2 Derivative. 1. Definition of Derivative at a Point: The derivative of the function f x at x a is defined as . Derivative. Definition of Derivative at a Point: Te derivative of te function f at a is defined as f fa fa a lim provided te limit eists. If te limit eists, we sa tat f is differentiable at a, oterwise,

More information

Reminder: Exam 3 Friday, July 6. The Compton Effect. General Physics (PHY 2140) Lecture questions. Show your work for credit.

Reminder: Exam 3 Friday, July 6. The Compton Effect. General Physics (PHY 2140) Lecture questions. Show your work for credit. General Pysics (PHY 2140) Lecture 15 Modern Pysics Cater 27 1. Quantum Pysics Te Comton Effect Potons and EM Waves Wave Proerties of Particles Wave Functions Te Uncertainty Princile Reminder: Exam 3 Friday,

More information

7. QUANTUM THEORY OF THE ATOM

7. QUANTUM THEORY OF THE ATOM 7. QUANTUM TEORY OF TE ATOM Solutions to Practice Problems Note on significant figures: If te final answer to a solution needs to be rounded off, it is given first wit one nonsignificant figure, and te

More information

CHAPTER 4 QUANTUM PHYSICS

CHAPTER 4 QUANTUM PHYSICS CHAPTER 4 QUANTUM PHYSICS INTRODUCTION Newton s corpuscular teory of ligt fails to explain te penomena like interference, diffraction, polarization etc. Te wave teory of ligt wic was proposed by Huygen

More information

Chemistry. Slide 1 / 63 Slide 2 / 63. Slide 4 / 63. Slide 3 / 63. Slide 6 / 63. Slide 5 / 63. Optional Review Light and Matter.

Chemistry. Slide 1 / 63 Slide 2 / 63. Slide 4 / 63. Slide 3 / 63. Slide 6 / 63. Slide 5 / 63. Optional Review Light and Matter. Slide 1 / 63 Slide 2 / 63 emistry Optional Review Ligt and Matter 2015-10-27 www.njctl.org Slide 3 / 63 Slide 4 / 63 Ligt and Sound Ligt and Sound In 1905 Einstein derived an equation relating mass and

More information

The Electromagnetic Spectrum. Today

The Electromagnetic Spectrum. Today Today Announcements: HW#7 is due after Spring Break on Wednesday Marc 1 t Exam # is on Tursday after Spring Break Te fourt extra credit project will be a super bonus points project. Tis extra credit can

More information

MATH CALCULUS I 2.1: Derivatives and Rates of Change

MATH CALCULUS I 2.1: Derivatives and Rates of Change MATH 12002 - CALCULUS I 2.1: Derivatives and Rates of Cange Professor Donald L. Wite Department of Matematical Sciences Kent State University D.L. Wite (Kent State University) 1 / 1 Introduction Our main

More information

1. Which one of the following expressions is not equal to all the others? 1 C. 1 D. 25x. 2. Simplify this expression as much as possible.

1. Which one of the following expressions is not equal to all the others? 1 C. 1 D. 25x. 2. Simplify this expression as much as possible. 004 Algebra Pretest answers and scoring Part A. Multiple coice questions. Directions: Circle te letter ( A, B, C, D, or E ) net to te correct answer. points eac, no partial credit. Wic one of te following

More information

Math 34A Practice Final Solutions Fall 2007

Math 34A Practice Final Solutions Fall 2007 Mat 34A Practice Final Solutions Fall 007 Problem Find te derivatives of te following functions:. f(x) = 3x + e 3x. f(x) = x + x 3. f(x) = (x + a) 4. Is te function 3t 4t t 3 increasing or decreasing wen

More information

1. ATOMIC STRUCTURE. Specific Charge (e/m) c/g

1. ATOMIC STRUCTURE. Specific Charge (e/m) c/g 1. ATOMIC STRUCTURE Synopsis : Fundamental particles: According to Dalton atom is te smallest indivisible particle. But discarge tube experiments ave proved tat atom consists of some more smaller particles.

More information

1 Limits and Continuity

1 Limits and Continuity 1 Limits and Continuity 1.0 Tangent Lines, Velocities, Growt In tion 0.2, we estimated te slope of a line tangent to te grap of a function at a point. At te end of tion 0.3, we constructed a new function

More information

2.11 That s So Derivative

2.11 That s So Derivative 2.11 Tat s So Derivative Introduction to Differential Calculus Just as one defines instantaneous velocity in terms of average velocity, we now define te instantaneous rate of cange of a function at a point

More information

Chapter-11 DUAL NATURE OF MATTER AND RADIATION

Chapter-11 DUAL NATURE OF MATTER AND RADIATION Chapter-11 DUAL NATURE OF MATTER AND RADIATION Work function (j o ): The minimum energy required for an electron to escape from the surface of a metal i.e. The energy required for free electrons to escape

More information

The Derivative The rate of change

The Derivative The rate of change Calculus Lia Vas Te Derivative Te rate of cange Knowing and understanding te concept of derivative will enable you to answer te following questions. Let us consider a quantity wose size is described by

More information

Lab 6 Derivatives and Mutant Bacteria

Lab 6 Derivatives and Mutant Bacteria Lab 6 Derivatives and Mutant Bacteria Date: September 27, 20 Assignment Due Date: October 4, 20 Goal: In tis lab you will furter explore te concept of a derivative using R. You will use your knowledge

More information

2.8 The Derivative as a Function

2.8 The Derivative as a Function .8 Te Derivative as a Function Typically, we can find te derivative of a function f at many points of its domain: Definition. Suppose tat f is a function wic is differentiable at every point of an open

More information

Problem Set 4 Solutions

Problem Set 4 Solutions University of Alabama Department of Pysics and Astronomy PH 253 / LeClair Spring 2010 Problem Set 4 Solutions 1. Group velocity of a wave. For a free relativistic quantum particle moving wit speed v, te

More information

1 2 x Solution. The function f x is only defined when x 0, so we will assume that x 0 for the remainder of the solution. f x. f x h f x.

1 2 x Solution. The function f x is only defined when x 0, so we will assume that x 0 for the remainder of the solution. f x. f x h f x. Problem. Let f x x. Using te definition of te derivative prove tat f x x Solution. Te function f x is only defined wen x 0, so we will assume tat x 0 for te remainder of te solution. By te definition of

More information

Extracting Atomic and Molecular Parameters From the de Broglie Bohr Model of the Atom

Extracting Atomic and Molecular Parameters From the de Broglie Bohr Model of the Atom Extracting Atomic and Molecular Parameters From te de Broglie Bor Model of te Atom Frank ioux Te 93 Bor model of te ydrogen atom was replaced by Scrödingerʹs wave mecanical model in 96. However, Borʹs

More information

Calculus I Homework: The Derivative as a Function Page 1

Calculus I Homework: The Derivative as a Function Page 1 Calculus I Homework: Te Derivative as a Function Page 1 Example (2.9.16) Make a careful sketc of te grap of f(x) = sin x and below it sketc te grap of f (x). Try to guess te formula of f (x) from its grap.

More information

E p = mgh (if h i=0) E k = ½ mv 2 Ek is measured in Joules (J); m is measured in kg; v is measured in m/s. Energy Continued (E)

E p = mgh (if h i=0) E k = ½ mv 2 Ek is measured in Joules (J); m is measured in kg; v is measured in m/s. Energy Continued (E) nergy Continued () Gravitational Potential nergy: - e energy stored in an object due to its distance above te surface of te art. - e energy stored depends on te mass of te object, te eigt above te surface,

More information

Section 2.7 Derivatives and Rates of Change Part II Section 2.8 The Derivative as a Function. at the point a, to be. = at time t = a is

Section 2.7 Derivatives and Rates of Change Part II Section 2.8 The Derivative as a Function. at the point a, to be. = at time t = a is Mat 180 www.timetodare.com Section.7 Derivatives and Rates of Cange Part II Section.8 Te Derivative as a Function Derivatives ( ) In te previous section we defined te slope of te tangent to a curve wit

More information

Pearson Physics Level 30 Unit VII Electromagnetic Radiation: Unit VII Review Solutions

Pearson Physics Level 30 Unit VII Electromagnetic Radiation: Unit VII Review Solutions Pearson Pysics Level 30 Unit VII Electromagnetic Radiation: Unit VII Review Solutions Student Book pages 746 749 Vocabulary 1. angle of diffraction: te angle formed between te perpendicular bisector and

More information

Downloaded from

Downloaded from UNIT VII- DUAL NATURE OF MATTER & RADIATION LIST OF FORMULAE 1. Energy of a photon E =hʋ = 2. Number of photon emitted per second N = 3. Momentum of photon P = mc = = = 4. Equivalent mass of photon m =

More information

Outline. MS121: IT Mathematics. Limits & Continuity Rates of Change & Tangents. Is there a limit to how fast a man can run?

Outline. MS121: IT Mathematics. Limits & Continuity Rates of Change & Tangents. Is there a limit to how fast a man can run? Outline MS11: IT Matematics Limits & Continuity & 1 Limits: Atletics Perspective Jon Carroll Scool of Matematical Sciences Dublin City University 3 Atletics Atletics Outline Is tere a limit to ow fast

More information

Exponentials and Logarithms Review Part 2: Exponentials

Exponentials and Logarithms Review Part 2: Exponentials Eponentials and Logaritms Review Part : Eponentials Notice te difference etween te functions: g( ) and f ( ) In te function g( ), te variale is te ase and te eponent is a constant. Tis is called a power

More information

Derivation Of The Schwarzschild Radius Without General Relativity

Derivation Of The Schwarzschild Radius Without General Relativity Derivation Of Te Scwarzscild Radius Witout General Relativity In tis paper I present an alternative metod of deriving te Scwarzscild radius of a black ole. Te metod uses tree of te Planck units formulas:

More information

Precalculus Test 2 Practice Questions Page 1. Note: You can expect other types of questions on the test than the ones presented here!

Precalculus Test 2 Practice Questions Page 1. Note: You can expect other types of questions on the test than the ones presented here! Precalculus Test 2 Practice Questions Page Note: You can expect oter types of questions on te test tan te ones presented ere! Questions Example. Find te vertex of te quadratic f(x) = 4x 2 x. Example 2.

More information

2.2 WAVE AND PARTICLE DUALITY OF RADIATION

2.2 WAVE AND PARTICLE DUALITY OF RADIATION Quantum Mecanics.1 INTRODUCTION Te motion of particles wic can be observed directly or troug microscope can be explained by classical mecanics. But wen te penomena like potoelectric effect, X-rays, ultraviolet

More information

SIMG Solution Set #5

SIMG Solution Set #5 SIMG-303-0033 Solution Set #5. Describe completely te state of polarization of eac of te following waves: (a) E [z,t] =ˆxE 0 cos [k 0 z ω 0 t] ŷe 0 cos [k 0 z ω 0 t] Bot components are traveling down te

More information

Physics 6C. De Broglie Wavelength Uncertainty Principle. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB

Physics 6C. De Broglie Wavelength Uncertainty Principle. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB Pyic 6C De Broglie Wavelengt Uncertainty Principle De Broglie Wavelengt Bot ligt and atter ave bot particle and wavelike propertie. We can calculate te wavelengt of eiter wit te ae forula: p v For large

More information

Some Review Problems for First Midterm Mathematics 1300, Calculus 1

Some Review Problems for First Midterm Mathematics 1300, Calculus 1 Some Review Problems for First Midterm Matematics 00, Calculus. Consider te trigonometric function f(t) wose grap is sown below. Write down a possible formula for f(t). Tis function appears to be an odd,

More information

DO NOT OPEN THIS EXAM UNTIL TOLD TO DO SO.

DO NOT OPEN THIS EXAM UNTIL TOLD TO DO SO. Exam 4.00 COMPREHENSIVE EXAM 7 May 2003 General Pysics II (PHSX 2020) Adam Jonston DO NOT OPEN THIS EXAM UNTIL TOLD TO DO SO. MAKE SURE TO PUT YOUR NAME AND SEAT NUMBER ON THE FIRST PAGE OF THE EXAM BEFORE

More information

Part C : Quantum Physics

Part C : Quantum Physics Part C : Quantum Pysics 1 Particle-wave duality 1.1 Te Bor model for te atom We begin our discussion of quantum pysics by discussing an early idea for atomic structure, te Bor model. Wile tis relies on

More information

Lesson 6: The Derivative

Lesson 6: The Derivative Lesson 6: Te Derivative Def. A difference quotient for a function as te form f(x + ) f(x) (x + ) x f(x + x) f(x) (x + x) x f(a + ) f(a) (a + ) a Notice tat a difference quotient always as te form of cange

More information

Quantum Mechanics and Atomic Theory

Quantum Mechanics and Atomic Theory A. Electromagnetic Radiation Quantum Mecanics and Atomic Teory 1. Ligt: consists of waves of oscillating electric field ( E ) and magnetic field ( B ) tat are perpendicular to eac oter and to te direction

More information

1. Consider the trigonometric function f(t) whose graph is shown below. Write down a possible formula for f(t).

1. Consider the trigonometric function f(t) whose graph is shown below. Write down a possible formula for f(t). . Consider te trigonometric function f(t) wose grap is sown below. Write down a possible formula for f(t). Tis function appears to be an odd, periodic function tat as been sifted upwards, so we will use

More information

Math Test No Calculator

Math Test No Calculator Mat Test No Calculator MINUTES, QUESTIONS Turn to Section of your answer seet to answer te questions in tis section. For questions -, solve eac problem, coose te best answer from te coices provided, and

More information

Lecture: Experimental Solid State Physics Today s Outline

Lecture: Experimental Solid State Physics Today s Outline Lecture: Experimental Solid State Pysics Today s Outline Te quantum caracter of particles : Wave-Particles dualism Heisenberg s uncertainty relation Te quantum structure of electrons in atoms Wave-particle

More information

Homework 1. L φ = mωr 2 = mυr, (1)

Homework 1. L φ = mωr 2 = mυr, (1) Homework 1 1. Problem: Streetman, Sixt Ed., Problem 2.2: Sow tat te tird Bor postulate, Eq. (2-5) (tat is, tat te angular momentum p θ around te polar axis is an integer multiple of te reduced Planck constant,

More information

UNIT : 3 STRUCTURE OF ATOM

UNIT : 3 STRUCTURE OF ATOM Composition of atom Electron ( e o ) () It was discovered by J.J. Tomson (897) and is negatively carged particle. () Electron is a component particle of catode rays. (3) Catode rays were discovered by

More information

Derivatives of Exponentials

Derivatives of Exponentials mat 0 more on derivatives: day 0 Derivatives of Eponentials Recall tat DEFINITION... An eponential function as te form f () =a, were te base is a real number a > 0. Te domain of an eponential function

More information

1watt=1W=1kg m 2 /s 3

1watt=1W=1kg m 2 /s 3 Appendix A Matematics Appendix A.1 Units To measure a pysical quantity, you need a standard. Eac pysical quantity as certain units. A unit is just a standard we use to compare, e.g. a ruler. In tis laboratory

More information

Section 15.6 Directional Derivatives and the Gradient Vector

Section 15.6 Directional Derivatives and the Gradient Vector Section 15.6 Directional Derivatives and te Gradient Vector Finding rates of cange in different directions Recall tat wen we first started considering derivatives of functions of more tan one variable,

More information

Bob Brown Math 251 Calculus 1 Chapter 3, Section 1 Completed 1 CCBC Dundalk

Bob Brown Math 251 Calculus 1 Chapter 3, Section 1 Completed 1 CCBC Dundalk Bob Brown Mat 251 Calculus 1 Capter 3, Section 1 Completed 1 Te Tangent Line Problem Te idea of a tangent line first arises in geometry in te context of a circle. But before we jump into a discussion of

More information

Phy 231 Sp 02 Homework #6 Page 1 of 4

Phy 231 Sp 02 Homework #6 Page 1 of 4 Py 231 Sp 02 Homework #6 Page 1 of 4 6-1A. Te force sown in te force-time diagram at te rigt versus time acts on a 2 kg mass. Wat is te impulse of te force on te mass from 0 to 5 sec? (a) 9 N-s (b) 6 N-s

More information

High potential difference + Gas. Manometer. Vacuum pump

High potential difference + Gas. Manometer. Vacuum pump Lig genius PHYSICS lectron, Poton, Potoelectric ffect and X-rays + lectric Discarge Troug Gases. At noral atosperic pressure, te gases are poor conductor of electricity. If we establis a potential difference

More information

ACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS 1 MATH00030 SEMESTER /2019

ACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS 1 MATH00030 SEMESTER /2019 ACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS MATH00030 SEMESTER 208/209 DR. ANTHONY BROWN 6. Differential Calculus 6.. Differentiation from First Principles. In tis capter, we will introduce

More information

Higher Derivatives. Differentiable Functions

Higher Derivatives. Differentiable Functions Calculus 1 Lia Vas Higer Derivatives. Differentiable Functions Te second derivative. Te derivative itself can be considered as a function. Te instantaneous rate of cange of tis function is te second derivative.

More information

5.1 We will begin this section with the definition of a rational expression. We

5.1 We will begin this section with the definition of a rational expression. We Basic Properties and Reducing to Lowest Terms 5.1 We will begin tis section wit te definition of a rational epression. We will ten state te two basic properties associated wit rational epressions and go

More information

WAVES AND PARTICLES. (c)

WAVES AND PARTICLES. (c) WAVES AND PARTICLES 1. An electron and a proton are accelerated through the same potential difference. The ration of their De Broglie wave length will be -- (a) (b) (c) (d) 1 2. What potential must be

More information

Math Module Preliminary Test Solutions

Math Module Preliminary Test Solutions SSEA Summer 207 Mat Module Preliminar Test Solutions. [3 points] Find all values of tat satisf =. Solution: = ( ) = ( ) = ( ) =. Tis means ( ) is positive. Tat is, 0, wic implies. 2. [6 points] Find all

More information

Downloaded from

Downloaded from 7. DUAL NATURE OF MATTER & RADIATION GIST ELECTRON EMISSION 1. There are three types of electron emission, namely, Thermionic Emission, Photoelectric Emission and Field Emission. 2. The minimum energy

More information

Graviton Induced Nuclear Fission through Electromagnetic Wave Flux Phil Russell, * Jerry Montgomery

Graviton Induced Nuclear Fission through Electromagnetic Wave Flux Phil Russell, * Jerry Montgomery Graviton Induced Nuclear Fission troug Electromagnetic Wave Flux Pil Russell, * Jerry Montgomery Nort Carolina Central University, Duram, NC 27707 Willowstick Tecnologies LLC, Draper, UT 84020 (Dated:

More information

MVT and Rolle s Theorem

MVT and Rolle s Theorem AP Calculus CHAPTER 4 WORKSHEET APPLICATIONS OF DIFFERENTIATION MVT and Rolle s Teorem Name Seat # Date UNLESS INDICATED, DO NOT USE YOUR CALCULATOR FOR ANY OF THESE QUESTIONS In problems 1 and, state

More information

DUAL NATURE OF RADIATION AND MATTER

DUAL NATURE OF RADIATION AND MATTER Chapter Eleven DUAL NATURE OF RADIATION AND MATTER MCQ I 111 A particle is dropped from a height H The de Broglie wavelength of the particle as a function of height is proportional to (a) H (b) H 1/2 (c)

More information

Lesson 4 - Limits & Instantaneous Rates of Change

Lesson 4 - Limits & Instantaneous Rates of Change Lesson Objectives Lesson 4 - Limits & Instantaneous Rates of Cange SL Topic 6 Calculus - Santowski 1. Calculate an instantaneous rate of cange using difference quotients and limits. Calculate instantaneous

More information

(c) (d) insufficient information

(c) (d) insufficient information Final Exam Pysics 130 Monday December 16, 00 Point distribution: Te multiple coice questions (1-5) are wort 5 points eac and answers sould be bubbled onto te answer seet. Questions 6-8 are long-answer

More information

The Doppler Factor and Quantum Electrodynamics Basics in Laser-Driven Light Sailing

The Doppler Factor and Quantum Electrodynamics Basics in Laser-Driven Light Sailing International Letters of Cemistry, Pysics and Astronomy Online: 013-10-0 ISSN: 99-3843, Vol. 19, pp 10-14 doi:10.1805/www.scipress.com/ilcpa.19.10 013 SciPress Ltd., Switzerland Te Doppler Factor and Quantum

More information

1 The concept of limits (p.217 p.229, p.242 p.249, p.255 p.256) 1.1 Limits Consider the function determined by the formula 3. x since at this point

1 The concept of limits (p.217 p.229, p.242 p.249, p.255 p.256) 1.1 Limits Consider the function determined by the formula 3. x since at this point MA00 Capter 6 Calculus and Basic Linear Algebra I Limits, Continuity and Differentiability Te concept of its (p.7 p.9, p.4 p.49, p.55 p.56). Limits Consider te function determined by te formula f Note

More information

Lecture XVII. Abstract We introduce the concept of directional derivative of a scalar function and discuss its relation with the gradient operator.

Lecture XVII. Abstract We introduce the concept of directional derivative of a scalar function and discuss its relation with the gradient operator. Lecture XVII Abstract We introduce te concept of directional derivative of a scalar function and discuss its relation wit te gradient operator. Directional derivative and gradient Te directional derivative

More information

Continuity and Differentiability Worksheet

Continuity and Differentiability Worksheet Continuity and Differentiability Workseet (Be sure tat you can also do te grapical eercises from te tet- Tese were not included below! Typical problems are like problems -3, p. 6; -3, p. 7; 33-34, p. 7;

More information

The Electron in a Potential

The Electron in a Potential Te Electron in a Potential Edwin F. Taylor July, 2000 1. Stopwatc rotation for an electron in a potential For a poton we found tat te and of te quantum stopwatc rotates wit frequency f given by te equation:

More information

REVIEW LAB ANSWER KEY

REVIEW LAB ANSWER KEY REVIEW LAB ANSWER KEY. Witout using SN, find te derivative of eac of te following (you do not need to simplify your answers): a. f x 3x 3 5x x 6 f x 3 3x 5 x 0 b. g x 4 x x x notice te trick ere! x x g

More information

. Compute the following limits.

. Compute the following limits. Today: Tangent Lines and te Derivative at a Point Warmup:. Let f(x) =x. Compute te following limits. f( + ) f() (a) lim f( +) f( ) (b) lim. Let g(x) = x. Compute te following limits. g(3 + ) g(3) (a) lim

More information

1 Power is transferred through a machine as shown. power input P I machine. power output P O. power loss P L. What is the efficiency of the machine?

1 Power is transferred through a machine as shown. power input P I machine. power output P O. power loss P L. What is the efficiency of the machine? 1 1 Power is transferred troug a macine as sown. power input P I macine power output P O power loss P L Wat is te efficiency of te macine? P I P L P P P O + P L I O P L P O P I 2 ir in a bicycle pump is

More information

Key Concepts. Important Techniques. 1. Average rate of change slope of a secant line. You will need two points ( a, the formula: to find value

Key Concepts. Important Techniques. 1. Average rate of change slope of a secant line. You will need two points ( a, the formula: to find value AB Calculus Unit Review Key Concepts Average and Instantaneous Speed Definition of Limit Properties of Limits One-sided and Two-sided Limits Sandwic Teorem Limits as x ± End Beaviour Models Continuity

More information

Differential Calculus (The basics) Prepared by Mr. C. Hull

Differential Calculus (The basics) Prepared by Mr. C. Hull Differential Calculus Te basics) A : Limits In tis work on limits, we will deal only wit functions i.e. tose relationsips in wic an input variable ) defines a unique output variable y). Wen we work wit

More information

NUMERICAL DIFFERENTIATION. James T. Smith San Francisco State University. In calculus classes, you compute derivatives algebraically: for example,

NUMERICAL DIFFERENTIATION. James T. Smith San Francisco State University. In calculus classes, you compute derivatives algebraically: for example, NUMERICAL DIFFERENTIATION James T Smit San Francisco State University In calculus classes, you compute derivatives algebraically: for example, f( x) = x + x f ( x) = x x Tis tecnique requires your knowing

More information

Lasers & Optical Fibers

Lasers & Optical Fibers Lasers & Optical Fibers 1. Emmission of a poton by an excited atom due to interaction wit passing poton nearby is called A) Spontaneous emission B) Stimulated emission C) induced absorption D) termionic

More information

The Derivative as a Function

The Derivative as a Function Section 2.2 Te Derivative as a Function 200 Kiryl Tsiscanka Te Derivative as a Function DEFINITION: Te derivative of a function f at a number a, denoted by f (a), is if tis limit exists. f (a) f(a + )

More information

Tangent Lines-1. Tangent Lines

Tangent Lines-1. Tangent Lines Tangent Lines- Tangent Lines In geometry, te tangent line to a circle wit centre O at a point A on te circle is defined to be te perpendicular line at A to te line OA. Te tangent lines ave te special property

More information

MAT 1339-S14 Class 2

MAT 1339-S14 Class 2 MAT 1339-S14 Class 2 July 07, 2014 Contents 1 Rate of Cange 1 1.5 Introduction to Derivatives....................... 1 2 Derivatives 5 2.1 Derivative of Polynomial function.................... 5 2.2 Te

More information

LIMITATIONS OF EULER S METHOD FOR NUMERICAL INTEGRATION

LIMITATIONS OF EULER S METHOD FOR NUMERICAL INTEGRATION LIMITATIONS OF EULER S METHOD FOR NUMERICAL INTEGRATION LAURA EVANS.. Introduction Not all differential equations can be explicitly solved for y. Tis can be problematic if we need to know te value of y

More information

APPENDIXES. Let the following constants be established for those using the active Mathcad

APPENDIXES. Let the following constants be established for those using the active Mathcad 3 APPENDIXES Let te following constants be establised for tose using te active Matcad form of tis book: m.. e 9.09389700 0 3 kg Electron rest mass. q.. o.6077330 0 9 coul Electron quantum carge. µ... o.5663706

More information