PHYS 280 Week 7 Homework Summer Choose the better choice of all choices given.

Similar documents
PHYS 280 Week 7 Homework Summer Choose the better choice of all choices given.

PHYS 280 Practice Final Exam Summer Choose the better choice of all choices given.

PHYS 280 Practice Final Exam Summer Choose the better choice of all choices given.

Physics 280 Quantum Mechanics Lecture

Explain how Planck resolved the ultraviolet catastrophe in blackbody radiation. Calculate energy of quanta using Planck s equation.

IB Physics SL Y2 Option B (Quantum and Nuclear Physics) Exam Study Guide Practice Problem Solutions

Lecture Outline Chapter 30. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc.

Constants & Atomic Data. The birth of atomic physics and quantum mechanics. debroglie s Wave Equations. Energy Calculations. λ = f = h E.

The birth of atomic physics and quantum mechanics. Honors Physics Don Rhine

Supplemental Activities. Module: Atomic Theory. Section: Electromagnetic Radiation and Matter

LECTURE 6 QUANTUM PHYSICS II. Instructor: Shih-Chieh Hsu

Modern Physics Lesson 1: Intro to Quantum Mechanics and Photoelectric Effect Lesson 2: Energy Levels Lesson 3: E = mc^2 Lesson 4: Standard Model of

Physics 1C. Lecture 27A

Introduction to Quantum Physics. Early Atomic Physics

CHEMISTRY 113 EXAM 3(A)

Recall the Goal. What IS the structure of an atom? What are the properties of atoms?

SPARKS CH301. Why are there no blue fireworks? LIGHT, ELECTRONS & QUANTUM MODEL. UNIT 2 Day 2. LM15, 16 & 17 due W 8:45AM

Preview. Atomic Physics Section 1. Section 1 Quantization of Energy. Section 2 Models of the Atom. Section 3 Quantum Mechanics

ATOMIC STRUCTURE, ELECTRONS, AND PERIODICITY

/60 (multiple choice) II /20 III /30 IV /10 V /60 (essay)

8 Wavefunctions - Schrödinger s Equation

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS

Quantum Mysteries. Scott N. Walck. September 2, 2018

Electronic Structure of Atoms. Chapter 6

Chapter 28 Quantum Mechanics of Atoms

Chem 1A, Fall 2015, Midterm Exam 1. Version A September 21, 2015 (Prof. Head-Gordon) 2

The Bohr Model of Hydrogen, a Summary, Review

Chemistry is in the electrons

Exam 2 Development of Quantum Mechanics

CHAPTER 4. Arrangement of Electrons in Atoms

Atomic Structure. Standing Waves x10 8 m/s. (or Hz or 1/s) λ Node

27-1 Planck Solves the Ultraviolet Catastrophe

Wave nature of particles

( ) # velocity. Wavelengths of massive objects. From Last Time. Wavelength of electron. Wavelength of 1 ev electron. A little complicated ( ) " = h mv

ATOMIC STRUCTURE, ELECTRONS, AND PERIODICITY

Quantum Theory of Light

PHYS 280 Quantum I: Tools Summer Theoretical Catastrophe, Unwanted Solutions, and the Quantum Revolution

Test Bank for General Chemistry Atoms First 2nd Edition by John E. McMurry and Robert C. Fay

Supplemental Activities. Module: Atomic Theory. Section: Electromagnetic Radiation and Matter - Key

Particle nature of light & Quantization

Topic 12: Quantum numbers. Heisenberg, Schrodinger, Quantum Theory, Quantum numbers, Practice

Sometimes light acts like a wave Reminder: Schedule changes (see web page)

Physics 1C Lecture 29A. Finish off Ch. 28 Start Ch. 29

Lecture 9: Introduction to QM: Review and Examples

SPH4U UNIVERSITY PHYSICS

The Atom. Result for Hydrogen. For example: the emission spectrum of Hydrogen: Screen. light. Hydrogen gas. Diffraction grating (or prism)

Alan Mortimer PhD. Ideas of Modern Physics

Electrons in Atoms. Before You Read. Chapter 4. Review the structure of the atom by completing the following table.

General Physics (PHY 2140) Lecture 15

Title / paragraph example Topic: Quantum Computers. Course Essay. Photoelectric effect summary. From Last Time. Compton scattering

Modern Physics Part 1: Quantization & Photons

Unit 4. Electrons in Atoms

Exam Results. Force between charges. Electric field lines. Other particles and fields

Chapter 37 Early Quantum Theory and Models of the Atom. Copyright 2009 Pearson Education, Inc.

Chapter 7. Quantum Theory and Atomic Structure

Physics 107 Final Exam May 6, Your Name: 1. Questions

PHYS 202. Lecture 23 Professor Stephen Thornton April 20, 2006

Blackbody radiation The photoelectric effect Compton effect Line spectra Nuclear physics/bohr model Lasers Quantum mechanics

Einstein. Quantum Physics at a glance. Planck s Hypothesis (blackbody radiation) (ultraviolet catastrophe) Quantized Energy

UNM Physics 262, Fall 2006 SAMPLE Midterm Exam 3: Quantum Mechanics

4.2 A Scientific View of Energy Kinetic Energy

Modern Physics Part 3: Bohr Model & Matter Waves

The Electron Cloud. Here is what we know about the electron cloud:

Chapter 27. Quantum Physics

Chapter 7. The Quantum Mechanical Model of the Atom

November 06, Chapter 7 Atomic Struture. CHAPTER 7 Atomic Structure. Oct 27 9:34 AM ATOMIC STRUCTURE. Oct 27 9:34 AM

2) The number of cycles that pass through a stationary point is called A) wavelength. B) amplitude. C) frequency. D) area. E) median.

Chapter 7 Atomic Structure and Orbitals

Early Quantum Theory and Models of the Atom

Class 21. Early Quantum Mechanics and the Wave Nature of Matter. Physics 106. Winter Press CTRL-L to view as a slide show. Class 21.

Electronic structure of atoms

Yellow. Strontium red white. green. yellow violet. green. red. Chapter 4. Arrangement of Electrons in Atoms. Table of Contents

General Physics (PHY 2140)

Radiation - Electromagnetic Waves (EMR): wave consisting of oscillating electric and magnetic fields that move at the speed of light through space.

Chapter 38. Photons and Matter Waves

Chapter 1. From Classical to Quantum Mechanics

CHAPTER 27 Quantum Physics

The temperature of a lava flow can be approximated by merely observing its colour. The result agrees nicely with the measured temperatures of lava

Homework 04 - Electromagnetic Radiation

Quantum Physics and Atomic Models Chapter Questions. 1. How was it determined that cathode rays possessed a negative charge?

Notes for Special Relativity, Quantum Mechanics, and Nuclear Physics

PHYSICS 3204 PUBLIC EXAM QUESTIONS (Quantum pt.1)

We also find the development of famous Schrodinger equation to describe the quantization of energy levels of atoms.

Physics and the Quantum Mechanical Model

Chem 3502/4502 Physical Chemistry II (Quantum Mechanics) 3 Credits Spring Semester 2006 Christopher J. Cramer. Lecture 20, March 8, 2006

Semiconductor Physics and Devices

PHYS 202. Lecture 23 Professor Stephen Thornton April 25, 2005

Physics 116. Nov 21, Session 31 De Broglie, duality, and uncertainty. R. J. Wilkes

Chapter 28: Quantum Physics. Don t Copy This. Quantum Physics 3/16/13

normalized spectral amplitude R(λ)

September 06, A B Which is which? What does Planck suggest? instead of resonantors being able to emit energy at any speed or energy?

CHE3935. Lecture 2. Introduction to Quantum Mechanics

If electrons moved in simple orbits, p and x could be determined, but this violates the Heisenberg Uncertainty Principle.

ATOMIC STRUCTURE. Kotz Ch 7 & Ch 22 (sect 4,5)

4/14/2015. Models of the Atom. Quantum Physics versus Classical Physics The Thirty-Year War ( ) Classical Model of Atom

General Chemistry. Contents. Chapter 9: Electrons in Atoms. Contents. 9-1 Electromagnetic Radiation. EM Radiation. Frequency, Wavelength and Velocity

CHAPTER 2: POSTULATES OF QUANTUM MECHANICS

Chapter 6 Electronic Structure of Atoms

Chemistry 1B-01, Fall 2013 Lectures 1-2

Fundamentals of Spectroscopy for Optical Remote Sensing. Course Outline 2009

Transcription:

PHYS 28 Week 7 Homework Summer 26 Name: Multiple Choice Choose the better choice of all choices given.. 2 points How many electrons can fit in one electron orbital shell? A. Only one B. Only two C. Only three D. Unlimited. 2. 2 points Which of the following isn t a truth about quantum mechanics? A. Energy is quantized B. Particles have wavelike properties. C. A cat can be dead and alive at the same time. D. A particle can be in a combination of two different states. 3. 2 points Given what we ve learned about relativity, which of the following is better to say than matter can neither be created nor destroyed : A. Matter can be converted to waves. B. Matter can be converted to particles. C. Matter exists as a particle and wave at the same time. D. Mass and energy can be seen as two names for the same underlying, conserved physical quantity. 4. 2 points Which of the following problem in physics wasn t fixed by quantum mechanics? A. The ultraviolet catastrophe of blackbody radiation B. The photoelectric mystery C. The helium spectrum mystery D. The contradiction between the universal speed of light and Galilean transforms. 5. 2 points Planck s quantization of energy was a desperate attempt to resolve the A. twin paradox. B. ultraviolet catastrophe. C. photoelectric mystery.

PHYS 28 Week 7 2 of 5 Summer 26 D. spectrum of hydrogen mystery. 6. 2 points We don t experience energy quantization in the everyday world because at our size A. the spaces between energy levels is too small to see with our senses. B. quantum mechanics isn t true on the macroscopic scale. C. energy becomes continuous past n = 493, 523, 235, 674, 453, 23, 956. 7. 2 points If I know the velocity of a subatomic particle precisely, then A. I know nothing about the particle s position. B. I known a very limited amount about the particle s position. C. The particle must be at rest. D. The particle can t be at rest. Problems 8. 5 points An HCL molecule vibrates with a frequency of 8. 3 Hz. What is the smallest possible change of energy that this molecule could experience? E = hf = 6.63 34 Js ( 8. 3 Hz ) = 5.4 2 J =.34eV 9. 5 points How much energy is needed to ionize a hydrogen atom in the n = 2 state? What frequency photon would that require? E ion = E n = 3.6eV n 2 = 3.4 ev

PHYS 28 Week 7 3 of 5 Summer 26. 5 points What percentage of mass does a hydrogen atom lose when it transitions from the n = 3 to the n = state (in other words, m/m )? The rest mass of hydrogen is m c 2 = 939 6 ev. m m = ( E c 2 ) m = E ( 3.6 ev = m c2 939 6 ev 3 2 ) =.29 8. Scientist A measures a quantum system by injecting an electron into a potential well, measuring its position with a laser beam (by finding where the photons reflect using Compton s equation, for example). After each measurement of its position, Scientist A flushes the electron out and repeats the measurement thousands upon thousands of times. (a) 4 points Each time the scientist locate the electron, will they see it as a wave or as a particle or something else? They will see it as a particle in each individual study, but as a probablistic distribution they will see wave-like manifestations. (b) point If the scientist were also to obtain some information about the momentum of the particle, what equation relates how accurately we can determine its momentum and position? x p 2 (c) 5 points After doing this thousands of times, the scientist finds that the probability of locating the particle in the well is: P (x) = 3 8 x2 What is the quantum wave function for the electron in this well, ψ(x)? Just a note, this wave function isn t physically realistic. Since P (x) = ψ 2 (x) for simple functions, then ψ(x) = P (x) = 3 8 x

PHYS 28 Week 7 4 of 5 Summer 26 Again, it is important to note that this is a dummy function and isn t physicall reasonable. (d) 5 points How long is the well? Hint: Assume that the left side of the well starts at x = and recall that the probability over the entire well has to equal. L 3 8 x2 dx = 3 x 3 8 3 L = 3 L 3 8 3 L = 2 (e) 3 points Name three effects that we see in quantum mechanics that we don t see in our everday lives. 2. 5 points An electron moves in a straight line with constant speed v =. 6 m/s which has been measured with precision of.%. What is the best possible precision in which its position could be measured? Recall that we require from the Heisenberg Uncertainty Principle that Here we have, x p 2 p = m e v = m e (.)(. 6 m/s) = m e. 5 m/s then, in the best case scenario, x = x p = 2 x = 2 p 2m e. 5 m/s = 5.26 m 3. 5 points Suppose a particle is confined to the x-axis from x = to x = 3, and that its wave function is given as ψ(x) = Ax. What is A? Note, this isn t a realistic function, just one that is solvable without tables of integrals.

PHYS 28 Week 7 5 of 5 Summer 26 We will use the normalization condition to solve for this: 3 ψ 2 (x)dx = 3 Thus A = /3 and the full wave function is: ψ(x) 2 = A 2 x 2 dx = A2 3 x3 3 = 9A2 = ψ(x) = x 3 4. 5 points Using the function from the previous problem, find the probability of finding the particle between x = and x = 2. P (x (, 2)) = 2 ψ 2 (x)dx = 2 x 2 x3 dx = 9 27 2 = 8 27 =.3 End of exam