Vacuum tube - V, only for shorter than certain wavelength Current V VoVo Fixed wavelength Varying intensity I2I 3I Maximum electron energy 0.

Slides:



Advertisements
Similar presentations
1 My Chapter 27 Lecture. 2 Chapter 27: Early Quantum Physics and the Photon Blackbody Radiation The Photoelectric Effect Compton Scattering Early Models.
Advertisements

Quantum Physics ISAT 241 Analytical Methods III Fall 2003 David J. Lawrence.
Chapter 29 - Particles and Waves. 1.Who won the Nobel prize for his explanation of the photoelectric effect? A.Planck B.Bohr C.De Broglie D.Einstein 2.The.
BUSINESS 1.EXAM 2THURSDAY NOVEMBER 4, MATERIAL COVERED: CHAPTERS 4, 5 & 6 3.TIME:7:00PM-8:00PM 4.WHERE:(TO BE ANNOUNCED LATER) 5.WHAT TO BRING:CALCULATOR,
The Arrangement of Electrons in Atoms
The Development of a New Atomic Model.
Quantum Theory and the Electronic Structure of Atoms
6. Atomic and Nuclear Physics Chapter 6.4 Interactions of matter with energy.
Hydrogen Atom Coulomb force “confines” electron to region near proton => standing waves of certain energy + -
Electronic Structure of Atoms
ENERGY & LIGHT THE QUANTUM MECHANICAL MODEL. Atomic Models What was Rutherford’s model of the atom like? What is the significance of the proton? What.
Arrangement of Electrons in Atoms Part One Learning Objectives Read Pages Asgn #16: 103/1-6 1.
Classical vs Quantum Mechanics Rutherford’s model of the atom: electrons orbiting around a dense, massive positive nucleus Expected to be able to use classical.
Quantum Physics. Black Body Radiation Intensity of blackbody radiation Classical Rayleigh-Jeans law for radiation emission Planck’s expression h =
Early Quantum Theory and Models of the Atom
Quantum Mechanics Directly observing electrons in the atom is impossible, the electron is so small that observing it changes its behavior The quantum-mechanical.
Modern Physics.
Particle Nature of Light
Chapter 4 Arrangement of Electrons in Atoms
Modern Physics Previously we showed that Light behaves like sound. It has characteristics of waves Now we get to see how it also behaves like a particle.
Modern Physics Wave Particle Duality of Energy and Matter Is light a particle or a wave? We have see that light acts like a wave from polarization, diffraction,
Where are the electrons ? Rutherford found the nucleus to be in the center. He determined that the atom was mostly empty space. So, how are the electrons.
Midterm results will be posted downstairs (by the labs) this afternoon No office hours today.
Early Quantum Theory AP Physics Chapter 27. Early Quantum Theory 27.1 Discovery and Properties of the Electron.
Waves, Particles, and the Spectrum Quantum Theory.
As an object gets hot, it gives Off energy in the form of Electromagnetic radiation.
Quantum Physics. Quantum Theory Max Planck, examining heat radiation (ir light) proposes energy is quantized, or occurring in discrete small packets with.
Quantum Theory and the Electronic Structure of Atoms Chapter 7 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Arrangement of Electrons in Atoms The Development of a New Atomic Model.
Mullis1 Arrangement of Electrons in Atoms Principles of electromagnetic radiation led to Bohr’s model of the atom. Electron location is described using.
-The Bohr Model -The Quantum Mechanical Model Mrs. Coyle Chemistry.
The Wave – Particle Duality OR. Light Waves Until about 1900, the classical wave theory of light described most observed phenomenon. Light waves: Characterized.
Chapter 27- Atomic/Quantum Physics
Photons, Electrons, and Atoms. Visible and non-visable light Frequencies around Hz Much higher than electric circuits Theory was about vibrating.
Slide 1 of 38 chemistry. Slide 2 of 38 © Copyright Pearson Prentice Hall Physics and the Quantum Mechanical Model > Light The amplitude of a wave is the.
Quantum Theory & the History of Light
Quantum Physics   Quantum   The smallest quantity of a substance that still has the specific properties of that substance Discrete vs. Continuous 
Modern Chemistry Chapter 4 Arrangement of Electrons in Atoms Sections 1-3 The Development of a New Atomic Model The Quantum Model of the Atom Electron.
Development of a New Atomic Model Properties of Light.
4: Introduction to Quantum Physics
Enriched Chemistry Chapter 4 – Arrangement of Electrons in Atoms
 Waves & Energy H Ch 5&6. Waves  Vibrating disturbance by which energy is transmitted Amplitude (Wavelength) u = λν.
Chapter 33 Early Quantum Theory and Models of Atom.
QUANTUM AND NUCLEAR PHYSICS. Wave Particle Duality In some situations light exhibits properties that are wave-like or particle like. Light does not show.
Quantum Theory and the Electronic Structure of Atoms Chapter 7.
Chemistry I Chapter 4 Arrangement of Electrons. Electromagnetic Radiation Energy that exhibits wavelike behavior and travels through space Moves at the.
Light, Quantitized Energy & Quantum Theory CVHS Chemistry Ch 5.1 & 5.2.
Electromagnetic Radiation. Waves To understand the electronic structure of atoms, one must understand the nature of electromagnetic radiation. The distance.
Phy2005 Applied Physics II Spring 2016 Announcements: Final exam: 50% Chs % Chs Don’t forget course evaluations Go over posted practice.
Warm-Up What is the difference between the Bohr’s Model of the Atom and the Quantum Model of the atom. What wavelength is associated with an electron.
Quantum Mechanics and Atomic Physics
Electromagnetic Radiation
Chapter 6 Electronic Structure of Atoms
Arrangement of electrons in atoms
Electronic Structure and Light
Electromagnetic Radiation
Atomic Structure the wave nature of light 1 2 3 2 Hz 4 Hz 6 Hz 
Electrons and Light Chapter 13.3.
Chapter 27 Early Quantum Theory
Electrons.
I. Waves & Particles (p ) Ch. 4 - Electrons in Atoms I. Waves & Particles (p )
Light and Energy Electromagnetic Radiation is a form of energy that is created through the interaction of electrical and magnetic fields. It displays wave-like.
Arrangement of Electrons in Atoms
Quantum Mechanics.
Early Quantum Theory AP Physics Chapter 27.
II. Bohr Model of the Atom (p )
The Compton Effect (1923) Compton scattered short-wavelength light (X- rays) from different materials The scattered light had lower frequency than the.
c = speed of light (ms-1, constant)
Presentation transcript:

Vacuum tube - V, only for shorter than certain wavelength Current V VoVo Fixed wavelength Varying intensity I2I 3I Maximum electron energy 0

Current V < 2 < 3 Q.Why the maximum electron energy depend on the wavelength (frequency)? Why strong beams of long wavelength cannot knock out electrons? Classical EM theory (wave theory) tells us that the max electron energy should depend on only the intensity of the light. In 1900, Max Planck postulated that electromagnetic energy is emitted in discrete packets, or quanta. The energy of these quanta is proportional to the frequency of the radiation. E = hf = hc/ Huge water wave, large amplitude sound wave h = 6.6 x Js (Planck’s constant)

In explaining the photoelectric effect, Einstein picked up the idea of Planck, and proposed in 1905 that light was not only emitted by bundles of energy E = hf, but it was also absorbed in such bundles. Light Quanta = Photons Kinetic Energy of an electron = E photon - E threshold E photon = hc/ > E threshold Work function: depends on material ~ eV - light quantum: photon

In this case, light can be considered as a massless particle, photon with energy solely determined by its wavelength (frequency). There is no conflict with Einstein’s relativistic mechanics: massless particle can have speed of light! E = hf = hc/ h = 6.6 x Js (Planck’s constant) = 580 nm photon (yellow light) carries E = (6.6 x Js)(3 x 10 8 m/s)/(580 x m) = 3.4 x J

How do we understand the intensity of light? Intensity of light (EM radiation) ≈ number of photons with same wavelength or frequency Wave behaves like a particle. Does a particle behaves like wave?

Q. Light of wavelength 650 nm is required to cause electrons to be ejected barely from the surface of a particular metal. What is the kinetic energy of the ejected electrons if the surface is bombarded with light of wavelength 450 nm? “…ejected barely…” means that ejected electron has ≈ 0 kinetic energy. Kinetic Energy of an electron = E photon - E threshold h /c = E threshold (work function) for = 650 nm E threshold = (6.6 x Js)(3 x 10 8 m/s)/(659 x m) = 3.06 x J E k = (6.6 x Js)(3 x 10 8 m/s)/(450 x m) – 3.06 x = (4.42 – 3.06) x = 1.36 x J

A light source produces 400 nm wavelength. When the light strikes a metal surface, a stream of electrons emerges from the metal. If the intensity of the light is doubled, 1. the electrons emitted are more energetic. 2. more electrons are emitted in a given time interval 3. both of the above 4. none of the above

In this case, light can be considered as a massless particle, photon with energy solely determined by its wavelength (frequency). There is no conflict with Einstein’s relativistic mechanics: massless particle can have speed of light! E = hf = hc/ h = 6.6 x Js (Planck’s constant) = 580 nm photon (yellow light) carries E = (6.6 x Js)(3 x 10 8 m/s)/(580 x m) = 3.4 x J Wave behaves like a particle. Does a particle behaves like wave?

It would seem that the basic idea of the quantum theory is the impossibility of imagining an isolated quantity of energy without associating with it a certain frequency de Broglie in 1923 as a graduate student light quantum (photon) E = hf = hc/ Relativistic case massless E = pc = hc/ = h/p wave quantity particle quantity for m o = 0

= h/p De Broglie proposed that all particles (electrons) should have wavelength associated with their momentum in exactly the same manner. particlewave

Q. What is the de Broglie wavelength of an electron that has a kinetic energy of 100 eV? After an electron is accelerated in 100 V potential difference, its kinetic energy is 100 eV. eV unit has to be converted into SI unit, Joule. 1 eV = 1.6 x J E k = (1/2)m o v 2 = 1.6 x J v 2 = 2E k /m o = 2(1.6 x J)/(9.1 x kg) = 3.52 x m 2 /s 2 v = 5.93 x 10 6 m/s low speed: no need to use relativistic = h/p = h/m o v = (6.6 x Js)/(9.1 x kg x 5.93 x 10 6 m/s) = 1.23 x m = nm

C.J. Davisson and L.H Germer scattered low energy electrons off The Ni crystal and observed a peculiar pattern of scattered electrons. Diffraction pattern from the regular Crystalline structure of order of 0.1 nm size.

Hydrogen Spectrum Emission SPECTRUM ABSORPTION SPECTRUM

Bohr’s Hydrogen Atom and the Electron as a Wave Niels Bohr (1885 – 1962) Louis de Broglie (1892 – 1987) In 1913, Rutherford’s atom received a quantitative description from Niels Bohr who explained experimentally observed discrete nature of atomic spectrum of Hydrogen. In spite of its immediate success in providing theoretical account of the spectrum and other nature of Hydrogen atom, a complete understanding of Bohr’s atom came only after de Broglie’s conjecture (1923) that electrons should display wave properties. + -

Bohr’s Hydrogen Atom (1 proton and 1 electron) centripetal force = Coulomb force electron as a wave (de Broglie) 2  r =, 2, 3, … = h/mv This is the necessary condition for electron to maintain an orbit.

2  r =, 2, 3, … = h/mv 2  r n = nh/mv nn r n = (5.3 x )n 2 (m); v n = 2 x10 6 /n (m/s)n r n (nm) v n (m/s) x x x x  0.1 nm is the size of Hydrogen atom

Now, let’s think about the total energy of the electron in the n th orbit. E tot = Potential Energy + Kinetic Energy -ke 2 /r n (1/2)mv n 2n E n (eV) ∞0

E tot 0 n = ∞ eVn = 1 n = eV n = eV - Ionized state of Hydrogen: proton

Electron Energy diagram of Hydrogen atom E tot 0 n = ∞ n = eV n = eV n = eV - lowest energy: ground state Electron has to absorb 10.2 eV energy for this - Electron has to absorb 12.1 eV energy for this

in eV (Rydberg const.) E(n  m) or  < 0Absorb photons of a given E (n  m) or > 0Emit photons of a given E = hc/

E tot 0 n = ∞ n = eV n = eV n = eV - E (1  2) = 10.2 eV = 10.2 x (1.6 x J/eV) = 1.63 x J E = hc/  = 121 nm Ultraviolet range

Q What is the longest wavelength em radiation that can ionize unexcited hydrogen atom? smallest energy ground state (n = 1) n = 1  m = ∞ 1/ = (1.097 x 10 7 ) x (0 – 1) = x 10 7 (m -1 ) = x (m) = (nm) (- means absorption)

Q. What is the shortest wavelength for the Balmer series? Largest energy difference in Balmer series From n = ∞ to m = 2 (Balmer) = (R x (1/4 – 0)) -1 = 365 nm The Balmer series are in the visible range.