Presented by Group 6: Neal Boseman, Vessen Hopkins, and Sarah Moorman.

Slides:



Advertisements
Similar presentations
Universe Eighth Edition Universe Roger A. Freedman William J. Kaufmann III CHAPTER 5 The Nature of Light CHAPTER 5 The Nature of Light.
Advertisements

Astronomy 201 Classical and Modern Astronomy Week 5 Slide Set 1 TAKE HOME TEST 3 HANDOUT TODAY! T3 & ADLER REPORTS DUE in 3 WKS on April 11. HW5 is due.
Kirchoff’s Loop Theorem
Blackbody Radiation & Planck’s Hypothesis
2. The Particle-like Properties Of Electromagnetic Radiation
Blackbody Radiation & Planck’s Hypothesis
Chapter 4 The Origin and Nature of Light
3RF Sciences, LLC. Blackbody defined…  A blackbody is an object that absorbs all light that hits it  Also emits light provided that its temperature.
1 Quantum Theory 1. 2 Topics l Discovery of the Electron l Millikan’s Experiment l Blackbody Radiation l An Act of Desperation l Summary.
What are the 3 ways heat can be transferred? Radiation: transfer by electromagnetic waves. Conduction: transfer by molecular collisions. Convection: transfer.
Introduction to Quantum Physics
Modern Physics (PC300) Class #10: 1)Experimental basis for the Introduction of Quantum Theory a) Photoelectric Effect b) X-Ray Production c) Charge/mass.
Astronomy 1 – Winter 2011 Lecture 7; January
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.
Black Body radiation Hot filament glows.
Lecture 5: Thermal Emission Chapter 6, Petty We thank Prof. Cheng-ta Cheng for sharing his online notes on this subject.
Modern Physics (PC300) Class #9: Introductory Stuff towards Quantum Mechanics.
Radiation PHYS390 (Astrophysics) Professor Lee Carkner Lecture 3.
Quantum physics. Quantum physics grew out failures of classical physics which found some quantum remedies in the Planck hypothesis and wave-particle duality.
Light as a Particle. Objectives  Define a quantum  Calculate the energy of a photon  Relate photon energy to wavelength and frequency of EMR.
Physics 361 Principles of Modern Physics Lecture 3.
Lecture 1 Quantization of energy. Quantization of energy Energies are discrete (“quantized”) and not continuous. This quantization principle cannot be.
WHAT IS A QUANTUM THEORY ? Quantum theory is the theoretical basis of modern physics that explains the nature and behavior of matter and energy on the.
Radiation: Processes and Properties -Basic Principles and Definitions- Chapter 12 Sections 12.1 through 12.3.
Blackbody Radiation & Atomic Spectra. “Light” – From gamma-rays to radio waves The vast majority of information we have about astronomical objects comes.
 Radiation emitted by hot objects is called thermal radiation.  Recall that the total radiation power emitted is proportional to T 4, where T is the.
Electromagnetic Radiation. Is light a wave or a particle? Yes It’s both, and neither At atomic scales, we have no exact analogs for phenomena For some.
Chapter 39 Particles Behaving as Waves
Lecture 4a. Blackbody Radiation Energy Spectrum of Blackbody Radiation - Rayleigh-Jeans Law - Rayleigh-Jeans Law - Wien’s Law - Wien’s Law - Stefan-Boltzmann.
Advanced Heat Transfer - Prof. Dr.-Ing. R. Weber - Winter 2005/ Lecture 1 (Governing Laws) Lecture-1. Governing Laws for Thermal Radiation Contents.
The Particlelike Properties of Electromagnetics Radiation Wei-Li Chen 10/27/2014.
Donna Kubik PHYS162 Fall, Because of its electric and magnetic properties, light is called electromagnetic radiation. It consists of perpendicular,
Photon Statistics Blackbody Radiation 1.The energy loss of a hot body is attributable to the emission of electromagnetic waves from the body. 2.The.
Physics 1C Lecture 28A. Blackbody Radiation Any object emits EM radiation (thermal radiation). A blackbody is any body that is a perfect absorber or emitter.
Radiation Fundamental Concepts EGR 4345 Heat Transfer.
Radiation Heat Transfer EGR 4345 Heat Transfer. Blackbody Radiation Blackbody – a perfect emitter & absorber of radiation Emits radiation uniformly in.
1 PHYS 3313 – Section 001 Lecture #9 Wednesday, Feb. 12, 2014 Dr. Jaehoon Yu Determination of Electron Charge Line Spectra Blackbody Radiation Wednesday,
Blackbody Spectrum Remember that EMR is characterized by wavelength (frequency) Spectrum: distribution of wavelength (or frequency) of some EMR Blackbody:
Physics 2170 – Spring Investigating electromagnetic radiation First midterm is 7:30pm on 2/17/09 Problem.
ATTENTION: EXAM next FRIDAY (one week)!! * Exam covers the reading Chapters 1-6 * Sample questions on the web. HW – due Wednesday midnight.
Introduction to Thermal Radiation and Radiation Heat Transfer.
Physics 1202: Lecture 30 Today’s Agenda Announcements: Extra creditsExtra credits –Final-like problems –Team in class HW 9 next FridayHW 9 next Friday.
Lecture 27 — The Planck Distribution Chapter 8, Friday March 21 st Quick review of exam 2 Black-body radiation Before Planck: Wien and Rayleigh-Jeans The.
4: Introduction to Quantum Physics
Wednesday, Feb. 25, 2015 PHYS , Spring 2014 Dr. Jaehoon Yu 1 PHYS 3313 – Section 001 Lecture #10 Wednesday, Feb. 25, 2015 Dr. Jaehoon Yu Blackbody.
Lecture_02: Outline Thermal Emission
Radiation Heat Transfer
Radiation (Ch 12 YAC) Thermal energy is emitted by matter as a result of vibrational and rotational motion of molecules, atoms and electrons. The energy.
Dualisme Cahaya Sebagai Gelombang dan Partikel
Light is a Particle Physics 12.
Quantum Theory By: Lucas, Steven, Brandon and Kristen.
IB Physics 12 Mr. Jean February 5 th, The plan: Video clip of the day. Quantum Theory Energy Levels.
Electromagnetic Radiation, Atomic Structure & Spectra.
Blackbody Radiation A blackbody is something that absorbs all radiation that shines on it Are all blackbodies black? - no!! - imagine a box full of lava.
NATS From the Cosmos to Earth Light as a Wave For a wave, its speed: s = l x f But the speed of light is a constant, c. For light: l x f = c The.
Blackbody. Kirchhoff’s Radiation  Radiated electromagnetic energy is the source of radiated thermal energy. Depends on wavelengthDepends on wavelength.
Light is a Particle Physics 12 Adv. Blackbody Radiation A blackbody is a perfect emitter; that is it emits the complete EM spectrum Work done by Gustav.
3.1 Discovery of the X-Ray and the Electron 3.2Determination of Electron Charge 3.3Line Spectra 3.4Quantization 3.5Blackbody Radiation 3.6Photoelectric.
Cool, invisible galactic gas (60 K, f peak in low radio frequencies) Dim, young star (600K, f peak in infrared) The Sun’s surface (6000K, f peak in visible)
Max Karl Ernst Ludwig Planck ( )
Plan for Today (AP Physics 2) Questions on HW (due tomorrow) Notes/Lecture on Blackbody Radiation.
PHYS 3313 – Section 001 Lecture #9
The Planck Distribution
VISHWAKARMA GOVERNMENT ENGINEERING COLLEGE
Early Quantum Theory and Models of the Atom
Max Karl Ernst Ludwig Planck ( )
Black Body Radiation Mr. Sonaji V. Gayakwad Asst. professor
Blackbody Radiation All bodies at a temperature T emit and absorb thermal electromagnetic radiation Blackbody radiation In thermal equilibrium, the power.
Blackbody Radiation All bodies at a temperature T emit and absorb thermal electromagnetic radiation Blackbody radiation In thermal equilibrium, the power.
PHYS 3313 – Section 001 Lecture #10
Presentation transcript:

Presented by Group 6: Neal Boseman, Vessen Hopkins, and Sarah Moorman

 What is Blackbody Radiation?  History of Blackbody Radiation  How has this discovery impacted Modern Physics?  Applications of Blackbody Radiation

 German physicist  3/12/1824 – 10/17/1887  Contributed in the Areas of: - Electrical Circuits - Spectroscopy - Blackbody Radiation Image Credit: Hulton Archive/Getty Images

 Spectroscopy - is the scientific study of an object based on the dispersion of said object’s light into its component colors.

1. Hot, dense object will produce a Continuous Spectrum. - This is what Kirchhoff termed a Blackbody. 2. Hot, low density object will produce an Emission Line Spectrum. 3. A cool, low density gas in front of a continuous light source will produce an Absorption Line Spectrum.

 Theorized in 1859 by Gustav Kirchhoff.  An ideal physical body.  Absorbs 100% of all incident radiation and reflects or transmits none.  Emits 100% radiation. Image Credit: NASA

 A Blackbody in thermal equilibrium emits EM radiation termed Blackbody Radiation.  Universal Property: Independent of material used.  Led to relation between radiation intensity ( I ), temperature ( T ), and wavelength ( λ ).  Blackbody Curves  Helped prove thermal radiation was also EM radiation.  Many physicist attempted to characterize shape of Blackbody curve…

Image credit:

 Wien’s Displacement Law :  Relation between peak wavelength and temperature.  Stefan-Boltzmann Law :  Relation between temperature and the power per unit area.  Rayleigh-Jeans Formula :  Relation between radiation intensity, temperature, and wavelength.  Ultraviolet Catastrophe!

Image credit:

 Rayleigh-Jeans Formula  Rayleigh-Jeans model failed to comply with experimental data at high frequencies  Wien’s Radiation Law  Wien's model failed to comply with experimental data at low frequencies.

 (Apr to Oct. 1947)  Approach to Blackbody Radiation Problem  Planck’s Radiation Law  Mathematical Trick  h = Planck’s Constant  Discrete Values of Energy: E = nhf Image credit: Hulton Archive/Getty Images

 Led to established relationships between light intensity, wavelength, and temperature:  Wien’s Displacement Law  Stefan-Boltzmann Law  Rayleigh-Jeans Formula  UV Catastrophe  Planck’s Radiation Law  Discrete Values Led to Best Fit for Experimental Data – Planck’s Mathematical Guess  Thus We Have Quantization of Energy: E = nhf  Implications for What’s Occurring at Atomic Level.  Birth of Quantum Mechanics!

 Gave people the ability to calculate temperatures of distance cosmic bodies  Inspired new devices such as thermal vision and new types of thermometers

 Thornton, Stephen T., and Andrew F. Rex. "The Experimental Basis of Quantum Physics." Modern Physics for Scientists and Engineers. 4th ed. Boston, MA: Cengage Learning, N. pag. Print.  Kirchhoff, G. (1860). "Ueber das Verhältniss zwischen dem Emissionsvermögen und dem Absorptionsvermögen der Körper für Wärme and Licht". Annalen der Physik und Chemie 109 (2): 275–301.Bibcode:1860AnP K. doi: /andp Translated by Guthrie, F. as Kirchhoff, G. (1860). "On the relation between the radiating and absorbing powers of different bodies for light and heat". Philosophical Magazine. Series 4 20 : 1–21.  Planck, Max (1901). "On the Law of Distribution of Energy in the Normal Spectrum". Annalen der Physik 4 : 553. Bibcode:1901AnP P.doi: /andp  Fowler, Michael. "Planck’s Route to the Black Body Radiation Formula and Quantization." Lecture. 25 July Web. 1 Dec