ELECTROMAGNETIC SPECTRUM LEARNING CHECK 2/1/16. What experiment proved light behaves as a wave? What experiment proved light behaves as a par6cle?

Similar documents
1/25/16 ANNOUNCEMENTS SELECTING AN ANALYTICAL METHOD

Light- Ma*er Interac0ons CHEM 314

JABLONSKI DIAGRAM INTERACTIONS BETWEEN LIGHT AND MATTER LIGHT AS A WAVE LIGHT AS A PARTICLE 2/1/16. Photoelectric effect Absorp<on Emission ScaDering

JABLONSKI DIAGRAM 2/15/16

Lecture 3: Light absorbance

An Introduction to Ultraviolet-Visible Molecular Spectrometry (Chapter 13)

What is spectroscopy?

RED. BLUE Light. Light-Matter

Analytical Chemistry II

24 Introduction to Spectrochemical Methods

Chem 321 Lecture 18 - Spectrophotometry 10/31/13

R O Y G B V. Spin States. Outer Shell Electrons. Molecular Rotations. Inner Shell Electrons. Molecular Vibrations. Nuclear Transitions

Introduction to Spectroscopic methods

Because light behaves like a wave, we can describe it in one of two ways by its wavelength or by its frequency.

10/2/2008. hc λ. νλ =c. proportional to frequency. Energy is inversely proportional to wavelength And is directly proportional to wavenumber

5.33 Lecture Notes: Introduction to Spectroscopy

Reference literature. (See: CHEM 2470 notes, Module 8 Textbook 6th ed., Chapters )

CHEM*3440. Photon Energy Units. Spectrum of Electromagnetic Radiation. Chemical Instrumentation. Spectroscopic Experimental Concept.

Chapter 17: Fundamentals of Spectrophotometry

JURONG JUNIOR COLLEGE J2 H1 Physics (2011) 1 Light of wavelength 436 nm is used to illuminate the surface of a piece of clean sodium metal in vacuum.

two slits and 5 slits

Singlet. Fluorescence Spectroscopy * LUMO

Chem Homework Set Answers

CHEM Atomic and Molecular Spectroscopy

Chapter 17: Fundamentals of Spectrophotometry

The Photoelectric Effect

Determining Riboflavin Content in a Multivitamin: Things to do before the lab

Reflection = EM strikes a boundary between two media differing in η and bounces back

Chemistry Instrumental Analysis Lecture 3. Chem 4631

What the Einstein Relations Tell Us

Spectroscopy. Page 1 of 8 L.Pillay (2012)

Spectroscopy Problem Set February 22, 2018

Chapter 4 Ultraviolet and visible spectroscopy Molecular Spectrophotometry

Chapter 10: Wave Properties of Particles

Reflection = EM strikes a boundary between two media differing in η and bounces back

Chapter 38. Photons Light Waves Behaving as Particles

Reference. What is spectroscopy? What is Light? / EMR 11/15/2015. Principles of Spectroscopy. Processes in Spectroscopy

Absorption, Emission and Fluorescence Spectroscopies. Chem M3LC. R. Corn

Absorption, Emission and Fluorescence Spectroscopies. R. Corn - Chem M3LC

Introduction. Molecules, Light and Natural Dyes. Experiment

Fluorescence Workshop UMN Physics June 8-10, 2006 Basic Spectroscopic Principles Joachim Mueller

Introduction to Chemical Research (CHEM 294) Introduction to Chemical Research (CHEM 294)

Introduction ENERGY. Heat Electricity Electromagnetic irradiation (light)

Spectroscopy II Introduction: Spectrophotometry and Fluorometry

Chemistry Instrumental Analysis Lecture 19 Chapter 12. Chem 4631

Beer's Law and Data Analysis *

Physics 126 Practice Exam #4 Professor Siegel

Chapter 13 An Introduction to Ultraviolet/Visible Molecular Absorption Spectrometry

Paper 2. Section B : Atomic World

Wavelength λ Velocity v. Electric Field Strength Amplitude A. Time t or Distance x time for 1 λ to pass fixed point. # of λ passing per s ν= 1 p

Photoelectric effect

Ultraviolet-Visible Spectroscopy

CHAPTER 12 TEST REVIEW

Chapter 9: Quantization of Light

Complete the following. Clearly mark your answers. YOU MUST SHOW YOUR WORK TO RECEIVE CREDIT.

Chem 434 -Instrumental Analysis Hour Exam 1

The ROXI Colorimeter & Fluorimeter. Laboratory Application I. Colorimetric measurements via Beer s Law.

Chapter 18. Fundamentals of Spectrophotometry. Properties of Light

Model Answer (Paper code: AR-7112) M. Sc. (Physics) IV Semester Paper I: Laser Physics and Spectroscopy

9/28/10. Visible and Ultraviolet Molecular Spectroscopy - (S-H-C Chapters 13-14) Valence Electronic Structure. n σ* transitions

Spectroscopy: Introduction. Required reading Chapter 18 (pages ) Chapter 20 (pages )

Skoog Chapter 6 Introduction to Spectrometric Methods

Chem 155 Midterm Exam Page 1 of 10 Spring 2010 Terrill

Spectrophotometry. Introduction

Chapter 5 Electrons In Atoms

Chemistry 2. Molecular Photophysics

Semiconductor Physics and Devices

LABORATORY OF ELEMENTARY BIOPHYSICS

hν' Φ e - Gamma spectroscopy - Prelab questions 1. What characteristics distinguish x-rays from gamma rays? Is either more intrinsically dangerous?

Skoog Chapter 7 Components of Optical Instruments

Chemistry Instrumental Analysis Lecture 2. Chem 4631

PARTICLES AND WAVES CHAPTER 29 CONCEPTUAL QUESTIONS

AS 101: Day Lab #2 Summer Spectroscopy

Energy and the Quantum Theory

6. A solution of red Kool-Aid transmits light at a wavelength range of nm.

Ch. 6: Introduction to Spectroscopic methods

Basics of UV-Visible Spectroscopy *

Lecture 36 Chapter 31 Light Quanta Matter Waves Uncertainty Principle

Assumed knowledge. Chemistry 2. Learning outcomes. Electronic spectroscopy of polyatomic molecules. Franck-Condon Principle (reprise)

Chemistry 311: Instrumentation Analysis Topic 2: Atomic Spectroscopy. Chemistry 311: Instrumentation Analysis Topic 2: Atomic Spectroscopy

Neutron Physics. The De Broglie relation for matter is: h mv (1) λ =

Ch 313 FINAL EXAM OUTLINE Spring 2010

Spectroscopy Chapter 13

Chapter 3. Electromagnetic Theory, Photons. and Light. Lecture 7

CHEM 115 Waves, Radiation, and Spectroscopy

Particle Detectors and Quantum Physics (2) Stefan Westerhoff Columbia University NYSPT Summer Institute 2002

Physics and the Quantum Mechanical Model

II. Spectrophotometry (Chapters 17, 19, 20)

5.111 Lecture Summary #3 Monday, September 8, 2014

c = λν 10/23/13 What gives gas-filled lights their colors? Chapter 5 Electrons In Atoms

LC-4: Photoelectric Effect

Laboratory Exercise. Atomic Spectra A Kirchoff Potpourri

Lecture 0. NC State University

Light and Atmosphere 1

Experiment 7: Adsorption Spectroscopy I, Determination of Iron with 1,10 Phenanthroline

Light and Matter: Reading Messages from the Cosmos Pearson Education, Inc.

Teaching philosophy. learn it, know it! Learn it 5-times and you know it Read (& simple question) Lecture Problem set

Properties of Light and Atomic Structure. Chapter 7. So Where are the Electrons? Electronic Structure of Atoms. The Wave Nature of Light!

AQA Physics A-level Section 12: Turning Points in Physics

Molecular Luminescence. Absorption Instrumentation. UV absorption spectrum. lg ε. A = εbc. monochromator. light source. Rotating mirror (beam chopper)

Transcription:

ELECTROMAGNETIC SPECTRUM Wavenumber (cm -1 ) Frequency (Hz) Wavelength (m) LEARNING CHECK What experiment proved light behaves as a wave? What experiment proved light behaves as a par6cle? List 5 examples of phenomena in which light interacts with ma;er as a wave. 1

YOUNG EXPERIMENT (1800)- PROVED LIGHT IS A WAVE PHOTOELECTRIC EFFECT- LIGHT IS A PARTICLE 1. Light incident on the photocathode 2. Electrons liberated 3. Voltage at anode adjusted to stop current 4. Stopping voltage depends on cathode substrate and radiazon energy 2

LEARNING CHECK Suppose that the screen in the figure below is 3.51 m from the plan containing the slits and that the slits are 0.200 mm apart. What is the wavelength of the third band from the center, located at 13 mm from the central band? 3

LEARNING CHECK List 5 examples of phenomena in which light interacts with ma;er as a wave. LEARNING CHECK 4

INTERACTIONS BETWEEN LIGHT AND MATTER LIGHT AS A WAVE DiffracZon RefracZon Transmission ReflecZon Sca`ering PolarizaZon LIGHT AS A PARTICLE Photoelectric effect AbsorpZon Emission Sca`ering 5

ABSORPTION ABSORPTION Compare atomic and molecular absorpzon? Why does atomic absorpzon occur at discrete wavelengths while molecular absorpzon occur in broad peaks? 6

EMISSION 7

LUMINESCENCE JABLONSKI DIAGRAM 8

JABLONSKI DIAGRAM TRANSITIONS Electronic excita6on- promo6on of an electron to an excited state (electronic, vibra6onal, rota6onal). S 0 à S 1 Nonradia6ve decay (vibra6onal relaxa6on)- vibra6onal energy transferred to other molecules through collisions. Very fast. Excited state à S 1 ground vibra6onal state Fluorescence- emission of photon to return to S 0. S 1 às 0 +hν Internal conversion- radia6onless transi6on to an extremely vibra6onally excited state of S 0 without a change in energy. S 1 às 0 Intersystem crossing- radia6onless transi6on from S 1 to T 1 with no change in energy. Change of electron spin. S 1 àt 1 Phosphorescence- emission of photon to return to S 0. T 1 às 0 +hν SCATTERING 9

TIMESCALES OF THE FOLLOWING TRANSITIONS. BASED ON THESE OBSERVATIONS, CAN YOU PREDICT WHICH TRANSITIONS MIGHT BE MORE LIKELY TO OCCUR (AND THUS MORE COMMON)? Phenomena Transmission NonradiaZve decay Electronic transizons fluorescence phosphorescence Time scale 10-14 - 10-15 s 10-15 s 10-8 s 10-5 s 10-5 to 100 s s BEER S LAW CHEM 314 SKOOG N HOLLER CH 13 10

OBJECTIVES State and apply Beer s law Apply Beer s law to a variety of useful situazons IdenZfy condizons under which Beer s law is not linear Troubleshoot absorpzon experiments and suggest ways to regain linearity in Beer s law. Derive Beer s Law equazon A SIMPLE ABSORPTION EXPERIMENT Beer s Law T= transmission P 0 = incident power P= transmi`ed power A= absorbance ε= molar absorpzvity b= path length C= analyte concentrazon ConcentraZon relazve to mixing direczons 2.85 2.0 1.0 0.5 0.25 0.1 0.01 0.001 11

WHY DOES KOOL-AID APPEAR RED? What color does the Kool-aid absorb? Absorbance (arb.) 2.0 1.5 1.0 0.5 0.0 Red #40 495.2 nm 300 400 500 600 700 800 wavelength (nm) Energy E 2 e - e - 3 2 1 0 3 2 1 E 0 1 Jablonski Diagram h`p://img.photobucket.com/albums/v645/fadeout95/roygbiv.gif h`p://roygbivcolors7.files.wordpress.com/2013/01/complementry-color-wheel-copy2.jpg 12

BEER S LAW: RELATING ANALYTE CONCENTRATION AND ABSORBANCE Absorbance (arb) 1.0 0.8 0.6 0.4 0.2 A=1.9 [Kool-aid] r 2 =0.97 ε molar absorbzvity 0.0 0.0 0.1 0.2 0.3 0.4 0.5 [Kool-aid] y=mx + b A=ε b [Kool-aid] b= path length APPLICATION OF BEER S LAW TO MIXTURES Spectra of mixtures can be assumed to generate a linear combinazon of the individual component spectra 13

ML 2 M ML SOURCES OF NONLINEARITY OF BEER S LAW 1. SoluZon factors 2. Non-monochromaZc light 3. Not analyzing at l max 4. Stray light 5. Mismatched cuve`es 6. Instrument noise Too much or too li`le absorpzon Absorbance (arb) 3.0 2.5 2.0 1.5 1.0 0.5 0.0 0.0 0.5 1.0 1.5 2.0 2.5 3.0 [Kool-aid] 14

1. SOLUTION FACTORS High analyte concentrazons (>0.01M) Red Cl High electrolyte concentrazons - 40 Na Red + Cl Red - Na 40 + RefracZve index of medium Na + 40 Cl- Cl - Na+ Cl - Na + Cl- Red Na + Na + Cl- Cl - Na + Cl- Na 40 Red + Cl- Na Red ReacZons within the soluzon + 40 Na Cl- + 40 HIn ó H + + In - Na + Na + Cl- Red Na + Cl - Cl - Na 40 + Cl- Incident Light P 0 Emergent Light P 1. SOLUTION FACTORS ReacZons within the soluzon HIn ó H + + In - AbsorpZon primarily by In - Absorbance (arb.) 2.0 1.5 1.0 0.5 0.0 300 400 500 600 700 800 wavelength (nm) AbsorpZon primarily by HIn 15

2. NON MONOCHROMATIC SOURCE Absorbance (arb.) 2.0 1.5 1.0 0.5 0.0 ε ε 300 400 500 600 700 800 wavelength (nm) λ and λ are different wavelengths 3. NOT MEASURING AT LAMDA MAX 16

EFFECT OF SLIT WIDTHS Mono slit width determines spread of λ incident on sample (bandwidth) Image incident on mono exit plane Wide slits allow More light (higher throughput) More λ (larger bandwidth) No such thing as a free lunch EFFECT OF SLIT WIDTHS What slit width should you choose? 17

EFFECT OF SLIT WIDTHS 4. STRAY LIGHT 18

4. STRAY LIGHT 5. MISMATCHED CUVETTES Differences in: Path length OpZcal characteriszcs Most likely to affect calibrazon curve intercept SoluZon: Double beam: Use matched cuve`es Single beam; Use the same cuve`e 19

LEARNING CHECK List and describe 4 types of instrumental error A SIMPLE ABSORPTION EXPERIMENT Components of an absorp6on experiment: 1. 0% T measurement (adjustment) 2. 100% T measurement 3. Sample T measurement Uncertainty associated with measurement is the aggregate of uncertainty in each step Uncertainty associated with error measurement depends on T 20

6. INSTRUMENTAL NOISE IN TRANSMISSION MEASUREMENTS 21

6. INSTRUMENTAL NOISE IN TRANSMISSION MEASUREMENTS 22

LINEAR RANGE OF BEER S LAW Absorbance (arb) 3.0 2.5 2.0 1.5 1.0 0.5 0.0 0.0 0.5 1.0 1.5 2.0 2.5 3.0 [Kool-aid] 23

DERIVATION OF BEER S LAW T= transmission P 0 = incident power P= transmi`ed power A= absorbance ε= molar absorpzvity b= path length C= analyte concentrazon LOOKING AHEAD Thursday (Jan 28)- Beer s Law (Ch 13, look through deriva6on on website) Project Overview (Due Feb 15) First day of Consumer Characteriza6on Project Experiment 1: Metals Analysis Due: Prelab 1, Experiment 1 Goals for lab today: disassemble your project, use handheld XRF Monday (Feb 1)- Instrument components (Ch 7) Standard Addi6on Due Tuesday (Feb 2)- Experiment 1 Metals Thursday (Feb 4)- Experiment 1 Metals Prelab 2, Experiment 1 Due 24