This page must be the first page of your solutions!

Size: px
Start display at page:

Download "This page must be the first page of your solutions!"

Transcription

1 ENERGY TRANSFER Submission deadline of December Total number of points = = 119 Name: FRET Max Real 5,1 A 3 B 3 C 3 5,2 A 3 B 3 C 4 5,3 A 15 B 5 C 8 D 6 5,4 A 3 B 5 C 5 5,5 30 5,6 A 5 B 10 C 5 D 3 SUM (MAX) % 119 This page must be the first page of your solutions! 1

2 PCR 3.1 (9) You have one A molecule and three variants of D molecule (D1, D2, D3). For all possible pairs the spectral overlapping is the same, the distance between D and A is the same in all pairs. The donors have the following characteristics: D1: fluorescence lifetime 1 = 2 ns, fluorescence quantum yield 1 = 0.25 D2: fluorescence lifetime 2 = 0.4 ns, fluorescence quantum yield 2 = 0.1 D3: fluorescence lifetime 3 = 3 ns, fluorescence quantum yield 1 = 0.5 a) (3) List the pairs in the order of increasing of the energy transfer rate (k FRET ) Write the dependence k FRET on and b) (3) List the pairs in the order of increasing of the Förster radius (R 0 ) Write the dependence R 0 on and c) (3) List the pairs in the order of increasing of the efficiency of FRET ( ) Write the dependence of on and PCR 3.2. (10) Energy transfer rate, k ET a) (3) Does k ET depend on radiative lifetime ( 0 ) of the donor? If so, write the equation. b) (3) Does k ET depend on radiative lifetime of the acceptor? If so, write the equation. c) (4) How does k ET depend on transition dipole moments of the donor ( D ) and the acceptor ( A )? 2

3 PCR 3.3. (34) Spectral overlap Absorption and fluorescence spectra of a donor (D) and an acceptor (A) molecule are given at the Figure. The fluorescence spectra are normalized: F d 1 wholespectrum Fluorescence quantum yield D in the absence of A is 0.5. Fluorescence quantum yield of A is 1. The solvent is water (n=1.33) a) (15) Calculate R 0 for energy transfer from D to A in solution (averaged over all orientations). In order to calculate the overlapping integral approximate the spectra in the spectral overlapping region by straight lines. b) (5) Do you expect to have any energy transfer from D to A if the distance between molecules is 10 nm? If so, estimate the transfer efficiency. c) (8) The concentration of D in a frozen solution is 10-4 mol/l. Estimate the concentration of A in the same solution in order to have 50% energy transferred from D to A? d) (6) You have a 50/50 mixture of D and A in the sample. With probability of 50% excited D transfers its energy to the acceptor. 1) Draw the shape of the absorption spectrum of the sample (use the graphs provided below). The relative amplitudes of the peaks should reflect the reality! 2) Draw the shape of the fluorescence spectrum if excitation = 650 nm 3) Draw the shape of the fluorescence spectrum if excitation = 500 nm In all the cases excitation intensity is the same. Your graphs should reflect the fluorescence intensities that you can compare cases 2 and 3. 3

4 4

5 PCR 3.4 (13) D A a) (3) Tell which of those DA pairs have zero energy transfer efficiency (consider orientations only). b) (5) Calculate 2 for all pairs c) (5) Calculate efficiency of energy transfer for the first pair if the distance between the molecules is 6 nm and R 0 for random orientations is 5 nm. PCR 3.5 (30) You have a nanostructure shown at the figure. The acceptor molecule is placed in the center of a 2-dimentional array of donor molecules. The donor molecules are excited by light. The fluorescence yield of the acceptor molecule is zero, so it works as a fluorescence quencher. The position of every acceptor molecule is given by r and (polar coordinates, see the picture). Neglect the discontinuity of the sample, in other words, assume that the size of the molecules and the distance between them are much smaller than 10 nm, which is R 0 for headto-tail oriented D and A Donors a) Obtain analytical expression for R 0 of energy transfer from A to D as a function of angle. b) Using this expression draw the area in the sample within which the donor molecules are quenched with probability more than 50%. D Acceptor A r R 0 ( ) =? 5

6 PCR 3.6. (23) Electron and Energy transfer Both energy transfer and electron transfer can lead to fluorescence quenching of a donor molecule in a DA pair if A is not fluorescent a) (5) Compare dependences of the quenching rates on distances between D and A for the two mechanisms b) (10) What are the typical values of D-A distances when electron transfer can compete with fluorescence decay of the donor? Fluorescence decay time of D without A is about 10 ns. Use the equation for the electron transfer rate with the following parameters: H AB = 0.5 ev T=300K =1 ev =30 nm -1 for the rest assume the most favorable condition in the Marcus theory of electron transfer. c) (5) What are typical values of D-A distances when Energy transfer can compete with fluorescence decay of the donor? Take typical values of the Förster radius for good DA pairs for your estimation. d) (3) For the DA pair with the intermolecular distance of 3 nm A quenches fluorescence of D very efficiently. Based on your answers in a) and b) tell the most probable mechanism of the quenching (electron or energy transfer?) 6

Molecular Spectroscopy

Molecular Spectroscopy Molecular Spectroscopy UV-Vis Spectroscopy Absorption Characteristics of Some Common Chromophores UV-Vis Spectroscopy Absorption Characteristics of Aromatic Compounds UV-Vis Spectroscopy Effect of extended

More information

Fundamentals of modern UV-visible spectroscopy. Presentation Materials

Fundamentals of modern UV-visible spectroscopy. Presentation Materials Fundamentals of modern UV-visible spectroscopy Presentation Materials The Electromagnetic Spectrum E = hν ν = c / λ 1 Electronic Transitions in Formaldehyde 2 Electronic Transitions and Spectra of Atoms

More information

Hydrogen Bonds The electrostatic nature of hydrogen bonds

Hydrogen Bonds The electrostatic nature of hydrogen bonds Hydrogen Bonds Hydrogen bonds have played an incredibly important role in the history of structural biology. Both the structure of DNA and of protein a-helices and b-sheets were predicted based largely

More information

Aspects of an introduction to photochemistry

Aspects of an introduction to photochemistry Aspects of an introduction to photochemistry Ground state reactants Excited state reactants Reaction Intermediates Ground state products Orbital occupancy Carbonyl photochemistry Vibrational structure

More information

The Rate Constant for Fluorescence Quenching 1

The Rate Constant for Fluorescence Quenching 1 The Rate Constant for Fluorescence Quenching 1 Purpose This experiment utilizes fluorescence intensity measurements to determine the rate constant for the fluorescence quenching of anthracene or perylene

More information

PCV Project: Excitons in Molecular Spectroscopy

PCV Project: Excitons in Molecular Spectroscopy PCV Project: Excitons in Molecular Spectroscopy Introduction The concept of excitons was first introduced by Frenkel (1) in 1931 as a general excitation delocalization mechanism to account for the ability

More information

Technical Note. Roche Applied Science. No. LC 18/2004. Assay Formats for Use in Real-Time PCR

Technical Note. Roche Applied Science. No. LC 18/2004. Assay Formats for Use in Real-Time PCR Roche Applied Science Technical Note No. LC 18/2004 Purpose of this Note Assay Formats for Use in Real-Time PCR The LightCycler Instrument uses several detection channels to monitor the amplification of

More information

Austin Peay State University Department of Chemistry Chem 1111. The Use of the Spectrophotometer and Beer's Law

Austin Peay State University Department of Chemistry Chem 1111. The Use of the Spectrophotometer and Beer's Law Purpose To become familiar with using a spectrophotometer and gain an understanding of Beer s law and it s relationship to solution concentration. Introduction Scientists use many methods to determine

More information

EXPERIMENT 11 UV/VIS Spectroscopy and Spectrophotometry: Spectrophotometric Analysis of Potassium Permanganate Solutions.

EXPERIMENT 11 UV/VIS Spectroscopy and Spectrophotometry: Spectrophotometric Analysis of Potassium Permanganate Solutions. EXPERIMENT 11 UV/VIS Spectroscopy and Spectrophotometry: Spectrophotometric Analysis of Potassium Permanganate Solutions. Outcomes After completing this experiment, the student should be able to: 1. Prepare

More information

Lecture 1: Basic Concepts on Absorption and Fluorescence

Lecture 1: Basic Concepts on Absorption and Fluorescence Lecture 1: Basic Concepts on Absorption and Fluorescence Nicholas G. James Cell and Molecular Biology University of Hawaii at Manoa, Honolulu The Goal The emission of light after absorption of an outside

More information

DNA Detection. Chapter 13

DNA Detection. Chapter 13 DNA Detection Chapter 13 Detecting DNA molecules Once you have your DNA separated by size Now you need to be able to visualize the DNA on the gel somehow Original techniques: Radioactive label, silver

More information

Technical Note. Roche Applied Science. No. LC 19/2004. Color Compensation

Technical Note. Roche Applied Science. No. LC 19/2004. Color Compensation Roche Applied Science Technical Note No. LC 19/2004 Purpose of this Note Color The LightCycler System is able to simultaneously detect and analyze more than one color in each capillary. Due to overlap

More information

13C NMR Spectroscopy

13C NMR Spectroscopy 13 C NMR Spectroscopy Introduction Nuclear magnetic resonance spectroscopy (NMR) is the most powerful tool available for structural determination. A nucleus with an odd number of protons, an odd number

More information

Copyright 1999 2010 by Mark Brandt, Ph.D. 12

Copyright 1999 2010 by Mark Brandt, Ph.D. 12 Introduction to Absorbance Spectroscopy A single beam spectrophotometer is comprised of a light source, a monochromator, a sample holder, and a detector. An ideal instrument has a light source that emits

More information

2 Absorbing Solar Energy

2 Absorbing Solar Energy 2 Absorbing Solar Energy 2.1 Air Mass and the Solar Spectrum Now that we have introduced the solar cell, it is time to introduce the source of the energy the sun. The sun has many properties that could

More information

Fluorescent dyes for use with the

Fluorescent dyes for use with the Detection of Multiple Reporter Dyes in Real-time, On-line PCR Analysis with the LightCycler System Gregor Sagner, Cornelia Goldstein, and Rob van Miltenburg Roche Molecular Biochemicals, Penzberg, Germany

More information

Broadband THz Generation from Photoconductive Antenna

Broadband THz Generation from Photoconductive Antenna Progress In Electromagnetics Research Symposium 2005, Hangzhou, China, August 22-26 331 Broadband THz Generation from Photoconductive Antenna Qing Chang 1, Dongxiao Yang 1,2, and Liang Wang 1 1 Zhejiang

More information

3. Electronic Spectroscopy of Molecules I - Absorption Spectroscopy

3. Electronic Spectroscopy of Molecules I - Absorption Spectroscopy 3. Electronic Spectroscopy of Molecules I - Absorption Spectroscopy 3.1. Vibrational coarse structure of electronic spectra. The Born Oppenheimer Approximation introduced in the last chapter can be extended

More information

FRET Basics and Applications an EAMNET teaching module

FRET Basics and Applications an EAMNET teaching module FRET Basics and Applications an EAMNET teaching module Timo Zimmermann + Stefan Terjung Advanced Light Microscopy Facility European Molecular Biology Laboratory, Heidelberg http://www.embl.de/almf/ http://www.embl.de/eamnet/

More information

AP CHEMISTRY 2009 SCORING GUIDELINES

AP CHEMISTRY 2009 SCORING GUIDELINES AP CHEMISTRY 2009 SCORING GUIDELINES Question 6 (8 points) Answer the following questions related to sulfur and one of its compounds. (a) Consider the two chemical species S and S 2. (i) Write the electron

More information

Molecular Engineering for Solar Energy Conversion and Lighting Materials

Molecular Engineering for Solar Energy Conversion and Lighting Materials 193 Figure 5.1 Schematic representation of photochemical water splitting (artificial photosynthesis). Five fundamental components are needed: (1) an antenna for light harvesting, (2) a charge-separation

More information

Problem Set 6 UV-Vis Absorption Spectroscopy. 13-1. Express the following absorbances in terms of percent transmittance:

Problem Set 6 UV-Vis Absorption Spectroscopy. 13-1. Express the following absorbances in terms of percent transmittance: Problem Set 6 UV-Vis Absorption Spectroscopy 13-1. Express the following absorbances in terms of percent transmittance: a 0.051 b 0.918 c 0.379 d 0.261 e 0.485 f 0.072 A = log P o /P = log1/t = - log T

More information

Experiment 5. Lasers and laser mode structure

Experiment 5. Lasers and laser mode structure Northeastern University, PHYS5318 Spring 2014, 1 1. Introduction Experiment 5. Lasers and laser mode structure The laser is a very important optical tool that has found widespread use in science and industry,

More information

Blackbody radiation derivation of Planck s radiation low

Blackbody radiation derivation of Planck s radiation low Blackbody radiation derivation of Planck s radiation low 1 Classical theories of Lorentz and Debye: Lorentz (oscillator model): Electrons and ions of matter were treated as a simple harmonic oscillators

More information

NanoChop NP-Functionalization and Determination of the Optical Properties of the Fluorescent NPs U. Resch-Genger

NanoChop NP-Functionalization and Determination of the Optical Properties of the Fluorescent NPs U. Resch-Genger anochop PFunctionalization and Determination of the Optical Properties of the Fluorescent Ps U. ReschGenger Preparation and Characterization of Fluorescent Particles I. Preparation of fluorescent nanoparticles

More information

ATOMIC SPECTRA. Apparatus: Optical spectrometer, spectral tubes, power supply, incandescent lamp, bottles of dyed water, elevating jack or block.

ATOMIC SPECTRA. Apparatus: Optical spectrometer, spectral tubes, power supply, incandescent lamp, bottles of dyed water, elevating jack or block. 1 ATOMIC SPECTRA Objective: To measure the wavelengths of visible light emitted by atomic hydrogen and verify the measured wavelengths against those predicted by quantum theory. To identify an unknown

More information

INFRARED SPECTROSCOPY (IR)

INFRARED SPECTROSCOPY (IR) INFRARED SPECTROSCOPY (IR) Theory and Interpretation of IR spectra ASSIGNED READINGS Introduction to technique 25 (p. 833-834 in lab textbook) Uses of the Infrared Spectrum (p. 847-853) Look over pages

More information

2, 8, 20, 28, 50, 82, 126.

2, 8, 20, 28, 50, 82, 126. Chapter 5 Nuclear Shell Model 5.1 Magic Numbers The binding energies predicted by the Liquid Drop Model underestimate the actual binding energies of magic nuclei for which either the number of neutrons

More information

Ultraviolet Spectroscopy

Ultraviolet Spectroscopy Ultraviolet Spectroscopy The wavelength of UV and visible light are substantially shorter than the wavelength of infrared radiation. The UV spectrum ranges from 100 to 400 nm. A UV-Vis spectrophotometer

More information

University of Cyprus Biomedical Imaging and Applied Optics Laboratory Light-Tissue Interaction

University of Cyprus Biomedical Imaging and Applied Optics Laboratory Light-Tissue Interaction University of Cyprus Biomedical Imaging and Applied Optics Laboratory Light-Tissue Interaction Costas Pitris, MD, PhD KIOS Research Center Department of Electrical and Computer Engineering University of

More information

The Physics of Energy sources Renewable sources of energy. Solar Energy

The Physics of Energy sources Renewable sources of energy. Solar Energy The Physics of Energy sources Renewable sources of energy Solar Energy B. Maffei Bruno.maffei@manchester.ac.uk Renewable sources 1 Solar power! There are basically two ways of using directly the radiative

More information

Structure Factors 59-553 78

Structure Factors 59-553 78 78 Structure Factors Until now, we have only typically considered reflections arising from planes in a hypothetical lattice containing one atom in the asymmetric unit. In practice we will generally deal

More information

1 The water molecule and hydrogen bonds in water

1 The water molecule and hydrogen bonds in water The Physics and Chemistry of Water 1 The water molecule and hydrogen bonds in water Stoichiometric composition H 2 O the average lifetime of a molecule is 1 ms due to proton exchange (catalysed by acids

More information

Chapter 10 Molecular Geometry and Chemical Bonding Theory

Chapter 10 Molecular Geometry and Chemical Bonding Theory Chem 1: Chapter 10 Page 1 Chapter 10 Molecular Geometry and Chemical Bonding Theory I) VSEPR Model Valence-Shell Electron-Pair Repulsion Model A) Model predicts Predicts electron arrangement and molecular

More information

Understanding Poles and Zeros

Understanding Poles and Zeros MASSACHUSETTS INSTITUTE OF TECHNOLOGY DEPARTMENT OF MECHANICAL ENGINEERING 2.14 Analysis and Design of Feedback Control Systems Understanding Poles and Zeros 1 System Poles and Zeros The transfer function

More information

Chapter 2. Atomic Structure and Interatomic Bonding

Chapter 2. Atomic Structure and Interatomic Bonding Chapter 2. Atomic Structure and Interatomic Bonding Interatomic Bonding Bonding forces and energies Primary interatomic bonds Secondary bonding Molecules Bonding Forces and Energies Considering the interaction

More information

Measuring Protein Concentration through Absorption Spectrophotometry

Measuring Protein Concentration through Absorption Spectrophotometry Measuring Protein Concentration through Absorption Spectrophotometry In this lab exercise you will learn how to homogenize a tissue to extract the protein, and then how to use a protein assay reagent to

More information

NMR - Basic principles

NMR - Basic principles NMR - Basic principles Subatomic particles like electrons, protons and neutrons are associated with spin - a fundamental property like charge or mass. In the case of nuclei with even number of protons

More information

Section Activity #1: Fill out the following table for biology s most common elements assuming that each atom is neutrally charged.

Section Activity #1: Fill out the following table for biology s most common elements assuming that each atom is neutrally charged. LS1a Fall 2014 Section Week #1 I. Valence Electrons and Bonding The number of valence (outer shell) electrons in an atom determines how many bonds it can form. Knowing the number of valence electrons present

More information

Copyright 2007 Casa Software Ltd. www.casaxps.com. ToF Mass Calibration

Copyright 2007 Casa Software Ltd. www.casaxps.com. ToF Mass Calibration ToF Mass Calibration Essentially, the relationship between the mass m of an ion and the time taken for the ion of a given charge to travel a fixed distance is quadratic in the flight time t. For an ideal

More information

Exciton Diffusion. Exciton Diffusion

Exciton Diffusion. Exciton Diffusion Exciton Diffusion Exciton Energy transfer Exciton Diffusion. Photoluminescence measurement. Photocurrent measurement Handout on Photocurrent Response: Bulovic and Forrest., Chemical Physics 210, 13 (1996).

More information

Nuclear Magnetic Resonance

Nuclear Magnetic Resonance Nuclear Magnetic Resonance NMR is probably the most useful and powerful technique for identifying and characterizing organic compounds. Felix Bloch and Edward Mills Purcell were awarded the 1952 Nobel

More information

ENERGY PER PHOTOELECTRON IN A COINCIDENCE LIQUID SCINTILLATION COUNTER AS A FUNCTION OF ELECTRON ENERGY. Donald L. Horrocks

ENERGY PER PHOTOELECTRON IN A COINCIDENCE LIQUID SCINTILLATION COUNTER AS A FUNCTION OF ELECTRON ENERGY. Donald L. Horrocks ENERGY PER PHOTOELECTRON IN A COINCIDENCE LIQUID SCINTILLATION COUNTER AS A FUNCTION OF ELECTRON ENERGY Donald L. Horrocks Nuclear Systems Operations Beckman Instruments, Inc. SmithKlirie Beckman Irvine,

More information

Symmetric Stretch: allows molecule to move through space

Symmetric Stretch: allows molecule to move through space BACKGROUND INFORMATION Infrared Spectroscopy Before introducing the subject of IR spectroscopy, we must first review some aspects of the electromagnetic spectrum. The electromagnetic spectrum is composed

More information

Energy band diagrams. Single atom. Crystal. Excited electrons cannot move. Excited electrons can move (free electrons)

Energy band diagrams. Single atom. Crystal. Excited electrons cannot move. Excited electrons can move (free electrons) Energy band diagrams In the atoms, the larger the radius, the higher the electron potential energy Hence, electron position can be described either by radius or by its potential energy In the semiconductor

More information

The accurate calibration of all detectors is crucial for the subsequent data

The accurate calibration of all detectors is crucial for the subsequent data Chapter 4 Calibration The accurate calibration of all detectors is crucial for the subsequent data analysis. The stability of the gain and offset for energy and time calibration of all detectors involved

More information

Reaction Stoichiometry and the Formation of a Metal Ion Complex

Reaction Stoichiometry and the Formation of a Metal Ion Complex Reaction Stoichiometry and the Formation of a Metal Ion Complex Objectives The objectives of this laboratory are as follows: To use the method of continuous variation to determine the reaction stoichiometry

More information

Chapter 30 - Magnetic Fields and Torque. A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University

Chapter 30 - Magnetic Fields and Torque. A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University Chapter 30 - Magnetic Fields and Torque A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University 2007 Objectives: After completing this module, you should

More information

Group Theory and Chemistry

Group Theory and Chemistry Group Theory and Chemistry Outline: Raman and infra-red spectroscopy Symmetry operations Point Groups and Schoenflies symbols Function space and matrix representation Reducible and irreducible representation

More information

Activitity (of a radioisotope): The number of nuclei in a sample undergoing radioactive decay in each second. It is commonly expressed in curies

Activitity (of a radioisotope): The number of nuclei in a sample undergoing radioactive decay in each second. It is commonly expressed in curies Activitity (of a radioisotope): The number of nuclei in a sample undergoing radioactive decay in each second. It is commonly expressed in curies (Ci), where 1 Ci = 3.7x10 10 disintegrations per second.

More information

Physics Notes Class 11 CHAPTER 3 MOTION IN A STRAIGHT LINE

Physics Notes Class 11 CHAPTER 3 MOTION IN A STRAIGHT LINE 1 P a g e Motion Physics Notes Class 11 CHAPTER 3 MOTION IN A STRAIGHT LINE If an object changes its position with respect to its surroundings with time, then it is called in motion. Rest If an object

More information

Chapter 19. General Matrices. An n m matrix is an array. a 11 a 12 a 1m a 21 a 22 a 2m A = a n1 a n2 a nm. The matrix A has n row vectors

Chapter 19. General Matrices. An n m matrix is an array. a 11 a 12 a 1m a 21 a 22 a 2m A = a n1 a n2 a nm. The matrix A has n row vectors Chapter 9. General Matrices An n m matrix is an array a a a m a a a m... = [a ij]. a n a n a nm The matrix A has n row vectors and m column vectors row i (A) = [a i, a i,..., a im ] R m a j a j a nj col

More information

Performance. 13. Climbing Flight

Performance. 13. Climbing Flight Performance 13. Climbing Flight In order to increase altitude, we must add energy to the aircraft. We can do this by increasing the thrust or power available. If we do that, one of three things can happen:

More information

Determination of source parameters from seismic spectra

Determination of source parameters from seismic spectra Topic Determination of source parameters from seismic spectra Authors Michael Baumbach, and Peter Bormann (formerly GeoForschungsZentrum Potsdam, Telegrafenberg, D-14473 Potsdam, Germany); E-mail: pb65@gmx.net

More information

where h = 6.62 10-34 J s

where h = 6.62 10-34 J s Electromagnetic Spectrum: Refer to Figure 12.1 Molecular Spectroscopy: Absorption of electromagnetic radiation: The absorptions and emissions of electromagnetic radiation are related molecular-level phenomena

More information

: : Solutions to Additional Bonding Problems

: : Solutions to Additional Bonding Problems Solutions to Additional Bonding Problems 1 1. For the following examples, the valence electron count is placed in parentheses after the empirical formula and only the resonance structures that satisfy

More information

ELECTRON SPIN RESONANCE Last Revised: July 2007

ELECTRON SPIN RESONANCE Last Revised: July 2007 QUESTION TO BE INVESTIGATED ELECTRON SPIN RESONANCE Last Revised: July 2007 How can we measure the Landé g factor for the free electron in DPPH as predicted by quantum mechanics? INTRODUCTION Electron

More information

O6: The Diffraction Grating Spectrometer

O6: The Diffraction Grating Spectrometer 2B30: PRACTICAL ASTROPHYSICS FORMAL REPORT: O6: The Diffraction Grating Spectrometer Adam Hill Lab partner: G. Evans Tutor: Dr. Peter Storey 1 Abstract The calibration of a diffraction grating spectrometer

More information

Time out states and transitions

Time out states and transitions Time out states and transitions Spectroscopy transitions between energy states of a molecule excited by absorption or emission of a photon hn = DE = E i - E f Energy levels due to interactions between

More information

Supporting Information

Supporting Information Supporting Information [C 70 ] Fullerene-Sensitized Triplet-Triplet Annihilation Upconversion Kyle Moor a, Jae-Hyuk Kim a, Samuel Snow b, and Jae-Hong Kim a,b a Department of Chemical and Environmental

More information

Wave Function, ψ. Chapter 28 Atomic Physics. The Heisenberg Uncertainty Principle. Line Spectrum

Wave Function, ψ. Chapter 28 Atomic Physics. The Heisenberg Uncertainty Principle. Line Spectrum Wave Function, ψ Chapter 28 Atomic Physics The Hydrogen Atom The Bohr Model Electron Waves in the Atom The value of Ψ 2 for a particular object at a certain place and time is proportional to the probability

More information

AP Chemistry A. Allan Chapter 8 Notes - Bonding: General Concepts

AP Chemistry A. Allan Chapter 8 Notes - Bonding: General Concepts AP Chemistry A. Allan Chapter 8 Notes - Bonding: General Concepts 8.1 Types of Chemical Bonds A. Ionic Bonding 1. Electrons are transferred 2. Metals react with nonmetals 3. Ions paired have lower energy

More information

The strength of the interaction

The strength of the interaction The strength of the interaction Host Guest Supramolecule (host-guest complex) When is the host capable to recognize the guest? How do we define selectivity Which element will we use to design the host

More information

Recording the Instrument Response Function of a Multiphoton FLIM System

Recording the Instrument Response Function of a Multiphoton FLIM System Recording the Instrument Response Function of a Multiphoton FLIM System Abstract. FLIM data analysis in presence of SHG signals or extremely fast decay components requires the correct instrument response

More information

From lowest energy to highest energy, which of the following correctly orders the different categories of electromagnetic radiation?

From lowest energy to highest energy, which of the following correctly orders the different categories of electromagnetic radiation? From lowest energy to highest energy, which of the following correctly orders the different categories of electromagnetic radiation? From lowest energy to highest energy, which of the following correctly

More information

Application Note AN4

Application Note AN4 TAKING INVENTIVE STEPS IN INFRARED. MINIATURE INFRARED GAS SENSORS GOLD SERIES UK Patent App. No. 2372099A USA Patent App. No. 09/783,711 World Patents Pending INFRARED SPECTROSCOPY Application Note AN4

More information

Lecture 3: Optical Properties of Bulk and Nano. 5 nm

Lecture 3: Optical Properties of Bulk and Nano. 5 nm Lecture 3: Optical Properties of Bulk and Nano 5 nm The Previous Lecture Origin frequency dependence of χ in real materials Lorentz model (harmonic oscillator model) 0 e - n( ) n' n '' n ' = 1 + Nucleus

More information

Integrating the Solar Spectrum

Integrating the Solar Spectrum Integrating the Solar Spectrum PHYS 4400, Principles and Varieties of Solar Energy Instructor: Randy J. Ellingson The University of Toledo January 24, 203 Pop Quiz Note: quiz does not count toward grade

More information

Excited state interaction in P-OLEDS implications for efficiency and lifetime

Excited state interaction in P-OLEDS implications for efficiency and lifetime Excited state interaction in P-OLEDS implications for efficiency and lifetime M. Roberts, S.M. King, M.Cass, M. Pintani, C.Coward N. Akino, H. Nakajima, M. Anryu SID 2011 Session 56: OLED Device I (Paper

More information

Mechanics lecture 7 Moment of a force, torque, equilibrium of a body

Mechanics lecture 7 Moment of a force, torque, equilibrium of a body G.1 EE1.el3 (EEE1023): Electronics III Mechanics lecture 7 Moment of a force, torque, equilibrium of a body Dr Philip Jackson http://www.ee.surrey.ac.uk/teaching/courses/ee1.el3/ G.2 Moments, torque and

More information

Organic Chemistry Tenth Edition

Organic Chemistry Tenth Edition Organic Chemistry Tenth Edition T. W. Graham Solomons Craig B. Fryhle Welcome to CHM 22 Organic Chemisty II Chapters 2 (IR), 9, 3-20. Chapter 2 and Chapter 9 Spectroscopy (interaction of molecule with

More information

How to compute Random acceleration, velocity, and displacement values from a breakpoint table.

How to compute Random acceleration, velocity, and displacement values from a breakpoint table. How to compute Random acceleration, velocity, and displacement values from a breakpoint table. A random spectrum is defined as a set of frequency and amplitude breakpoints, like these: 0.050 Acceleration

More information

Atomic Structure: Chapter Problems

Atomic Structure: Chapter Problems Atomic Structure: Chapter Problems Bohr Model Class Work 1. Describe the nuclear model of the atom. 2. Explain the problems with the nuclear model of the atom. 3. According to Niels Bohr, what does n stand

More information

Blackbody Radiation References INTRODUCTION

Blackbody Radiation References INTRODUCTION Blackbody Radiation References 1) R.A. Serway, R.J. Beichner: Physics for Scientists and Engineers with Modern Physics, 5 th Edition, Vol. 2, Ch.40, Saunders College Publishing (A Division of Harcourt

More information

Using light scattering method to find The surface tension of water

Using light scattering method to find The surface tension of water Experiment (8) Using light scattering method to find The surface tension of water The aim of work: The goals of this experiment are to confirm the relationship between angular frequency and wave vector

More information

dissociation: projectile charge and Furthermore we have observed that with increasing impact energy the kinetic energy of the fragments

dissociation: projectile charge and Furthermore we have observed that with increasing impact energy the kinetic energy of the fragments Kinetic energy release in molecular dissociation: projectile charge and collision energy dependence Dissociation products of CO have been measured in coincidence with each other for collisions with He

More information

2. Molecular stucture/basic

2. Molecular stucture/basic 2. Molecular stucture/basic spectroscopy The electromagnetic spectrum Spectral region for atomic and molecular spectroscopy E. Hecht (2nd Ed.) Optics, Addison-Wesley Publishing Company,1987 Spectral regions

More information

Section 5 Molecular Electronic Spectroscopy (lecture 9 ish)

Section 5 Molecular Electronic Spectroscopy (lecture 9 ish) Section 5 Molecular Electronic Spectroscopy (lecture 9 ish) Previously: Quantum theory of atoms / molecules Quantum Mechanics Vl Valence Molecular Electronic Spectroscopy Classification of electronic states

More information

PV (0.775 atm)(0.0854 L) n = = = 0.00264 mol RT -1-1

PV (0.775 atm)(0.0854 L) n = = = 0.00264 mol RT -1-1 catalyst 2 5 g ¾¾¾¾ 2 4 g 2 g DH298 = rxn DS298 C H OH( ) C H ( ) + H O( ) 45.5 kj/mol ; = 126 J/(K mol ) ethanol ethene water rxn 1 atm 760 torr PV (0.775 atm)(0.0854 L) n = = = 0.00264 mol RT -1-1 (0.08206

More information

Raman Spectroscopy Basics

Raman Spectroscopy Basics Raman Spectroscopy Basics Introduction Raman spectroscopy is a spectroscopic technique based on inelastic scattering of monochromatic light, usually from a laser source. Inelastic scattering means that

More information

Simulation of Fluorescence Spectroscopy Experiments

Simulation of Fluorescence Spectroscopy Experiments Simulation of Fluorescence Spectroscopy Experiments Dissertation Zur Erlangung des Doktorgrades der Mathematisch-Naturwissenschaftlichen Fakultäten der Georg-August-Universität zu Göttingen Vorgelegt von

More information

QUANTITATIVE INFRARED SPECTROSCOPY. Willard et. al. Instrumental Methods of Analysis, 7th edition, Wadsworth Publishing Co., Belmont, CA 1988, Ch 11.

QUANTITATIVE INFRARED SPECTROSCOPY. Willard et. al. Instrumental Methods of Analysis, 7th edition, Wadsworth Publishing Co., Belmont, CA 1988, Ch 11. QUANTITATIVE INFRARED SPECTROSCOPY Objective: The objectives of this experiment are: (1) to learn proper sample handling procedures for acquiring infrared spectra. (2) to determine the percentage composition

More information

CHAPTER 13 MOLECULAR SPECTROSCOPY

CHAPTER 13 MOLECULAR SPECTROSCOPY CHAPTER 13 MOLECULAR SPECTROSCOPY Our most detailed knowledge of atomic and molecular structure has been obtained from spectroscopy study of the emission, absorption and scattering of electromagnetic radiation

More information

Electron Orbits. Binding Energy. centrifugal force: electrostatic force: stability criterion: kinetic energy of the electron on its orbit:

Electron Orbits. Binding Energy. centrifugal force: electrostatic force: stability criterion: kinetic energy of the electron on its orbit: Electron Orbits In an atom model in which negatively charged electrons move around a small positively charged nucleus stable orbits are possible. Consider the simple example of an atom with a nucleus of

More information

MiSeq: Imaging and Base Calling

MiSeq: Imaging and Base Calling MiSeq: Imaging and Page Welcome Navigation Presenter Introduction MiSeq Sequencing Workflow Narration Welcome to MiSeq: Imaging and. This course takes 35 minutes to complete. Click Next to continue. Please

More information

Molecular Spectroscopy:

Molecular Spectroscopy: : How are some molecular parameters determined? Bond lengths Bond energies What are the practical applications of spectroscopic knowledge? Can molecules (or components thereof) be identified based on differences

More information

Selecting Receiving Antennas for Radio Tracking

Selecting Receiving Antennas for Radio Tracking Selecting Receiving Antennas for Radio Tracking Larry B Kuechle, Advanced Telemetry Systems, Inc. Isanti, Minnesota 55040 lkuechle@atstrack.com The receiving antenna is an integral part of any radio location

More information

Hydrogen Bonds in Water-Methanol Mixture

Hydrogen Bonds in Water-Methanol Mixture Bulg. J. Phys. 34 (2007) 103 107 Hydrogen Bonds in Water-Methanol Mixture G.M. Georgiev, K. Vasilev, K. Gyamchev Faculty of Physics, University of Sofia 5J.Bourchier Blvd., 1164 Sofia, Bulgaria Received

More information

Determining the Structure of an Organic Compound

Determining the Structure of an Organic Compound Determining the Structure of an Organic Compound The analysis of the outcome of a reaction requires that we know the full structure of the products as well as the reactants In the 19 th and early 20 th

More information

Uniformly Accelerated Motion

Uniformly Accelerated Motion Uniformly Accelerated Motion Under special circumstances, we can use a series of three equations to describe or predict movement V f = V i + at d = V i t + 1/2at 2 V f2 = V i2 + 2ad Most often, these equations

More information

AP* Atomic Structure & Periodicity Free Response Questions KEY page 1

AP* Atomic Structure & Periodicity Free Response Questions KEY page 1 AP* Atomic Structure & Periodicity ree Response Questions KEY page 1 1980 a) points 1s s p 6 3s 3p 6 4s 3d 10 4p 3 b) points for the two electrons in the 4s: 4, 0, 0, +1/ and 4, 0, 0, - 1/ for the three

More information

for excitation to occur, there must be an exact match between the frequency of the applied radiation and the frequency of the vibration

for excitation to occur, there must be an exact match between the frequency of the applied radiation and the frequency of the vibration ! = 1 2"c k (m + M) m M wavenumbers! =!/c = 1/" wavelength frequency! units: cm 1 for excitation to occur, there must be an exact match between the frequency of the applied radiation and the frequency

More information

Spectrochimica Acta Part A: Molecular and Biomolecular Spectroscopy

Spectrochimica Acta Part A: Molecular and Biomolecular Spectroscopy Spectrochimica Acta Part A: Molecular and Biomolecular Spectroscopy 104 (2013) 315 327 Contents lists available at SciVerse ScienceDirect Spectrochimica Acta Part A: Molecular and Biomolecular Spectroscopy

More information

Introduction to Geiger Counters

Introduction to Geiger Counters Introduction to Geiger Counters A Geiger counter (Geiger-Muller tube) is a device used for the detection and measurement of all types of radiation: alpha, beta and gamma radiation. Basically it consists

More information

A-LEVEL PHYSICS A. PHYA2 mechanics, materials and waves Mark scheme. 2450 June 2014. Version: 1.0 Final

A-LEVEL PHYSICS A. PHYA2 mechanics, materials and waves Mark scheme. 2450 June 2014. Version: 1.0 Final A-LEVEL PHYSICS A PHYA2 mechanics, materials and waves Mark scheme 2450 June 2014 Version: 1.0 Final Mark schemes are prepared by the Lead Assessment Writer and considered, together with the relevant questions,

More information

Improved predictive modeling of white LEDs with accurate luminescence simulation and practical inputs

Improved predictive modeling of white LEDs with accurate luminescence simulation and practical inputs Improved predictive modeling of white LEDs with accurate luminescence simulation and practical inputs TracePro Opto-Mechanical Design Software s Fluorescence Property Utility TracePro s Fluorescence Property

More information

The Hydrogen Atom Is a Magnet. http://www.seed.slb.com/en/scictr/watch/gashydrates/detecting.htm

The Hydrogen Atom Is a Magnet. http://www.seed.slb.com/en/scictr/watch/gashydrates/detecting.htm The Hydrogen Atom Is a Magnet Nuclear Magnetic Resonance Spectroscopy (NMR) Proton NMR A hydrogen nucleus can be viewed as a proton, which can be viewed as a spinning charge. As with any spinning charge,

More information

Use the Force! Noncovalent Molecular Forces

Use the Force! Noncovalent Molecular Forces Use the Force! Noncovalent Molecular Forces Not quite the type of Force we re talking about Before we talk about noncovalent molecular forces, let s talk very briefly about covalent bonds. The Illustrated

More information

NMR SPECTROSCOPY. Basic Principles, Concepts, and Applications in Chemistry. Harald Günther University of Siegen, Siegen, Germany.

NMR SPECTROSCOPY. Basic Principles, Concepts, and Applications in Chemistry. Harald Günther University of Siegen, Siegen, Germany. NMR SPECTROSCOPY Basic Principles, Concepts, and Applications in Chemistry Harald Günther University of Siegen, Siegen, Germany Second Edition Translated by Harald Günther JOHN WILEY & SONS Chichester

More information

Calculation of Source-detector Solid Angle, Using Monte Carlo Method, for Radioactive Sources with Various Geometries and Cylindrical Detector

Calculation of Source-detector Solid Angle, Using Monte Carlo Method, for Radioactive Sources with Various Geometries and Cylindrical Detector International Journal of Pure and Applied Physics ISSN 0973-1776 Volume 3, Number 2 (2007), pp. 201 208 Research India Publications http://www.ripublication.com/ijpap.htm Calculation of Source-detector

More information