Physics 248, Spring 2009 Lab 9: Franck-Hertz Experiment
|
|
- Kelly Joel Harrell
- 5 years ago
- Views:
Transcription
1 Name Section Physics 248, Spring 2009 Lab 9: Franck-Hertz Experiment Your TA will use this sheet to score your lab. It is to be turned in at the end of lab. To receive full credit you must use complete sentences and explain your reasoning clearly. The Franck-Hertz experiment, first performed in 1914, demonstrates the quantization of atomic energy levels. In the experiment, accelerated electrons collide with mercury (Hg) atoms. A measurement of the electron current as a function of the accelerating voltage reveals a series of rises and abrupt falls. The abrupt drops in current arise from inelastic collisions in which the Hg atoms make transitions to excited states, lending credence to the Bohr theory of the atom. For this discovery, Franck and Hertz were awarded the Nobel Prize in physics in Introduction. The Franck-Hertz experiment consists of a glass tube that surrounds three electrodes (a cathode that serves as the electron source, grid-form anode, and a plate which serves as the electron collector) and a drop of mercury. A thermostat-controlled oven allows the tube to be heated to temperatures of order 180 C, which vaporizes the mercury. The electrons produced at the cathode are accelerated through a potential difference V that is maintained between the cathode and the anode. The electrons then collide with the Hg atoms as they travel toward the anode. These collisions may be elastic, in which the electrons maintain (almost all of) their kinetic energy, or inelastic, in which the Hg atom is excited to a higher energy state. To distinguish between these two possibilities, a small retarding potential is maintained between the anode and the collector plate, such that electrons with sufficiently low kinetic energies cannot overcome this potential difference and therefore are not collected as current. Hence, by measuring the output current as a function of the accelerating voltage, it is possible to observe the energies at which inelastic collisions occur, and thus deduce the quantization of the Hg energy levels.
2 Procedure. Each lab station (there are only 4 in total) includes a Franck-Hertz oven/tube apparatus, a Franck-Hertz controller, a digital multimeter, and a Hg thermometer. To proceed, follow the instructions in the online lab manual as well as the instructions given below. IMPORTANT: the experimental setup is quite delicate and requires that you carefully follow the safety and equipment precautions described here and in the manual! 1. Follow the instructions regarding handling the glass thermometer. Note that these thermometers are extremely delicate, and if they break the Hg can spill, which is very dangerous. Handle the thermometers with EXTREME care. 2. The oven is controlled by a thermostat and must also be handled carefully. Follow an iterative procedure to raise the temperature to the desired value starting from 4 on the temperature controller on the oven, as described in the lab manual. Note that the temperature fluctuations can be quite extreme, so proceed very slowly and carefully, and in small increments. The desired range for the temperature controller should be somewhere between 6 and 7. Hold off on applying the accelerating voltage until the temperature is (reasonably) stabilized. 3. Be sure to monitor the temperature carefully. As stated in the manual, BE SURE NOT TO LET THE TEMPERATURE EXCEED 195 C, as this can damage the oven as well as the Hg thermometer. You must also take great care not to touch the oven once it is heated, as the outside gets extremely hot. 4. Follow the circuit diagram in the manual to connect the apparatus. The Franck- Hertz oven and controller are labeled to indicate which points should be connected. Note that the M denotes the mesh electrode, the Y is the output current, the A is the anode, and the X is the accelerating voltage. 5. You will use the Pasco interface to record your data. To do so, connect the Pasco box to the Franck-Hertz controller. Ignore the (outdated) Using the PASCO 750 Interface instructions in the lab manual and launch the Franck-Hertz lab icon using DataStudio. (Note: you may need to adjust the DataStudio settings to have your data be displayed properly.) 6. As described in the manual, the accelerating voltage at the recorder output is a fraction (about 5/70) of the actual accelerating potential. To calibrate it, connect the digital multimeter to the monitor leads, which measure the actual potential. 7. Once you have taken data, in lieu of the questions asked in the lab manual, you should follow the steps on the next pages of this sheet. 2
3 Results. Measure the output current as a function of the accelerating voltage. (Use the ramp function on the controller.) Be sure to calibrate the accelerating voltage, as described in #6 above. Obtain several sets of data. Place a representative plot (or plots) of your data in the space provided below. Compute the mean of the voltage difference between the peaks. Convert the voltage to electron volts, and compare your result with the energy of the transition of Hg from the 6s6p 3 P 1 state to the 6s6s 1 S 0 ground state, which is 4.86 ev. Include an error estimate. 3
4 Analysis and Discussion. (i) Summarize below why inelastic collisions of the electrons with the Hg atoms result in a drop in the collected current in this experiment. (ii) What is the physical interpretation of the series of drops in current as the accelerating voltage increases? (iii) What are the sources of error that you can identify in this experiment? Can you identify any further measurements you might make to account for these errors (and if so, please make those measurements and include your results)? 4
5 5
University of Massachusetts, Amherst
PHYSICS 286: Modern Physics Laboratory SPRING 2010 (A. Dinsmore and K. Kumar) Feb 2009 Experiment 4: THE FRANCK HERTZ EXPERIMENT Electronic Excitations of a Gas, and Evidence for the Quantization of Atomic
More informationEXPERIMENT 14. The Franck-Hertz Experiment. E 1 E 2 = hf (1)
EXPERIMENT 14 The Franck-Hertz Experiment The Franck-Hertz experiment is one of the best demonstrations to show the existence of discrete energy states in an atom as suggested by Niels Bohr. In this experiment,
More informationFranck-Hertz Experiment
Franck-Hertz Experiment Introduction: In 1914, James Franck and Gustav Hertz discovered in the course of their investigations an energy loss in distinct steps for electrons passing through mercury vapor,
More informationTHE FRANCK-HERTZ EXPERIMENT
Rice University Physics 332 THE FRANCK-HERTZ EXPERIMENT I. INTRODUCTION... 2 II. THEORETICAL CONSIDERATIONS... 3 III. MEASUREMENT AND ANALYSIS... 5 Revised July 1991 I. Introduction By the early part of
More informationEXPERIMENT 15. The Frank Hertz Experiment. 1. Pre-Laboratory Work [2 pts] Lab section: Partner's name(s): Grade:
Name: Date: Course number: MAKE SURE YOUR TA OR TI STAMPS EVERY PAGE BEFORE YOU START! Lab section: Partner's name(s): Grade: EXPERIMENT 15 The Frank Hertz Experiment 1. Pre-Laboratory Work [2 pts] 1.
More informationPhysics 201: Experiment #1 Franck-Hertz Experiment
Physics 201: Experiment #1 Franck-Hertz Experiment Carl Adams Winter 2004 Purpose To demonstrate that electrons colliding with gaseous mercury atoms lose energy in discrete amounts. Nobel Prize Winner
More informationFranck-Hertz Experiment
Instruction Manual and Experiment Guide for the PASCO scientific Model SE-9640 Franck-Hertz Tube Model SE-9641 Franck-Hertz Oven Model SE-9642 Franck-Hertz Control Unit 2/90 Franck-Hertz Experiment 0 C
More informationExperiment 6: Franck Hertz Experiment v1.3
Experiment 6: Franck Hertz Experiment v1.3 Background This series of experiments demonstrates the energy quantization of atoms. The concept was first implemented by James Franck and Gustaf Ludwig Hertz
More informationFRANCK-HERTZ EXPERIMENT ===========================
PHYS 4211 Last edit: May 3, 2011 T.E. Coan FRANCK-HERTZ EXPERIMENT =========================== GOAL You will repeat a portion of the 1914 Nobel-Prize winning experiment that demonstrates the quantization
More informationFranck-Hertz Experiment in Neon/Hg
Franck-Hertz Experiment in Neon/Hg Equipment Franck-Hertz tube (Ne or Hg) & Operating Unit Analog oscilloscope Many Banana cables; 1 BNC cables; 2 BNC-Banana Plug connector Graphing paper Theory This experiment
More informationThe Franck-Hertz Experiment Physics 2150 Experiment No. 9 University of Colorado
Experiment 9 1 Introduction The Franck-Hertz Experiment Physics 2150 Experiment No. 9 University of Colorado During the late nineteenth century, a great deal of evidence accumulated indicating that radiation
More informationLaboratory #12: Franck-Hertz Experiment: Electron Spectroscopy
INDIANA UNIVERSITY, DEPARTMENT OF PHYSICS, P309 LABORATORY Laboratory #12: Franck-Hertz Experiment: Electron Spectroscopy Goal: Verify Bohr's hypothesis that atomic excitation energies are quantized by
More informationThe Franck-Hertz Experiment
The Franck-Hertz Experiment David-Alexander Robinson; Jack Denning; 08332461 11th March 2010 Contents 1 Abstract 2 2 Introduction & Theory 2 2.1 The Franck-Hertz Experiment.................. 2 2.2 Energy
More informationEXPERIMENT #5 The Franck-Hertz Experiment: Electron Collisions with Mercury
EXPERIMENT #5 The Franck-Hertz Experiment: Electron Collisions with Mercury GOALS Physics Measure the energy difference between the ground state and the first excited state in mercury atoms, and conclude
More informationPhysics 476LW. Advanced Physics Laboratory - Franck Hertz
Physics 476LW Advanced Physics Laboratory Franck-Hertz Experiment Introduction In 1914 James Franck and Gustav Hertz performed an experiment that has become one of the classic demonstrations of the quantization
More informationThe Franck-Hertz Experiment David Ward The College of Charleston Phys 370/Experimental Physics Spring 1997
The Franck-Hertz Experiment David Ward The College of Charleston Phys 370/Experimental Physics Spring 1997 Abstract One of the most important experiments supporting quantum theory is the Franck- Hertz
More informationThe Franck-Hertz Experiment
The Franck-Hertz Experiment 1/30/06 The Franck-Hertz experiment, first undertaken shortly after Bohr s theory of the atom was presented, provided one of the early indications that atoms had discrete energy
More informationFranck-Hertz Experiment
Physikalisches Institut der Universität Bern Experimental Lab Sheet for Franck-Hertz Experiment (July 2013) Supervisor: Prof. Dr. Ingo Leya Assistants: Dr. Tamer Tolba Dr. Lucian Ancu Introduction: In
More informationFranck-Hertz experiment using Neon tube
Franck-Hertz experiment using Neon tube Objective: Study of quantized excitation of Neon atoms by inelastic scattering and determine the excitation energy. Introduction: Franck and Hertz described the
More informationEXPERIMENT 5. The Franck-Hertz Experiment (Critical Potentials) Introduction
EXPERIMENT 5 The Franck-Hertz Experiment (Critical Potentials) Introduction In the early part of the twentieth century the structure of the atom was studied in depth. In the process of developing and refining
More informationDetermining the excitation energies of mercury and neon using Franck-Hertz tubes
Determining the excitation energies of mercury and neon using Franck-Hertz tubes Sam Brind and Ali Abdollali 8926382 & 8949665 School of Physics and Astronomy The University of Manchester Second Year Laboratory
More informationThe Franck-Hertz Experiment
Physics 42 Spring 1995 Lab 1 - The Franck-Hertz Experiment and the Critical Potentials of Helium Theory At the turn of the century, spectroscopic work had clearly shown that atoms absorbed and emitted
More informationTHE FRANCK-HERTZ EXPERIMENT
THE FRANCK-HERTZ EXPERIMENT OBJECT: To measure the excitation potential of mercury using the Franck-Hertz method. EQUIPMENT LIST: Mercury vapor triode, oven and control unit (Neva-Klinger Scientific),
More informationTHE FRANCK-HERTZ EXPERIMENT
THE FRANCK-HERTZ EXPERIMENT OBJECT: To measure the excitation potential of mercury using the Franck-Hertz method. EQUIPMENT LIST: Mercury vapor triode, oven and control unit (Neva-Klinger Scientific),
More informationFinding e/m. Purpose. The purpose of this lab is to determine the charge to mass ratio of the electron. Equipment
Finding e/m Purpose The purpose of this lab is to determine the charge to mass ratio of the electron. Equipment Pasco Model SE-9638 E/M Apparatus Digital Multi-Meter, DMM Power Supply, Elenco Lead, Banana/Banana
More informationThermionic emission and Frank-Hertz oscillations
Thermionic emission and Frank-Hertz oscillations Matthew Krupcale, Evan Telford Department of Physics, Case Western Reserve University, Cleveland Ohio, 44106-7079 21 October 2012 Abstract Charges emitted
More informationMeasurement of Charge-to-Mass (e/m) Ratio for the Electron
Measurement of Charge-to-Mass (e/m) Ratio for the Electron Experiment objectives: measure the ratio of the electron charge-to-mass ratio e/m by studying the electron trajectories in a uniform magnetic
More informationLab 1: Determination of e/m for the electron
Lab 1: Determination of e/m for the electron Background Reading: Tipler, Llewellyn pp. 125 130; this covers the original method of Thomson which is somewhat different from that used in this experiment
More informationInvestigation #8 INTRODUCTION TO QUANTUM PHENONEMA
Name: Investigation #8 Partner(s): INTRODUCTION TO QUANTUM PHENONEMA Near the end of the 19 th century, many practitioners of what was then known as natural philosophy (now called physics ) believed that
More informationCharge to Mass Ratio of The Electron
Introduction Charge to Mass Ratio of The Electron The electron was first discovered by Sir J.J. Thomson in 1897 at the Cavendish Laboratory in Cambridge, England. His experimental apparatus is not very
More informationPhysics 248, Spring 2009 Lab 7: Capacitors and RC-Decay
Name Section Physics 248, Spring 2009 Lab 7: Capacitors and RC-Decay Your TA will use this sheet to score your lab. It is to be turned in at the end of lab. To receive full credit you must use complete
More informationFigure 1: Capacitor circuit
Capacitors INTRODUCTION The basic function of a capacitor 1 is to store charge and thereby electrical energy. This energy can be retrieved at a later time for a variety of uses. Often, multiple capacitors
More informationElectric Deflection of Electrons
Electric Deflection of Electrons Objective The purpose of this experiment is to observe that the spacial deflection of an electron in a cathode ray tube is directly proportional to the deflection potential.
More informationLab 5 - ELECTRON CHARGE-TO-MASS RATIO
81 Name Date Partners Lab 5 - ELECTRON CHARGE-TO-MASS RATIO OBJECTIVES To understand how electric and magnetic fields impact an electron beam To experimentally determine the electron charge-to-mass ratio
More informationE/M. Hunter Layman Bridgewater College 1/16/2016
E/M Hunter Layman Bridgewater College 1/16/016 Abstract The charge to mass ratio of an electron was observed in the experiment. This experiment involved the use of a PASCO scientific Model SE 9638 e/m
More informationPhotoelectric Effect
PHYS 201 LAB 02 Photoelectric Effect 1. Objectives The objectives of this experiment is to show that that light behaves like a particle when it interacts with matter, such as electrons on a metal surface.
More informationThe Franck-Hertz Experiment
The Franck-Hertz Experiment Andy Chmilenko, 20310799 Instructor: Tan Dinh Section 1 (Dated: 2:30 pm Wednesday July 10, 2013) I. PURPOSE The purpose of this experiment is to study the quantization of energy
More informationElectric Field and Electric Potential
Electric Field and Electric Potential INTRODUCTION Physicists use the concept of a field 1 to explain the interaction of particles or bodies through space, i.e., the action-at-a-distance 2 force between
More informatione/m APPARATUS Instruction Manual and Experiment Guide for the PASCO scientific Model SE D 5/ PASCO scientific $5.
Includes Teacher's Notes and Typical Experiment Results Instruction Manual and Experiment Guide for the PASCO scientific Model SE9638 020347D 5/94 e/m APPARATUS 987 PASCO scientific $5.00 020347D e/m
More informationPhotoelectric Effect
PC1144 Physics IV Photoelectric Effect 1 Objectives Demonstrate the different predictions of the classical wave and quantum model of light with respect to the photoelectric effect. Determine an experimental
More informationLab 5 - ELECTRON CHARGE-TO-MASS RATIO
79 Name Date Partners OBJECTIVES OVERVIEW Lab 5 - ELECTRON CHARGE-TO-MASS RATIO To understand how electric and magnetic fields impact an electron beam To experimentally determine the electron charge-to-mass
More informationElectric Fields. Goals. Introduction
Lab 2. Electric Fields Goals To understand how contour lines of equal voltage, which are easily measured, relate to the electric field produced by electrically charged objects. To learn how to identify
More informationLab 7 - ELECTRON CHARGE-TO-MASS RATIO
107 Name Date Partners Lab 7 - ELECTRON CHARGE-TO-MASS RATIO OBJECTIVES To understand how electric and magnetic fields impact an electron beam To experimentally determine the electron charge-to-mass ratio
More informationCharge to Mass Ratio of The Electron
Physics Topics Charge to Mass Ratio of The Electron If necessary, review the following topics and relevant textbook sections from Serway / Jewett Physics for Scientists and Engineers, 9th Ed. Electric
More informationConservation of Momentum
Conservation of Momentum 1 Introduction In this lab you will investigate conservation of momentum and the concepts of elastic and inelastic collisions. You will use similar techniques that you developed
More informationThis lab was adapted from Kwantlen University College s Determination of e/m lab.
e /m: Charge to Mass Ratio of the Electron This lab was adapted from Kwantlen University College s Determination of e/m lab. Purpose To determine the charge to mass ratio of the electron, e /m, using Helmholtz
More informationLab 6 - Electron Charge-To-Mass Ratio
Lab 6 Electron Charge-To-Mass Ratio L6-1 Name Date Partners Lab 6 - Electron Charge-To-Mass Ratio OBJECTIVES To understand how electric and magnetic fields impact an electron beam To experimentally determine
More informationLab 6 - ELECTRON CHARGE-TO-MASS RATIO
101 Name Date Partners OBJECTIVES OVERVIEW Lab 6 - ELECTRON CHARGE-TO-MASS RATIO To understand how electric and magnetic fields impact an electron beam To experimentally determine the electron charge-to-mass
More informationCHARGED PARTICLES IN FIELDS
The electron beam used to study motion of charged particles in electric and/or magnetic fields. CHARGED PARTICLES IN FIELDS Physics 41/61 Fall 01 1 Introduction The precise control of charged particles
More informationLC-4: Photoelectric Effect
LC-4: Photoelectric Effect Lab Worksheet Name In this lab you investigate the photoelectric effect, one of the experiments whose explanation by Einstein forced scientists into accepting the ideas of quantum
More informationExperimental Physics I & II "Junior Lab" Fall Spring 2008
MIT OpenCourseWare http://ocw.mit.edu 8.13-14 Experimental Physics I & II "Junior Lab" Fall 2007 - Spring 2008 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms.
More informationExperiment objectives: measure the ratio of Planck s constant to the electron charge h/e using the photoelectric effect.
Chapter 1 Photoelectric Effect Experiment objectives: measure the ratio of Planck s constant to the electron charge h/e using the photoelectric effect. History The photoelectric effect and its understanding
More informationThe Digital Multimeter (DMM)
The Digital Multimeter (DMM) Since Physics 152 covers electricity and magnetism, the analysis of both DC and AC circuits is required. In the lab, you will need to measure resistance, potential (voltage),
More informationImpulse and Conservation of Momentum
SEP0 LABORATORY MANUAL EXPERIMENT 6 EXPERIMENT 6 Impulse and Conservation of Momentum PREPARED BY PASCO SCIENTIFIC AND JOHN LONG FOR THE UNIT TEAM Deakin University 03 EXPERIMENT 6 SEP0 LABORATORY MANUAL
More informationCharge-to-mass ratio for the electron
Charge-to-mass ratio for the electron Introduction This is a variation of the original experiment carried out by J.J.Thomson in 1895. The deflection of a charge moving in a magnetic field is clearly demonstrated.
More informationThe Franck Hertz Experiment and the Ramsauer Townsend Effect: Elastic and Inelastic Scattering of Electrons by Atoms
The Franck Hertz Experiment and the Ramsauer Townsend Effect: Elastic and Inelastic Scattering of Electrons by Atoms MIT Department of Physics (Dated: May 11, 2005) The main purpose of these experiments
More informationTHE CONSERVATION OF LINEAR MOMENTUM
THE CONSERVATION OF LINEAR MOMENTUM Introduction In this experiment you will test the validity of the Law of Conservation of Linear Momentum in one dimension utilizing elastic and inelastic collisions
More informationPHYS320 ilab (O) Experiment 2 Instructions Conservation of Energy: The Electrical Equivalent of Heat
PHYS320 ilab (O) Experiment 2 Instructions Conservation of Energy: The Electrical Equivalent of Heat Objective: The purpose of this activity is to determine whether the energy dissipated by a heating resistor
More informationCharge to Mass Ratio of the Electron
Charge to Mass Ratio of the Electron 1. Purpose: To determine the charge to mass ratio of the electron, e/m, by subjecting a beam of electrons to a magnetic field and examining their trajectories. It can
More informationTo determine relative oxidizing and reducing strengths of a series of metals and ions.
Redox Reactions PURPOSE To determine relative oxidizing and reducing strengths of a series of metals and ions. GOALS 1 To explore the relative oxidizing and reducing strengths of different metals. 2 To
More informationThe Ballistic Pendulum
The Ballistic Pendulum Experimental Objectives The objective of this experiment is to study the law of conservation of momentum. We will apply the principle of conservation of linear momentum to a case
More informationFranck-Hertz experiment, Bohr atom, de Broglie waves Announcements:
Franck-Hertz experiment, Bohr atom, de Broglie waves Announcements: Problem solving sessions Tues. 1-3. Reading for Wednesday TZD 6.1-.4 2013 Nobel Prize Announcement Tomorrow Few slides on the Higgs Field
More informationRatio of Charge to Mass (e/m) for the Electron
Objective: In this experiment you will determine the ratio of charge to mass (e/m) of the electron, by measuring the deflecting of electrons as they move through a magnetic field. Apparatus: e/m apparatus
More informationRC Studies Relaxation Oscillator
RC Studies Relaxation Oscillator Introduction A glass tube containing neon gas will give off its characteristic light when the voltage across the tube exceeds a certain value. The value corresponds to
More informationChanges in Energy and Momentum
Changes in Energy and Momentum Name: Group Members: Date: TA s Name: Learning Objectives: 1. Understanding the relationship between force, distance and changes in kinetic energy. 2. Understanding the relationship
More informationLab in a Box Measuring the e/m ratio
Safety Precautions All the signal voltages are small and harmless. The mains voltages in the mains powered equipment is dangerous but is screened in normal use. The fine beam tube requires dangerous contact
More informationElectron Diffraction
Electron iffraction o moving electrons display wave nature? To answer this question you will direct a beam of electrons through a thin layer of carbon and analyze the resulting pattern. Theory Louis de
More informationMEASUREMENT OF THE CHARGE TO MASS RATIO (e/m e ) OF AN ELECTRON
MEASUREMENT OF THE CHARGE TO MASS RATIO (e/m e ) OF AN ELECTRON Object This experiment will allow you to observe and understand the motion of a charged particle in a magnetic field and to measure the ratio
More informationEXPERIMENT 9 Superconductivity & Ohm s Law
Name: Date: Course number: MAKE SURE YOUR TA OR TI STAMPS EVERY PAGE BEFORE YOU START! Lab section: Partner's name(s): Grade: EXPERIMENT 9 Superconductivity & Ohm s Law 0. Pre-Laboratory Work [2 pts] 1.
More informationM-3: Statics & M-10 Elasticity
Group member names This sheet is the lab document your TA will use to score your lab. It is to be turned in at the end of lab. To receive full credit you must use complete sentences and explain your reasoning
More informationAP Physics 1: Algebra-Based
018 AP Physics 1: Algebra-Based Scoring Guidelines College Board, Advanced Placement Program, AP, AP Central, and the acorn logo are registered trademarks of the College Board. AP Central is the official
More informationExperiment 4: Resistances in Circuits
Name: Partners: Date: Experiment 4: Resistances in Circuits EQUIPMENT NEEDED: Circuits Experiment Board Multimeter Resistors Purpose The purpose of this lab is to begin experimenting with the variables
More informationActivity P27: Speed of Sound in Air (Sound Sensor)
Activity P27: Speed of Sound in Air (Sound Sensor) Concept Speed of sound DataStudio P27 Speed of Sound 1.DS Equipment Needed Qty Other Qty Sound Sensor (CI-6506B) 1 Tape, duct 1 roll Base and Support
More informationThe Phenomena of Quantum Mechanics
Introduction The Phenomena of Quantum Mechanics Quantum mechanics is a general theory. It is presumed to apply to everything, from subatomic particles to galaxies. But interest is naturally focussed on
More informationEXPERIMENT 2-6. e/m OF THE ELECTRON GENERAL DISCUSSION
Columbia Physics: Lab -6 (ver. 10) 1 EXPERMENT -6 e/m OF THE ELECTRON GENERAL DSCUSSON The "discovery" of the electron by J. J. Thomson in 1897 refers to the experiment in which it was shown that "cathode
More informationPRELAB: COLLISIONS Collisions, p. 1/15
PRELAB: COLLISIONS Collisions, p. 1/15 1. What is your Prediction 1-7 when the truck is accelerating? Explain the reasoning behind your prediction. 2. If you set up the force probes according to the instructions
More informationtp03: The Ideal Gas Law
tp03: The Ideal Gas Law Jack Lyes 18/01/2014 The main objective of this experiment was to calculate a value for absolute zero, the temperature at which a gas exerts zero pressure. This was achieved by
More informationMEASUREMENT OF THE CHARGE TO MASS RATIO (e/m e ) OF AN ELECTRON
MEASUREMENT OF THE CHARGE TO MASS RATIO (e/m e ) OF AN ELECTRON Object This experiment will allow you to observe and understand the motion of a charged particle in a magnetic field and to measure the ratio
More informationThe Photoelectric E ect
Physics Topics The Photoelectric E ect If necessary, review the following topics and relevant textbook sections from Serway / Jewett Physics for Scientists and Engineers, 9th Ed. Electric Potential and
More informationExperiment P14: Collision Impulse & Momentum (Force Sensor, Motion Sensor)
PASCO scientific Physics Lab Manual: P14-1 Experiment P14: (Force Sensor, Motion Sensor) Concept Time SW Interface Macintosh file Windows file Newton s Laws 45 m 500 or 700 P14 Collision P14_COLL.SWS EQUIPMENT
More informationPHYSICS B (ADVANCING PHYSICS) 2864/01 Field and Particle Pictures
THIS IS A LEGACY SPECIFICATION ADVANCED GCE PHYSICS B (ADVANCING PHYSICS) 2864/01 Field and Particle Pictures *CUP/T52879* Candidates answer on the question paper OCR Supplied Materials: Data, Formulae
More informationMomentum in One Dimension
Momentum in One Dimension Theory The linear momentum p of an object is defined as p = m v (1) where m is the mass of the object and v its velocity. Note that since velocity is a vector, momentum is as
More informationA fluorescent tube is filled with mercury vapour at low pressure. After mercury atoms have been excited they emit photons.
Q1.(a) A fluorescent tube is filled with mercury vapour at low pressure. After mercury atoms have been excited they emit photons. In which part of the electromagnetic spectrum are these photons? What is
More informationActivity P11: Collision Impulse and Momentum (Force Sensor, Motion Sensor)
Name Class Date Activity P11: Collision Impulse and Momentum (Force Sensor, Motion Sensor) Concept DataStudio ScienceWorkshop (Mac) ScienceWorkshop (Win) Newton s Laws P11 Impulse.DS P14 Collision P14_COLL.SWS
More informationBrown University PHYS 0060 Physics Department LAB B -190
Physics Department LAB B -190 THE FORCE OF A MAGNETIC FIELD ON A MOVING ELECTRIC CHARGE DETERMINATION OF THE RATIO OF CHARGE TO MASS, e/m, FOR ELECTRONS References: H.D. Young, University Physics, Eleventh
More informationSuperconductivity. Never store liquid nitrogen in a container with a tight fitting lid.
Superconductivity 1 Introduction In this lab we will do some very simple experiments involving superconductors. You will not have to take much data; much of what you do will be qualitative. However, in
More informationPhysics 1C OPTICAL SPECTROSCOPY Rev. 2-AH. Introduction
Introduction In this lab you will use a diffraction grating to split up light into its various colors (like a rainbow). You will assemble a spectrometer, incorporating the diffraction grating. A spectrometer
More informationPhysics with Technology
EXAM INFORMATION Items 33 Points 34 Prerequisites NONE Grade Level 10-12 Course Length ONE YEAR DESCRIPTION A STEM course that emphasizes a hands-on learning approach to studying the principles of force,
More informationIncline Plane Activity
Purpose Incline Plane Activity During the activity, students will become familiar with solving static and dynamic incline plane problems. The students will use standard component methods and free body
More informationActivity P24: Conservation of Linear and Angular Momentum (Photogate/Pulley System)
Name Class Date Activity P24: Conservation of Linear and Angular Momentum (Photogate/Pulley System) Concept DataStudio ScienceWorkshop (Mac) ScienceWorkshop (Win) Momentum P24 Linear Angular.DS P28 Cons
More informationPhysics 43, Fall 1995 Lab 1 - Boltzmann's Law
Physics 43, Fall 1995 Lab 1 - Boltzmann's Law Introduction Boltzmann's law states that the probability of occupation of a state of energy E, in a system in equilibrium with a heat bath at temperature T
More informationExperiment 2 Deflection of Electrons
Name Partner(s): Experiment 2 Deflection of Electrons Objectives Equipment Preparation Pre-Lab To study the effects of electric fields on beams of fast moving electrons. Cathode-ray tube (CRT), voltage
More informationhν' Φ e - Gamma spectroscopy - Prelab questions 1. What characteristics distinguish x-rays from gamma rays? Is either more intrinsically dangerous?
Gamma spectroscopy - Prelab questions 1. What characteristics distinguish x-rays from gamma rays? Is either more intrinsically dangerous? 2. Briefly discuss dead time in a detector. What factors are important
More informationThe e/m Ratio of the Electron
OBJECTIVE The e/m Ratio of the Electron To study the behavior of a charged particle in the presence of a potential difference. To study the behavior of a charged particle moving in a magnetic field. To
More informationLab 6: Capacitors and Resistor-Capacitor Circuits Phy208 Spr 2008 Name Section
: Capacitors and Resistor-Capacitor Circuits Phy208 Spr 2008 Name Section Your TA will use this sheet to score your lab. It is to be turned in at the end of lab. You must use complete sentences and clearly
More informationhigh energy state for the electron in the atom low energy state for the electron in the atom
Atomic Spectra Objectives The objectives of this experiment are to: 1) Build and calibrate a simple spectroscope capable of measuring wavelengths of visible light. 2) Measure several wavelengths of light
More informationTHE CHARGE-TO-MASS RATIO OF THE ELECTRON
THE CHARGE-TO-MASS RATIO OF THE ELECTRON Is the beam that produces images on a cathode ray tube (CRT) television or computer monitor a beam of particles or of waves? This was a lively source of debate
More information2 Electric Field Mapping Rev1/05
2 Electric Field Mapping Rev1/05 Theory: An electric field is a vector field that is produced by an electric charge. The source of the field may be a single charge or many charges. To visualize an electric
More informationNewton s Second Law of Motion
Newton s Second Law of Motion Topic Newton s second law of motion describes how acceleration is related to force and mass. Introduction Newton s second law of motion states that the acceleration of an
More informationwhich is deemed to be defective in material or workmanship.
Table of Contents %, Page.. Equipment Return... u Introduction... 1 The Eranck-Hertz Apparatus...:... 2 Important Cautions and Tips... 3 The Experiment: Setup, Operation, and Analysis... 4 Please-feel
More information