sliwa richard franck hertz
TRANSCRIPT
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Frank Hertz ExperimentFrank Hertz Experiment
Ben Richard and Katrina SliwaBen Richard and Katrina Sliwa
PHY243WPHY243W
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Preview of Things to ComePreview of Things to Come
HistoryHistory
TheoryTheory
ApparatusApparatus
IonizationIonization
ExcitationExcitation
ShieldingShielding ConclusionsConclusions
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HistoryHistory
In 1914, by James Franck and Gustav Ludwig HertzIn 1914, by James Franck and Gustav Ludwig Hertz
One year after Bohrs theory of quantized energy statesOne year after Bohrs theory of quantized energy states
Nobel Prize in 1925: for their discovery of the lawsNobel Prize in 1925: for their discovery of the laws
governing the impact of an electron upon an atomgoverning the impact of an electron upon an atom
Photos: Copyright The Nobel Foundation
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Energy LevelsEnergy Levels
Bohr: discrete energy levelsBohr: discrete energy levels
Excite electrons with electron impactExcite electrons with electron impact
Hg: 80 electronsHg: 80 electrons
Excited transitions from electronsExcited transitions from electrons
33PP00
11SS00 ((4.6 eV)4.6 eV)
33PP11 11SS00 ((4.9 eV)4.9 eV)
33PP22
11SS00 ((5.4 eV)5.4 eV)
11PP11
11SS00 ((6.7 eV)6.7 eV)
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Electron ScatteringElectron Scattering
Why Hg?Why Hg?
Monoatomic vaporMonoatomic vapor
Easy to control vapor pressureEasy to control vapor pressure
Mean free path through a gas in a cavity:Mean free path through a gas in a cavity:
I = (2I = (2nRnR00))--
Kinetic energy gained in an electric field during I:Kinetic energy gained in an electric field during I:
K = eEIK = eEI
Elastic scattering: K
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Frank Hertz Vacuum TubeFrank Hertz Vacuum Tube
Anode
Cathode (VF)
Grid (VCG
)
Electric field
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Frank HertzBox
Control Box
MultimeterElectrometer
To Computer
A
G
F C
Experimental SetupExperimental Setup
Thermometer
B
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IonizationIonization
Anode at negative potential w.r.t. cathodeAnode at negative potential w.r.t. cathode
Grid at positive potential w.r.t. cathodeGrid at positive potential w.r.t. cathode
Electrons can ionize mercuryElectrons can ionize mercury
positive Hg ions pulled toward anodepositive Hg ions pulled toward anode
SettingsSettings
Retarding voltage: 1.5 VRetarding voltage: 1.5 V VVff= 6.3 V= 6.3 V
Temperature from 100Temperature from 10000C to 185C to 18500CC
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Temperature ResultsTemperature Results
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Ionization ResultsIonization Results
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ExcitationExcitation
Retarding voltage: 1.5 VRetarding voltage: 1.5 V VVff= 6.30 V= 6.30 V
0 V < V0 V < Vcgcg < 45 V in 0.1 V steps< 45 V in 0.1 V steps
Assumptions:Assumptions:
KKe cathodee cathode= 0= 0
All electrons with KAll electrons with K
ee < eV< eV
retardingretarding captured by gridcaptured by grid
Electrons with required energy travel negligibleElectrons with required energy travel negligible
distances before collisiondistances before collision
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Excitation resultsExcitation results
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Excitation resultsExcitation results
Avg dist between peaks: 4.93Avg dist between peaks: 4.93+/- .25 eV+/- .25 eV For Hg:For Hg:E = 4.6 eV, 4.9 eV, 5.4 eV, 6.7 eVE = 4.6 eV, 4.9 eV, 5.4 eV, 6.7 eV
LifetimeLifetime
33
PP00 11
SS00 >> Lifetime>> Lifetime33
PP11 11
SS00 Accepted value: 4.9 eVAccepted value: 4.9 eV
h = Veh = Ve/c;/c; = 253.6 x 10= 253.6 x 10-9-9 mm
h = 6.63 +/- .34 x 10h = 6.63 +/- .34 x 10-34-34 JsJs
Accepted value: h=Accepted value: h=6.626 x 106.626 x 10-34-34 JsJs
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Excitation ObservationsExcitation Observations
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Excitation ObservationsExcitation Observations
www.physics.umd.edu/.../demos/demosn2/n2-06.htm
http://www.physics.umd.edu/.../demos/demosn2/n2-06.htmhttp://www.physics.umd.edu/.../demos/demosn2/n2-06.htmhttp://www.physics.umd.edu/.../demos/demosn2/n2-06.htmhttp://www.physics.umd.edu/.../demos/demosn2/n2-06.htm -
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ElectrometerElectrometer
Very sensitive to external electric fieldsVery sensitive to external electric fields
Attempted to create grounded tin foil shieldAttempted to create grounded tin foil shield
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ConclusionsConclusions
Inconclusive ionization resultsInconclusive ionization results
Found excitation peaks at: 4.93Found excitation peaks at: 4.93 +/- .25 eV+/- .25 eV
Measured h to be: 6.63 +/- .34 x 10Measured h to be: 6.63 +/- .34 x 10-34-34
JsJs Future work:Future work:
Fine tune parameters for ionizationFine tune parameters for ionization
Obtain VObtain Vff experimentallyexperimentally Create better shield for electrometerCreate better shield for electrometer
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ReferencesReferences
UR Advanced Laboratory Manual, The Franck-HertzExperiment [Online]http://www.pas.rochester.edu/~AdvLab/2-Frank-Hertz/La
K. M. Beck and J. Mainzer, The Franck-HertzExperiment [Online] http://www.pas.rochester.edu/~advlab/reports/beck_mainzer_franckhertz.pdf
A. C. Melissinos, Experiments in Modern PhysicsAcademic Press (1966)
C. J. SansonettiC. J. Sansonetti et al.et al., Phys. Scr., Phys. Scr. 6363 219-242, 2001219-242, 2001
Nobel FoundationNobel Foundationhttp://nobelprize.org/nobel_prizes/physics/laureahttp://nobelprize.org/nobel_prizes/physics/laureates/1925/index.htmltes/1925/index.html
http://www.pas.rochester.edu/~AdvLab/2-Frank-Hertz/Lab02%20Hertz.pdfhttp://www.pas.rochester.edu/~advlab/reports/http://www.pas.rochester.edu/~advlab/reports/http://www.pas.rochester.edu/~advlab/reports/http://www.pas.rochester.edu/~advlab/reports/http://www.pas.rochester.edu/~advlab/reports/http://www.pas.rochester.edu/~advlab/reports/http://www.pas.rochester.edu/~advlab/reports/http://www.pas.rochester.edu/~advlab/reports/http://www.pas.rochester.edu/~advlab/reports/http://www.pas.rochester.edu/~AdvLab/2-Frank-Hertz/Lab02%20Hertz.pdf