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Welcome to 3.091 Lecture 3 September 14, 2009 Atomic Models: Rutherford & Bohr
34

Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

Dec 29, 2016

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Page 1: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

Welcome to 3.091Lecture 3

September 14, 2009

Atomic Models: Rutherford & Bohr

Page 2: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

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33 34 35 36

39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54

57 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86

37 38

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87 88 89

Periodic Table Quiz

Name Grade /10

Image by MIT OpenCourseWare.

Page 3: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

La Lazy Ce collegePr professorsNd neverPm produceSm sufficientlyEu educatedGd graduatesTb toDy dramaticallyHo helpEr executivesTm trimYb yearlyLu losses.

© source unknown. All rights reserved. This image is excluded from our Creative Commons license. For more information, see http://ocw.mit.edu/fairuse.

Page 4: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

La Loony Ce chemistryPr professorNd needsPm partner:Sm seekingEu educatedGd graduateTb toDy developHo hazardousEr experimentsTm testingYb youngLu lab assistants.

cannot be referring to 3.091!

must be the “other” chemistry professor

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Page 5: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

CEase not I to slave, back breaking to tend;PRideless and bootless stoking hearth and fire.No Dream of mine own precious time to spendPour'ed More to sate your glutt'nous desire.SMelting anew my ten-thousandth hourEUtopia forever I eschew.Growing Dimmer is my fleeing powerTo Bid these curs'ed problem sets adieu.DYing away whilst thy hosts are foughtHOpeless I come should in lecture I doze.ERgo, like a sad slave, stay and rest nought.Then Must I tool and toil while fatigue grows. Yet, Bloody though I must be, and quite ill Light the Universal abyss I will.

57138.905592034556.1461.105.577[Xe]5d16s2

Lanthanum

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La3*

Courtesy of MIT Student. Used with permission.

Page 6: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

The Structure of the Atomstatus report ca. end of the 19th century

* atom is electrically neutral

* -ve charge carried by electrons

* e- has very small mass

bulk of the atom is +ve,

most mass resides in +ve charge

Question: what is the spatial distribution of charge inside an atom?

Page 7: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

Figure 1.18

Image by MIT OpenCourseWare.

Page 8: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

Figure 1.19

Paper0.5- cm lead10-cm lead

γ rays

β particles

α particles

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Page 9: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

Rutherford-Geiger-Marsden experiment

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Page 10: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

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Page 11: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

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Page 12: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

b

Marsden's Analysis

Scattering of an α-particle which approaches a heavy nucleus with an impact parameter b.

θTrajectory of incident α particle

gold nucleus

Image by MIT OpenCourseWare.

Page 13: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

principles of modern chemistry:

* recognize patterns

* develop a quantitative model that - explains our observations - makes predictions that can be tested by experiment

Page 14: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT
Page 15: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT
Page 16: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT
Page 17: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT
Page 18: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

Bohr Postulates for the Hydrogen Atom 1. Rutherford atom is correct 2. Classical EM theory not applicable to orbiting e-

3. Newtonian mechanics applicable to orbiting e-

4. Eelectron = Ekinetic + Epotential

5. e- energy quantized through its angular momentum: L = mvr = nh/2π, n = 1, 2, 3,…

6. Planck-Einstein relation applies to e- transitions: ΔE = Ef - Ei = hν = hc/λ

c = νλ

Page 19: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

Bohr Postulates for the Hydrogen Atom 1. Rutherford atom is correct 2. Classical EM theory not applicable to orbiting e-

3. Newtonian mechanics applicable to orbiting e-

4. Eelectron = Ekinetic + Epotential

5. e- energy quantized through its angular momentum: L = mvr = nh/2π, n = 1, 2, 3,…

6. Planck-Einstein relation applies to e- transitions: ΔE = Ef - Ei = hν = hc/λ

c = νλ

Page 20: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

Image by MIT OpenCourseWare.

Page 21: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

Bohr Postulates for the Hydrogen Atom 1. Rutherford atom is correct 2. Classical EM theory not applicable to orbiting e-

3. Newtonian mechanics applicable to orbiting e-

4. Eelectron = Ekinetic + Epotential

5. e- energy quantized through its angular momentum: L = mvr = nh/2π, n = 1, 2, 3,…

6. Planck-Einstein relation applies to e- transitions: ΔE = Ef - Ei = hν = hc/λ

c = νλ

Page 22: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

Bohr Postulates for the Hydrogen Atom 1. Rutherford atom is correct 2. Classical EM theory not applicable to orbiting e-

3. Newtonian mechanics applicable to orbiting e-

4. Eelectron = Ekinetic + Epotential

5. e- energy quantized through its angular momentum: L = mvr = nh/2π, n = 1, 2, 3,…

6. Planck-Einstein relation applies to e- transitions: ΔE = Ef - Ei = hν = hc/λ

c = νλ

Page 23: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

0 500 1000 1500 2000 2500 3000

5000 K

4000 K

3000 K

Rad

iatio

n in

tens

ity

Wavelength (nm)

Classical prediction6000 K

E = hν

Planck suggests that light is composed of energypackets or quanta. The elementary unit of e-mradiation is the photon.

InfraredVisibleUV

6000 K

Image by MIT OpenCourseWare.

Page 24: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

Bohr Postulates for the Hydrogen Atom 1. Rutherford atom is correct 2. Classical EM theory not applicable to orbiting e-

3. Newtonian mechanics applicable to orbiting e-

4. Eelectron = Ekinetic + Epotential

5. e- energy quantized through its angular momentum: L = mvr = nh/2π, n = 1, 2, 3,…

6. Planck-Einstein relation applies to e- transitions: ΔE = Ef - Ei = hν = hc/λ

c = νλ

Page 25: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

Image by MIT OpenCourseWare.

Page 26: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

© source unknown. All rights reserved. This image is excluded from our Creative Commonslicense.For more information,

see http://ocw.mit.edu/fairuse.

Page 27: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

© source unknown. All rightsreserved. This image isexcluded from our CreativeCommons license. For moreinformation, seehttp://ocw.mit.edu/fairuse.

Page 28: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

© source unknown. All rights reserved. This image is excluded from ourCreative Commons license. For more information, see http://ocw.mit.edu/fairuse.

Page 29: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

© source unknown. All rights reserved. This image is excluded from ourCreative Commons license. For more information, see http://ocw.mit.edu/fairuse.

Page 30: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

© source unknown. All rights reserved. This image is excluded from ourCreative Commons license. For more information, see http://ocw.mit.edu/fairuse.

Page 31: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

Isotopes of Hydrogen

hydrogen1766 Henry Cavendish, London

deuterium

1931 Harold Urey, Columbia U. tritium

1934 Ernest Rutherford, Cambridge U.

Page 32: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

Dalton proposes theindivisible unit of an element is the atom.

1803

Thomson discovers electrons,believed to reside within a sphere of uniform positive

charge (the "plum pudding" model).

1904

Rutherford demonstrates the existence of a positively chargednucleus that contains nearly all

the mass of an atom.

1911

Bohr proposes fixed circularorbits around the nucleus

for electrons.

1913

In the current model of theatom, electrons occupy regions of space (orbitals) around the

nucleus determined by their energies.

1926

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Page 33: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

J. J. Thomson (1856-1940)Cathode ray = Charged particle = Electron (1897)charge-to-mass ratio of electron (1897)

J.J Thomson"Plum pudding" model of atom (1904)

Robert Millikan (1868-1953) Charge and mass of electron (1909)

James Chadwick (1891-1974)Neutron (1932)

Ernest RutherfordProton (1920)

Ernest RutherfordNuclear model of atom (1911)

Ernest Rutherford (1871-1937)α and β particles (1898)

Marie and Pierre Curie(1867-1934, 1854-1906)Radioactive elements polonium and radium (1898)

Henri Becquerel (1852-1908)Uranium emits rays that fog photographic film (1869)

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Page 34: Lecture #3, Atomic Structure ( Rutherford , Bohr Models) - MIT

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3.091SC Introduction to Solid State ChemistryFall 2009

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