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Chapter 28 Atomic Physics.

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1 Chapter 28 Atomic Physics

2 Plum Pudding Model of the Atom
J. J. Thomson’s “Plum Pudding” model of the atom: Electrons embedded throughout the a volume of positive charge A change from Newton’s model of the atom as a tiny, hard, indestructible sphere Sir Joseph John Thomson 1856 – 1940

3 Scattering Experiments
Ernest Rutherford 1871 – 1937 The source was a naturally radioactive material that produced alpha particles Most of the alpha particles passed though the foil A few deflected from their original paths Some even reversed their direction of travel

4 Planetary Model of the Atom
Based on results of thin foil scattering experiments, Rutherford’s Planetary model of the atom: Positive charge is concentrated in the center of the atom, called the nucleus Electrons orbit the nucleus like planets orbit the sun

5 Chapter 28 Problem 6 In a Rutherford scattering experiment, an α-particle (charge = +2e) heads directly toward a gold nucleus (charge = +79e). The α-particle had a kinetic energy of 5.0 MeV when very far (r → ∞) from the nucleus. Assuming the gold nucleus to be fixed in space, determine the distance of closest approach.

6 Difficulties with the Rutherford Model
Atoms emit certain discrete characteristic frequencies of electromagnetic radiation but the Rutherford model is unable to explain this phenomena Rutherford’s electrons are undergoing a centripetal acceleration and so should radiate electromagnetic waves of the same frequency The radius should steadily decrease as this radiation is given off The electron should eventually spiral into the nucleus, but it doesn’t

7 Emission Spectra A gas at low pressure and a voltage applied to it emits light characteristic of the gas When the emitted light is analyzed with a spectrometer, a series of discrete bright lines –emission spectrum – is observed Each line has a different wavelength and color

8 Emission Spectrum of Hydrogen
The wavelengths of hydrogen’s spectral lines can be found from RH = x 107 m-1 is the Rydberg constant and n is an integer, n = 3, 4, 5, … The spectral lines correspond to different values of n n = 3, λ = nm n = 4, λ = nm Johannes Robert Rydberg 1854 – 1919

9 Absorption Spectra An element can also absorb light at specific wavelengths An absorption spectrum can be obtained by passing a continuous radiation spectrum through a vapor of the gas Such spectrum consists of a series of dark lines superimposed on the otherwise continuous spectrum The dark lines of the absorption spectrum coincide with the bright lines of the emission spectrum

10 The Bohr Theory of Hydrogen
In 1913 Bohr provided an explanation of atomic spectra that includes some features of the currently accepted theory His model was an attempt to explain why the atom was stable and included both classical and non-classical ideas Niels Henrik David Bohr 1885 – 1962

11 The Bohr Theory of Hydrogen
The electron moves in circular orbits around the proton under the influence of the Coulomb force of attraction, which produces the centripetal acceleration Only certain electron orbits are stable In these orbits electrons do not emit energy in the form of electromagnetic radiation Therefore, the energy of the atom remains constant and classical mechanics can be used to describe the electron’s motion

12 The Bohr Theory of Hydrogen
Radiation is emitted when the electrons “jump” (not in a classical sense) from a more energetic initial state to a lower state The frequency emitted in the “jump” is related to the change in the atom’s energy: Ei – Ef = h ƒ The size of the allowed electron orbits is determined by a quantization condition imposed on the electron’s orbital angular momentum: me v r = n ħ where n = 1, 2, 3, …; ħ = h / 2 π

13 Radii and Energies of Orbits

14 Radii and Energies of Orbits

15 Radii and Energies of Orbits
The radii of the Bohr orbits are quantized When n = 1, the orbit has the smallest radius, called the Bohr radius, ao = nm A general expression for the radius of any orbit in a hydrogen atom is rn = n2 ao

16 Radii and Energies of Orbits
The lowest energy state (n = 1) is called the ground state, with energy of –13.6 eV The next energy level (n = 2) has an energy of –3.40 eV The energies can be compiled in an energy level diagram with the energy of any orbit of En = eV / n2

17 Energy Level Diagram

18 Energy Level Diagram The value of RH from Bohr’s analysis is in excellent agreement with the experimental value of the Rydberg constant A more generalized equation can be used to find the wavelengths of any spectral lines

19 Energy Level Diagram The uppermost level corresponds to E = 0 and n   The ionization energy: energy needed to completely remove the electron from the atom The ionization energy for hydrogen is 13.6 eV

20 Chapter 28 Problem 18 A particle of charge q and mass m, moving with a constant speed v, perpendicular to a constant magnetic field, B, follows a circular path. If in this case the angular momentum about the center of this circle is quantized so that mvr = 2nħ, show that the expression for the allowed radii for the particle is written in the corner, where n = 1, 2, 3, . . .

21 Chapter 28 Problem 24 Two hydrogen atoms collide head-on and end up with zero kinetic energy. Each then emits a nm photon (n = 2 to n = 1 transition). At what speed were the atoms moving before the collision?

22 Modifications of the Bohr Theory – Elliptical Orbits
Sommerfeld extended the results to include elliptical orbits Retained the principle quantum number, n, which determines the energy of the allowed states Added the orbital quantum number, ℓ, ranging from 0 to n-1 in integer steps All states with the same principle quantum number are said to form a shell, whereas the states with given values of n and ℓ are said to form a subshell Arnold Johannes Wilhelm Sommerfeld 1868 – 1951

23 Modifications of the Bohr Theory – Elliptical Orbits
Arnold Johannes Wilhelm Sommerfeld 1868 – 1951

24 Modifications of the Bohr Theory – Zeeman Effect
Another modification was needed to account for the Zeeman effect: splitting of spectral lines in a strong magnetic field, indicating that the energy of an electron is slightly modified when the atom is immersed in a magnetic field A new quantum number, m ℓ, called the orbital magnetic quantum number, had to be introduced m ℓ can vary from - ℓ to + ℓ in integer steps Pieter Zeeman 1865 – 1943

25 Quantum Number Summary
The values of n can range from 1 to  in integer steps The values of ℓ can range from 0 to n-1 in integer steps The values of m ℓ can range from -ℓ to ℓ in integer steps

26 Modifications of the Bohr Theory – Fine Structure
High resolution spectrometers show that spectral lines are, in fact, two very closely spaced lines, even in the absence of a magnetic field This splitting is called fine structure Another quantum number, ms, called the spin magnetic quantum number, was introduced to explain the fine structure

27 Spin Magnetic Quantum Number
It is convenient to think of the electron as spinning on its axis (the electron is not physically spinning) There are two directions for the spin: spin up, ms = ½; spin down, ms = - ½ There is a slight energy difference between the two spins and this accounts for the doublet in some lines A classical description of electron spin is incorrect: the electron cannot be located precisely in space, thus it cannot be considered to be a spinning solid object

28 de Broglie Waves in the Hydrogen Atom
One of Bohr’s postulates was the angular momentum of the electron is quantized, but there was no explanation why the restriction occurred de Broglie assumed that the electron orbit would be stable only if it contained an integral number of electron wavelengths

29 de Broglie Waves in the Hydrogen Atom
This was the first convincing argument that the wave nature of matter was at the heart of the behavior of atomic systems By applying wave theory to the electrons in an atom, de Broglie was able to explain the appearance of integers in Bohr’s equations as a natural consequence of standing wave patterns

30 Quantum Mechanics and the Hydrogen Atom
Schrödinger’s wave equation was subsequently applied to hydrogen and other atomic systems - one of the first great achievements of quantum mechanics The quantum numbers and the restrictions placed on their values arise directly from the mathematics and not from any assumptions made to make the theory agree with experiments

31 Electron Clouds The graph shows the solution to the wave equation for hydrogen in the ground state The curve peaks at the Bohr radius The electron is not confined to a particular orbital distance from the nucleus The probability of finding the electron at the Bohr radius is a maximum

32 Electron Clouds The wave function for hydrogen in the ground state is symmetric The electron can be found in a spherical region surrounding the nucleus The result is interpreted by viewing the electron as a cloud surrounding the nucleus The densest regions of the cloud represent the highest probability for finding the electron

33 The Pauli Exclusion Principle
No two electrons in an atom or in the same location can ever have the same set of values of the quantum numbers n, ℓ, m ℓ, and ms This explains the electronic structure of complex atoms as a succession of filled energy levels with different quantum numbers Wolfgang Ernst Pauli 1900 – 1958

34 Filling Shells As a general rule, the order that electrons fill an atom’s subshell is: 1) Once one subshell is filled, the next electron goes into the vacant subshell that is lowest in energy 2) Otherwise, the electron would radiate energy until it reached the subshell with the lowest energy 3) A subshell is filled when it holds 2(2ℓ+1) electrons

35 Filling Shells

36 Dmitriy Ivanovich Mendeleyev
The Periodic Table The outermost electrons are primarily responsible for the chemical properties of the atom Mendeleev arranged the elements according to their atomic masses and chemical similarities The electronic configuration of the elements is explained by quantum numbers and Pauli’s Exclusion Principle Dmitriy Ivanovich Mendeleyev 1834 – 1907

37 The Periodic Table


39 Chapter 28 Problem 28 (a) Construct an energy level diagram for the He+ ion, for which Z = 2. (b) What is the ionization energy for He+?

40 Explanation of Characteristic X-Rays
The details of atomic structure can be used to explain characteristic x-rays A bombarding electron collides with an electron in the target metal that is in an inner shell If there is sufficient energy, the electron is removed from the target atom

41 Explanation of Characteristic X-Rays
The vacancy created by the lost electron is filled by an electron falling to the vacancy from a higher energy level The transition is accompanied by the emission of a photon whose energy is equal to the difference between the two levels

42 Energy Bands in Solids In solids, the discrete energy levels of isolated atoms broaden into allowed energy bands separated by forbidden gaps The separation and the electron population of the highest bands determine whether the solid is a conductor, an insulator, or a semiconductor

43 Energy Bands in Solids Sodium example
Blue represents energy bands occupied by the sodium electrons when the atoms are in their ground states, gold represents energy bands that are empty, and white represents energy gaps Electrons can have any energy within the allowed bands and cannot have energies in the gaps

44 Energy Level Definitions
The valence band is the highest filled band The conduction band is the next higher empty band The energy gap has an energy, Eg, equal to the difference in energy between the top of the valence band and the bottom of the conduction band

45 Conductors When a voltage is applied to a conductor, the electrons accelerate and gain energy In quantum terms, electron energies increase if there are a high number of unoccupied energy levels for the electron to jump to For example, it takes very little energy for electrons to jump from the partially filled to one of the nearby empty states

46 Insulators The valence band is completely full of electrons
A large band gap separates the valence and conduction bands A large amount of energy is needed for an electron to be able to jump from the valence to the conduction band The minimum required energy is Eg

47 Semiconductors A semiconductor has a small energy gap
Thermally excited electrons have enough energy to cross the band gap The resistivity of semiconductors decreases with increases in temperature The light-color area in the valence band represents holes – empty states in the valence band created by electrons that have jumped to the conduction band

48 Semiconductors Some electrons in the valence band move to fill the holes and therefore also carry current The valence electrons that fill the holes leave behind other holes It is common to view the conduction process in the valence band as a flow of positive holes toward the negative electrode applied to the semiconductor

49 Semiconductors An external voltage is supplied
Electrons move toward the positive electrode Holes move toward the negative electrode There is a symmetrical current process in a semiconductor

50 Doping in Semiconductors
Doping is the adding of impurities to a semiconductor (generally about 1 impurity atom per 107 semiconductor atoms) Doping results in both the band structure and the resistivity being changed

51 n-type Semiconductors
Donor atoms are doping materials that contain one more electron than the semiconductor material This creates an essentially free electron with an energy level in the energy gap, just below the conduction band Only a small amount of thermal energy is needed to cause this electron to move into the conduction band

52 p-type Semiconductors
Acceptor atoms are doping materials that contain one less electron than the semiconductor material A hole is left where the missing electron would be The energy level of the hole lies in the energy gap, just above the valence band An electron from the valence band has enough thermal energy to fill this impurity level, leaving behind a hole in the valence band

53 A p-n Junction A p-n junction is formed when a p-type semiconductor is joined to an n-type Three distinct regions exist: a p region, an n region, and a depletion region Mobile donor electrons from the n side nearest the junction diffuse to the p side, leaving behind immobile positive ions

54 A p-n Junction At the same time, holes from the p side nearest the junction diffuse to the n side and leave behind a region of fixed negative ions The resulting depletion region is depleted of mobile charge carriers There is also an electric field in this region that sweeps out mobile charge carriers to keep the region truly depleted

55 Diode Action The p-n junction has the ability to pass current in only one direction When the p-side is connected to a positive terminal, the device is forward biased and current flows When the n-side is connected to the positive terminal, the device is reverse biased and a very small reverse current results

56 Answers to Even Numbered Problems
Chapter 28: Problem 34 4 7

57 Answers to Even Numbered Problems
Chapter 28: Problem 36 Use the lecture notes

58 Answers to Even Numbered Problems
Chapter 28: Problem 44 137

59 Answers to Even Numbered Problems
Chapter 28: Problem 52 135 eV ~ 10 times the magnitude of the ground state energy of hydrogen

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