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The Hydrogen Atom and the Periodic Table

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The Hydrogen Atom and the Periodic Table. Chapter 4 of Solymar. The Hydrogen Atom ... Periodic Table Summary. Schrodinger's equation gives a set of discrete states ... – PowerPoint PPT presentation

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Title: The Hydrogen Atom and the Periodic Table


1
The Hydrogen Atom and the Periodic Table
  • Chapter 4 of Solymar

2
The Hydrogen Atom
  • The simplest atom
  • A proton and an electron
  • Questions
  • What is the probability of finding the electron
    at a distance from the proton?
  • What are the allowed energy levels?
  • Time-independent Schrodingers equation

3
Schrodingers Equation
  • Proton sits in the center (origin)
  • Electron orbits proton in a spherical fashion
  • The potential energy of the electron given by
    electrostatics
  • Schrodingers equation becomes
  • Its tedious and boring to solve it, so lets
    limit to the simplest case, the spherically
    symmetric solution

4
Spherical Coordinate System
  • The spherical coordinate system best suited for
    the spherical solution (Fig. 4.1)
  • r, q, and f
  • For a spherically symmetric case, y depends
    neither on f nor on q, but only on r

5
More Derivation
  • Similar for y and z
  • Since

6
More Derivation
  • In spherical coordinate system

7
Schrodingers Equation Again
  • Schrodingers equation in spherical coordinate
    system
  • A spherically symmetric solution is

8
Solution
  • When put back into the equation
  • For any r
  • This agrees with the lowest energy level of
    hydrogen

9
Probability of Finding Electron
  • Probability of finding the electron
  • Highest probability at origin ( r 0 )
  • What is the probability of finding the electron
    in the spherical shell between r and r dr?
  • The maximum is (Fig. 4.2)
  • This is Bohr radius of the first orbit

10
Other Solutions
  • Still consider spherically symmetric cases
  • Ln(r) is a polynomial
  • Energy level
  • n 1, 2, 3,
  • n 1 gives the lowest energy level, which is
    called the ground state
  • Probability distributions of excited states (Fig.
    4.3, n 2, 3, )
  • The maximum gets further away from the proton

11
Quantum Numbers
  • The general solution
  • n, l, ml are quantum numbers
  • n 1, 2, 3,
  • l 0, 1, 2, , n-1
  • ml 0, ?1, ?2, , ?l
  • For n 1, l 0, ml 0, the solution is
  • For n 2, 3, l 0, ml 0, the solutions are in
    Fig. 4.3
  • These are all spherically symmetric

12
Cylindrically Symmetric Solution
  • For n 2, l 1, ml 0, the solution
  • Its no longer spherically symmetric, but
    cylindrically symmetric
  • Dumbbell shaped (Fig. 4.4)
  • A plot in the x-z plane
  • Maximum probability at x 0 and z ?2/Co (or q
    0 and p, r 2/Co)
  • For n 2, l 1, ml ?1, the dumbbell is in the
    x or y direction

13
Notation
  • The notation for quantum numbers
  • For example, in 3 p
  • 3 is quantum number n
  • p is quantum number l
  • l 0 1 2 3 4 5 6 7
  • s p d f g h i k

14
Electron Spin
  • There is one more quantum number
  • Spin quantum number s
  • It takes values ?1/2
  • There are in total four quantum numbers
  • n, l, ml, s
  • Any permissible combination of these quantum
    numbers gives a state
  • Once the four quantum numbers are given, the
    wavefunction is defined, and the electrons
    energy is determined

15
Paulis Exclusion Principle
  • Question
  • How many electrons can occupy the same state
    defined by a permissible combination of the 4
    quantum numbers?
  • Answer is ONE
  • There can be no more than one electron in any
    given state Paulis exclusion principle
  • It can be derived from a relativistic quantum
    theory

16
The Helium Atom
  • The helium atom has two protons and two electrons
  • Two differential operators for two electrons
  • Potential energy for electron 1
    , for electron 2
  • For interaction between 1 and 2
  • Schrodingers equationelectrons
  • It can not be solved without many assumptions

17
No Electron Interaction
  • One assumption we can make is
  • There are no interactions between electrons
  • When there are Z protons in the nucleus
  • More energy is needed to liberate an electron
    when Z 1
  • This allows us to build the periodic table

18
Building the Periodic Table
  • We have all the knowledge required to build the
    periodic table
  • Lets begin with the lowest energy level n 1, l
    0, ml 0, s ?1/2
  • The state can take up to two electrons
  • One electron gives hydrogen
  • Two electrons give helium
  • Now the n 1 shell is fully occupied
  • It doesnt want to give up any of its electrons
  • It cant take another electron
  • Helium is chemically inert

19
Periodic Table n 2
  • Now n has to go to 2 (n 2, Table 4.1)
  • Lithium has two electrons with n 1 and l 0
    one electron with n 2 and l 0 1s22s1
  • It can give up the 2s electron easily, so its a
    metal
  • Beryllium 1s22s2
  • Boron has two electrons with n 1 and l 0 two
    electrons with n 2 and l 0 one electron with
    n 2, l 1 1s22s22p1
  • Carbon 1s22s22p2
  • Nitrogen 1s22s22p3
  • Oxygen 1s22s22p4

20
Periodic Table n 2
  • n 2
  • Fluorine 1s22s22p5
  • For n 2 and l 1, ml can be 0, 1, -1 and s
    can be ½ and 1/2, so it can take up to six
    electrons
  • Fluorine has five 2p electrons and wants to take
    one more electron
  • When Li meets F, Li gives up one electron and F
    takes it. Both now have closed n 2 shell
  • They form a compound or chemical bond due to
    electrostatic attraction
  • Neon is chemically inert 1s22s22p6

21
Periodic Table n 3
  • Now n has to go to 3 (n 3, Table 4.1)
  • Sodium behaves like Li 1s22s22p63s1
  • Magnesium 1s22s22p63s2
  • Aluminum 1s22s22p63s23p1
  • Silicon 1s22s22p63s23p2
  • Phosphorous 1s22s22p63s23p3
  • Sulfur 1s22s22p63s23p4
  • Chlorine behaves like F 1s22s22p63s23p5
  • Argon is chemically inert 1s22s22p63s23p6

22
Periodic Table n 4
  • Potassium 1s22s22p63s23p64s1
  • 4s instead of 3d, because 4s states have lower
    energy than 3d states
  • Due to electron interactions
  • 4p states have higher energy than 3d states
  • Transition metals
  • Scandium 1s22s22p63s23p63d14s2
  • Chromium 1s22s22p63s23p63d54s1
  • Copper 1s22s22p63s23p63d104s1
  • Krypton inert 1s22s22p63s23p63d104s24p6

23
Periodic Table n 5
  • More irregularities
  • Rare-earth metals
  • Eleven electrons occupy the n 5 shell while 4f
    states are being filled
  • They are chemically similar

24
Periodic Table Summary
  • Schrodingers equation gives a set of discrete
    states
  • Paulis exclusion principle prohibits more than
    one electron per state
  • Electrons are filled into these states
  • There is a slow variation of energy within a
    shell
  • There is a large energy difference between shells
  • Alkali elements starts new shells with one
    electron
  • They can easily lose the electron
  • Halogen electrons have one less electron in the
    out shell
  • They want to get an extra electron to close the
    shell

25
HW Assignment
  • 4.2, 4.3, 4.5, 4.7
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