after pointing out several discrepancies between electron difference density results and lewis...

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After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics. The wave function Ψ, which beginning students find confusing, was equally confusing to the physicists who created quantum mechanics. The Schroedinger equation reckons kinetic energy through the shape of Ψ. When Ψ curves toward zero, kinetic energy is positive; but when it curves away, kinetic energy is negative! A simple tool allows finding Ψ for one-dimensional problems. Chemistry 125: Lecture 7 Sept. 16, 2009 Quantum Mechanical Kinetic Energy For copyright notice see final page of this file

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Page 1: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

After pointing out several discrepancies between electron difference density results and

Lewis bonding theory, the course introduces quantum mechanics. The wave function Ψ,

which beginning students find confusing, was equally confusing to the physicists who created

quantum mechanics. The Schroedinger equation reckons kinetic energy through the shape

of Ψ. When Ψ curves toward zero, kinetic energy is positive; but when it curves away, kinetic

energy is negative! A simple tool allows finding Ψ for one-dimensional problems.

Chemistry 125: Lecture 7Sept. 16, 2009

Quantum MechanicalKinetic Energy

For copyright notice see final page of this file

Page 2: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

Exam 1 - Friday, Sept. 25 !

Exam Review 8-10 pm Wednesday, Sept. 23, Room TBA

Covers Lectures through Wednesday, Sept. 23

Including:

Functional GroupsX-Ray Diffraction

1-Dimensional Quantum Mechanics & 1-Electron Atoms

(Sections I-V of quantum webpage& Erwin Meets Goldilocks )

Get-aquainted with Erwin at Thursday Discussion

IMPORTANT PROBLEMStherein due Monday, Sept. 21

Page 3: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

Dunitz et al. (1981)

Page 4: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

Dunitz et al. (1981)

Surprising only for its beauty

Page 5: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

Lone "Pair"of N atom

Dunitz et al. (1981)

Bond Cross SectionsMissing Bond?

H

H

H

H

HH

Pathological Bonding

Page 6: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

Dunitz et al. (1981)

MissingBond !

BentBonds !

In three weeks we’ll understand these pathologies.

Pathological Bonding

Page 7: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

Lewis Pairs/Octets provide a pretty good bookkeeping device

for keeping track of valencebut they are hopelessly crude when it comes to describing actual electron distribution.

There is electron sharing (~5% of Lewis's prediction).

There are unshared "pairs" (<5% of Lewis's prediction).

Page 8: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

Is there a Better Bond Theory, maybe even a Quantitative one?

YES!Chemical Quantum

Mechanics

Page 9: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

Erwin Schrödinger (Zurich,1925)Schrödinger Wave Equation

(1926)

http://www.zbp.univie.ac.at/schrodinger/lebensbilder/bilder9.htm

Age 38

Page 10: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

www.uni-leipzig.de/ ~gasse/gesch1.html

"So in one of the next colloquia, Schrödinger gave a beautifully clear account of how de Broglie associated a wave with a particle…When he had finished, Debye casually remarked that he thought this way of talking was rather childish… he had learned that, to deal properly with waves, one had to have a wave equation. It sounded rather trivial and did not seem to make a great impression, but Schrödinger evidently thought a bit more about the idea afterwards."

Felix Bloch, Physics Today (1976)

"Once at the end of a colloquium I heard Debye saying something like: Schrödinger, you are not working right now on very important problems anyway. Why don't you tell us sometime about that thesis of de Broglie?

Page 11: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

Well, I have found one."

"Just a few weeks later he gave another talk in the colloquium, which he started by saying: My colleague Debye suggested that one should have a wave equation:

H = E

Page 12: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

- Stockholm

PaulDirac

WernerHeisenberg

ErwinSchrödinger

AIP Emilio Segre Visual Archives, Peierls Collection

December 1933

Page 13: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

Schrödinger Equation

H = E ???

Page 14: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

Leipzig (1931)

AIP Emilio Segre Visual Archives, Peierls Collection

WernerHeisenberg

FelixBloch

1952 (NMR)

Page 15: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

Felix Bloch & Erich Hückel on Gar Manches rechnet Erwin schon Mit seiner Wellenfunktion.Nur wissen möcht man gerne wohl, Was man sich dabei vorstell'n soll.

Erwin with his Psi can do calculations, quite a few.We only wish that we could glean an inkling of what Psi could mean.

(1926)

Page 16: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

“etwa so wie Cervantes einmal den Sancho Panza, sein liebes Eselchen auf dem er zu reiten pflegte, verlieren läßt. Aber ein paar Kapitel später hat der Autor das vergessen und das gute Tier ist wieder da.

“Once Cervantes had Sancho Panza lose the well-loved little donkey he rode on. But a couple chapters later the author had forgotten and the good beast reappeared.

Ehrlich müßte ich darauf bekennen, ich weiß es sowenig, als ich weiß, wo Sancho Panzas zweites Eselchen hergekommen ist.

I must admit honestly, on this subject I know just as little, as I know where Sancho Panza’s second little donkey came from.

Nun werden sie mich vielleicht zuletzt fragen, ja was sind denn nun aber wirklich diese Korpuskeln, diese Atome - Moleküle.

Now you will perhaps in conclusion ask me, “So what are they then, I mean really, these corpuscles – these atoms – molecules?”

Schrödinger Lecture“What is Matter”

(1952)

by permission from Supposé CDErwin Schrödinger Was ist Materie?

Even Schrödinger was never comfortable with what really means:

Schrödinger’s GraveAlpbach, Austria

Wik

iped

ia

Page 17: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

First we’ll learn howto findand use it.

Later we learn what it means.

Page 18: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

of What?

Named by "quantum numbers"(e.g. n,l,m ; 1s ; 3dxy ;

Function of Particle Position(s)[and sometimes of time and "spin"]

We focus first on one particle, one dimension,then three dimensions (one atomic electron),

then atoms with several electrons,

then molecules and bonding,finally functional groups & reactivity

N particles 3N arguments![sometimes as many as 4N+1]

?

Function of

a Function

Page 19: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

Schrödinger Equation

H = E

(for “stationary” states)time-independent

( E times )(NOT H times )

Page 20: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

=

H = E

Kinetic Energy + Potential Energy = Total Energy

Given - Nothing to do with (Couloumb is just fine)

Hold your breath!

H = E

Page 21: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

Kinetic Energy?

Sum of classicalkinetic energy

over all particles of interest.

(adjusts for desired units)

mi vi2

i

Const 12 Fine for our great grandparents

Page 22: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

Kinetic Energy!2

xi2

2

yi2

2

zi2

+ +1mi

i

h2

82

d2

dx21

mC

C

Curvature of

m

One particle, One dimension:

Note:

Involves the shape of , not just its value.

Page 23: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

Solving a Quantum Problem

Given : a set of particlestheir masses & their potential energy law

[ e.g. 1 Particle/1 Dimension : 1 amu & Hooke's Law ]

Ta Function of the position(s) of the particle(s)Such that H/ is the same (E) everywhere

AND remains finite!!!(single-valued, continuous, 2 integrable)

Given :

To Find :

Page 24: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

What's Coming?1 Particle, 1 Dimension

Molecules & Bonds

Functional Groups & Reactivity

1-Electron Atoms (3 Dimensions)

Many Electrons & OrbitalsSept 25 Exam

Page 25: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

The Jeopardy ApproachAnswer

()

Problemmass and

Potential Energy(x)

= sin (x)

= sin (ax)

= ex

Kinetic Energy

= e-x

C/mIndependent of x

Const PE(particle in free space)

a2 C/mhigher kinetic energy’’

-C/m

-C/m

Const PE > TE

”Not just a mathematical curiosity.

Actually happens for all electrons bound to nuclei!

Negative kinetic energy!

C Curvature of

m

- sin (x)

sin (x)Cm

- a2 sin (ax)

sin (ax)Cm

( a > 1 shortened wave)

ex

ex

Cm

NOT your great grandparent’s 1/2 mv2.

(at large distance, where 1/r ceases changing much)

1 / 2

a = 3

E

0

V

Page 26: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

+

0

_

(x

)

x

Potential E

nergy

Total Energy• •

Curvingtoward = 0 Positive

Curving awayfrom = 0 Negative

Potential Energy from Arbitrary Shape

The potential energy function for this

must be a double minimum.

PositiveZero

Negative?

CurvatureAmplitude

via Kinetic Energy

Page 27: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

From “Jeopardy” Approachto Recipe for Solution of Schrödinger Equation

Using Guessed Total Energies

Page 28: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

Rearranging Schrödinger to give a formula for curve tracing.

C

Curvature of

m

+ V = E

CCurvature of

m

(V- E)=Curves away from 0 for V>E; toward 0 for V<E.

Since m, C, V(x) are given, this recipe allows tracing (x) in steps, from initial (0) [= 1], with initial slope [0], and a guessed E.

Page 29: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

100 kcal/mole

2.5Å0

Nodes and Quantizationin One Dimension

from Erwin Meets Goldilocks(for Wiki see Monday Problem Set)

Too Cold

Too Hot

Just Right!

20.74 kcal/moleGuess 21 kcal/mole

Guess 20 kcal/mole

DangerNegativeKineticEnergy

(Curve Away from Baseline)

DangerNegativeKineticEnergy

(Curve Away from Baseline)

Erwin Meets Goldilocks

Page 30: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

End of Lecture 7Sept 16, 2009

Copyright © J. M. McBride 2009. Some rights reserved. Except for cited third-party materials, and those used by visiting speakers, all content is licensed under a Creative Commons License (Attribution-NonCommercial-ShareAlike 3.0).

Use of this content constitutes your acceptance of the noted license and the terms and conditions of use.

Materials from Wikimedia Commons are denoted by the symbol .

Third party materials may be subject to additional intellectual property notices, information, or restrictions. 

The following attribution may be used when reusing material that is not identified as third-party content: J. M. McBride, Chem 125. License: Creative Commons BY-NC-SA 3.0

Page 31: After pointing out several discrepancies between electron difference density results and Lewis bonding theory, the course introduces quantum mechanics

100 kcal/mole

2.5Å0

20.74 kcal/mole

Erwin Meets Goldilocks

Could there be a lower-energy Psi?

4.15 kcal/mole

12.45 kcal/mole

Could there be an energy between?

NODES0 because of sign change

More Energy

More Curvature

More Nodes