quantum theory micro-world macro-world lecture 14

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Quantum Theory Micro-world Macro-world Lecture 14

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Page 1: Quantum Theory Micro-world Macro-world Lecture 14

Quantum Theory

Micro-world Macro-worldLecture 14

Page 2: Quantum Theory Micro-world Macro-world Lecture 14

Light propagates like a wave,& interacts as a particle

E=hf

hp =

Page 3: Quantum Theory Micro-world Macro-world Lecture 14

Louis deBroglie

If light behaves as particles, maybe other “particles” (such as electrons) behave as waves h

p = Photons:

hp =

particles:

hp =

Wave-particle duality is

a universal phenomenon

“deBroglie

wavelength”

Page 4: Quantum Theory Micro-world Macro-world Lecture 14

Ordinary-sized objects have tiny wavelengths

0.2kg30m/s

hp =

hmv

= 6.6x10-34Js

0.2kg x 30 m/s =

6.6x10-34Js6.0 kg m/s = 1.1x10-34m =

Incredibly small

Page 5: Quantum Theory Micro-world Macro-world Lecture 14

the wavelength of an electronis not so small

9x10-31 kg 6x106 m/s

hp =

hmv

= 6.6x10-34Js

9x10-31kg x 6x106 m/s =

6.6x10-34Js5.4x10-24 kg m/s = 1.2x10-10m =

-

About the size of an atom

Page 6: Quantum Theory Micro-world Macro-world Lecture 14

Send low-momentum electrons thru narrow slits

See a diffraction pattern characteristic of

wavelength =h/p as predicted by de Broglie

Page 7: Quantum Theory Micro-world Macro-world Lecture 14

or through a small hole

“Diffraction”rings

Page 8: Quantum Theory Micro-world Macro-world Lecture 14

Matter waves(electrons through a crystal)

“Diffraction”rings

Page 9: Quantum Theory Micro-world Macro-world Lecture 14

Electron waves through a narrow slit acquire some py

py

py

y

x

y

Page 10: Quantum Theory Micro-world Macro-world Lecture 14

Waves thru a narrower slit

wider

py

py

y

When the slit becomes narrower, thespread in vertical momentum increases

x

y

Page 11: Quantum Theory Micro-world Macro-world Lecture 14

y/2

x

y

/2

hyp

hyp

yp

h

yph

y

y

sin2

2sin

Page 12: Quantum Theory Micro-world Macro-world Lecture 14

Heisenberg Uncertainty Principle

y py > h

Uncertaintyin location

Uncertainty in

momentum in

that direction

If you make one of these smaller, the other has to become bigger

Page 13: Quantum Theory Micro-world Macro-world Lecture 14

Heisenberg tries to measure the location of an atom

For better precision, usea shorter wavelength

But then the momentumchange is higher

x px > h

Page 14: Quantum Theory Micro-world Macro-world Lecture 14

Localize a baseball

0.2kg x px > h px > hx

Suppose x= 1x10-10m

px > 6.6x10-34Js

1x10-10m

vx >

= 6.6x10-24kgm/s

A very tiny uncertainty

About the size of a single atom

px m

6.6x10-44Js

0.2kg = = 3.3x10-23 m/s

Page 15: Quantum Theory Micro-world Macro-world Lecture 14

Localize an electron

x px > h px > hx

Suppose x= 1x10-10m

px > 6.6x10-34Js

1x10-10m

vx >

= 6.6x10-24kgm/s

Huge, about 2% of c

About the size of a single atom

px me

6.6x10-24Js

9x10-31kg = = 7x106 m/s

-me=9x10-31kg

Page 16: Quantum Theory Micro-world Macro-world Lecture 14

uncertainty is inherentin the quantum world

Page 17: Quantum Theory Micro-world Macro-world Lecture 14

The Bohr-Rutherford Atom

Physics 100

Chapt 23

Nils Bohr

Ernest Rutherford

Page 18: Quantum Theory Micro-world Macro-world Lecture 14

1895 J.J. Thomson discovered electron

+-

- -

-

+ +

+ +

cathode

anode

“cathode rays”

Vacuum flask

Page 19: Quantum Theory Micro-world Macro-world Lecture 14

Cathode rays have negative chargeand very small mass

+-

- -

-

+ +

+ +

cathode

anode N

S

m=0.0005MHydrogen

Page 20: Quantum Theory Micro-world Macro-world Lecture 14

Plum pudding?

-

-

--

-

--

-

-

10-10m

+

+

+

+

+

+

+

+

+

+

++

+

+

+

+

Positively chargedporridge

Negatively chargedraisins (plums)

Page 21: Quantum Theory Micro-world Macro-world Lecture 14

Planetary-like?

10-10m

+

-

-

-

-

-

Positively chargeddense central nucleus

Negatively chargedorbiting electrons

Page 22: Quantum Theory Micro-world Macro-world Lecture 14

Rutherford Experiment

Vacuumflask

-rays

Page 23: Quantum Theory Micro-world Macro-world Lecture 14

What’s in the box?

Is all the mass spreadthroughout as in a box

of marshmallows”?

or is all the massconcentrated in a dense

“ball-bearing”?

Page 24: Quantum Theory Micro-world Macro-world Lecture 14

Figure it out without opening (or shaking)

Shoot bullets randomly through the box. If it is filled with marshmallows, all the bullets will go straight through without (much) deflection

Page 25: Quantum Theory Micro-world Macro-world Lecture 14

Figure it out without opening (or shaking)

If it contains a ball-bearing most the bullets will go straight through without deflection---but not all

Occasionally, a bullet will collide nearly head-on to the ball-bearing and be deflected by a large angle

Page 26: Quantum Theory Micro-world Macro-world Lecture 14

Rutherford used -ray “bullets” to distinguish between the plum-pudding & planetary models

-

-

--

-

--

-

-

+

+

+

+

+

+

+

+

+

+

++

+

+

+

+

no way for -rays to scatter at wide angles

Plum-pudding:

Page 27: Quantum Theory Micro-world Macro-world Lecture 14

+

-

-

-

-

-

Occasionally, an-rays will be pointed head-on to a nucleus & will scatter at a wide angle

distinguishing between the plum-pudding & planetary models

Page 28: Quantum Theory Micro-world Macro-world Lecture 14

Rutherford saw ~1/10,000a-rays scatter at wide angles

+

-

-

-

-

-

from this he inferred a nuclearsize of about 10-14m

Page 29: Quantum Theory Micro-world Macro-world Lecture 14

Rutherford atom

+10-14m

10-10m

Not to scale!!!If it were to scale,the nucleus wouldbe too small to seeEven though it has more than 99.9% of the atom’s mass

Page 30: Quantum Theory Micro-world Macro-world Lecture 14

Relative scalesAloha stadium

Golf ball

AtomNucleus

99.97% of the mass

x10-4

Page 31: Quantum Theory Micro-world Macro-world Lecture 14

Classical theory had trouble with Rutherford’s atom

Orbiting electrons are accelerating

Accelerating electrons should radiate light

According to Maxwell’stheory, a Rutherford

atom would only survivefor only about 10-12 secs

Page 32: Quantum Theory Micro-world Macro-world Lecture 14

Fraunhofer discovered that some wavelengths aremissing from the sun’s black-body spectrum

sola

Other peculiar discoveries:

Solar light spectrum:

Page 33: Quantum Theory Micro-world Macro-world Lecture 14

Other discoveries…Low pressure gasses, when heated,

do not radiate black-body-like spectra;instead they radiate only a few specific colors

Page 34: Quantum Theory Micro-world Macro-world Lecture 14

bright colors from hydrogen match the missing colors in sunlight

Hydrogen spectrum

Solar spectrum

Page 35: Quantum Theory Micro-world Macro-world Lecture 14

Bohr’s idea

“Allowed”orbits

Page 36: Quantum Theory Micro-world Macro-world Lecture 14

Hydrogen energy levels

+1

3

4

Page 37: Quantum Theory Micro-world Macro-world Lecture 14

Hydrogen energy levels

+

1

2

Page 38: Quantum Theory Micro-world Macro-world Lecture 14

What makes Bohr’s allowed energy levels allowed?

Recall what happens when we force waves into confined spaces:

Page 39: Quantum Theory Micro-world Macro-world Lecture 14

Confined waves

Only waves with wavelengths that just fit in survive(all others cancel themselves out)

Page 40: Quantum Theory Micro-world Macro-world Lecture 14

Electrons in atoms are confined matter waves ala deBroglie

This wave, as it goes around, will interferewith itself destructively and cancel itself out

However, if the circumference is exactly an integer number of wavelengths, successive

turns will interfere constructively

Bohr’s allowed energy states correspond to thosewith orbits that are integer numbers of wavelengths

Page 41: Quantum Theory Micro-world Macro-world Lecture 14

Bohr orbits

Page 42: Quantum Theory Micro-world Macro-world Lecture 14

Bohr orbits

Page 43: Quantum Theory Micro-world Macro-world Lecture 14

Quantum Mechanics

Erwin Schrodinger

Schrodinger’s equation

ExV

dx

d

m )(

2 2

222h

Page 44: Quantum Theory Micro-world Macro-world Lecture 14

Matter waves are “probability” waves

Probability to detect theelectron at some place

is 2 at that spot

Electrons are most likely

to be detected hereor here

Electrons will never be detected here

Page 45: Quantum Theory Micro-world Macro-world Lecture 14

Electron “clouds” in Hydrogen

Page 46: Quantum Theory Micro-world Macro-world Lecture 14

Nobel prizes for Quantum Theory

1918 Max Planck E=hf1921 Albert Einstein photons1922 Niels Bohr atomic orbits1929 Louis de Broglie matter waves1932 Werner Heisenberg uncertainty principle…