Physics 2D Lecture Slides
Lecture 13
Feb.6, 2008
• X rays are EM waves of low wavelength, high
frequency (and energy) and demonstrate
characteristic features of a wave
– Interference
– Diffraction
• To probe into a structure you need a light source
with wavelength much smaller than the features of
the object being probed
– Good Resolution  λ<< Δ
• X rays allows one probe at atomic size (10-10)m
Compton Scattering : Quantum
Pool !
•
1922: Arthur Compton (USA) proves that X-rays (EM Waves)
have particle like properties (acts like photons)
– Showed that classical theory failed to explain the scattering effect
of
• X rays on to free (not bound, barely bound electrons)
•
Experiment : shine X ray EM waves on to a surface with “almost”
free electrons
– Watch the scattering of light off electron : measure time +
wavelength of scattered X-ray
Compton Scattering : Setup & Results
Δλ = (λ '− λ ) ∝ (1 − cos θ )
Scattered λ ' larger than incident
Compton Scattering Observations
Compton Scattering : Summary of Observations
Δλ = (λ -λ ) ∝ (1 − cos θ ) !
Not isotropy in distribution of
scattered radiation
'
How does one explain this startling anisotropy?
Compton Scattering: The Quantum Picture
Energy Conservation:
E+m e c 2 = E '+ Ee
Momentum Conserv:
p = p'cosθ +p e cos φ
0 = p'sinθ -p e sin φ
((E − E ') + m c )
2
e
2
= ⎡⎣ p 2 − 2 pp 'cosθ + p '2 ⎤⎦ c 2 + (me c 2 )2
E
For light p= ⇒
c
Use these to eliminate
electron deflection
angle (not measured)
2
2
⎡
⎤ 2
E
EE
'
E
'
2
2
2
E + E ' − 2EE '+ 2(E − E ')mc = ⎢ 2 − 2 2 cosθ + 2 ⎥ c
c
c ⎦
⎣c
⇒ − EE '+ (E − E ')mc 2 = − EE 'cosθ
⇒
E-E'
1
h
=
(1
−
cos
θ
)
⇒
(
λ
'−
λ
)
=
(
)(1 − cosθ )
2
EE' me c
me c
Rules of Quantum Pool between Photon and Electron
h
(λ '− λ ) = (
)(1 − cos θ )
me c
Checking for h in Compton Scattering
It’s the same value for h again !!
Plot scattered photon data, calculate slope and measure “h”
Δλ
(λ '− λ ) = (
h
)(1 − cos θ )
me c
Energy Quantization is a
UNIVERSAL characteristic
of energy transactions !
1-cos ϑ
Interference of Waves: A Reminder
Two Identical waves yi ( x, t ) = ymax sin(ki x - ωi t + φi ) travel along +x and interefere
to give a resulting wave y ' ( x, t ). The resulting wave form depends on relative phase difference
2
Read Ch17-8 from Resnick et
between 2 waves. Shown for Δφ = 0, π , π
3
al
An X-ray Tube from 20th Century
e
Xray
The “High Energy Accelerator” of 1900s: produced energetic light : X
Ray , gave new optic to subatomic phenomena
Modern Synchrotron ----World’s most powerful
Modern Synchrotron -- World’s most powerful source of X-ray Beams
X-Ray Scattering Studies of
Thin Polymer Films
Bragg Scattering
photographic film
Bragg Scattering: Probing Atoms
With X-Rays
X-ray
detector
Constructive Interference when net phase difference is 0, 2π etc
This implied path difference traveled by two waves must be integral
multiple of wavelength : nλ=2dsinϑ
Example : X-Ray Picture of a DNA Crystal and Discovery of
DNA Structure
!
Proteins inside Rhinovirus reconstructed by x-ray diffraction
Other forms of Interaction of Energy Exchange between Radiation and Matter
E
mc 2 +mc 2
Always same form of
Matter & Antimatter
Saw what light does, Now examine nature
of matter
• Fundamental Characteristics of different forms of matter
– Rest Mass (m)
– Electric Charge (q)
• Measurable
– using some combination of E & B fields interacting with the
particle
F = q ( E + v x B)
– Or E/B or some other macroscopic force
e.g. Drag Force
The “magic” is that one is measuring tiny tiny numbers using Macroscopic
devices
Thomson’s Determination of e/m
of the Electron
• In E Field alone, electron lands at D
• In B field alone, electron lands at E
• When E and B field adjusted to cancel
each other’s force  electron lands at F
 e/m = 1.7588 x 1011 C/Kg
Millikan’s Measurement of Electron
Charge
Find charge on oil drop is always in integral multiple of some Q
qe = 1.688 x 10-19 Coulombs
 me = 9.1093 x 10-31 Kg
 Fundamental properties (finger print) of electron
(similarly can measure proton properties etc)
Summary : From X Ray (EM
Wave) Scattering data, Size of
the Atom was known to be about
10-10 m
Where are the electrons inside the atom?
Early Thought: “Plum pudding” model: Atom has a homogenous distribution of
Positive charge with electrons embedded in them
(atom is neutral)
Positively charged
ematter
e
e e
ee- e
e- e- e- e-
e-
or
ee-
e-
ee-
e-
e-
+ Core
+
?
• How to test these hypotheses?  Shoot “bullets” at the atom and
watch their trajectory. What Kind of bullets ?
•Indestructible charged bullets  Ionized He++ atom = α++ particles
•Q = +2e , Mass Mα=4amu >> me , Vα= 2 x 10 7 m/s (non-relavistic)
[charged to probe charge & mass distribution inside atom]
Plum Pudding Model of Atom
•
•
•
•
•
Non-relativistic mechanics (Va/c = 0.1)
In Plum-pudding model, a-rays hardly scatter because
Positive charge distributed over size of atom (10-10m)
Ma >> Me (like moving truck hits a bicycle)
à predict a-rays will pass thru array of atoms with little scatter
(~1o)
Need to test this hypothesis  Ernest Rutherford
Probing Within an Atom with a Particles
•
Most α particles pass thru gold foil with nary a deflection
•
•
SOME (≅10-4) scatter at LARGE angles Φ
Even fewer scatter almost backwards  Why
“Rutherford Scattering” discovered by his
PhD Student (Marsden)
Rutherford Discovers Nucleus
(Nobel Prize)
Force on α-particle due to heavy Nucleus
α particle trajectory is hyperbolic
Scattering angle is related to impact par.
•Outside radius r =R, F ∝ Q/r2
•Inside radius r < R, F ∝ q/r2 = Qr/R2
•Maximum force at radius r = R
⎛ kqα Q ⎞ ⎛
θ⎞
Impact Parameter b = ⎜
cot ⎟
2 ⎟⎜
2⎠
⎝ mα vα ⎠ ⎝
Δn =
k 2 Z 2 e 4 NnA
2
⎛1
2 ⎞
4 R ⎜ mα vα ⎟ Sin 4 (ϕ / 2)
⎝2
⎠
2
•# scattered Vs φ depends on :
•n = # of incident alpha particles
•N = # of nuclei/area of foil
•Ze = Nuclear charge
• Kα of incident alpha beam
•A= detector area
Rutherford Scattering & Size of Nucleus
nucleus
distance of closest appoach ∝ r size of nucleus
1
Kinetic energy of α = Kα = mα vβ2
2
α particle will penetrate thru a radius r
until all its kinetic energy is used up to do
work AGAINST the Coulomb potential of
the Nucleus:
Kα =
⇒
(Ze )(2e )
1
mα vβ2 = 8MeV = k
2
r
2kZe 2
r=
Kα
For Kα =7.7.MeV, Z
⇒
nucleus
Al
= 13
2kZe 2
r=
= 4.9 ×10−15 m
Kα
Size of Nucleus = 10-15 m
Size of Atom = 10-10 m
Dimension Matters !
-15
Size of Nucleus = 10 m
-10
Size of Atom = 10 m
•how are the electrons located inside an atom
•How are they held in a stable fashion
•necessary condition for us to exist !
•All these discoveries will require new experiments and observations
Rutherford Atom & Classical
Physics
?
Continuous & Discrete spectra of
Elements
Visible Spectrum of Sun Through
a Prism
Emission & Absorption Line
Spectra of Elements
Kirchhoff’ Experiment : “D” Lines in Na
D lines darken noticeably when Sodium vapor introduced
Between slit and prism
Emission & Absorption Line Spectrum of Elements
•Emission line appear dark
because of photographic
exposure
Absorption spectrum of Na
While light passed thru Na vapor
is absorbed at specific λ
Atom: The Classical disaster