Physics 2D Lecture Slides Oct 21 Vivek Sharma UCSD Physics - - PDF document

physics 2d lecture slides oct 21
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Physics 2D Lecture Slides Oct 21 Vivek Sharma UCSD Physics - - PDF document

Physics 2D Lecture Slides Oct 21 Vivek Sharma UCSD Physics Modern View of Photoelectric Effect = = + E hf KE Is h same in Photoelectric Effect as in BBQ Radiation? Slope h = 6.626 x 10 -34 JS Einstein Nobel Prize! No


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Physics 2D Lecture Slides Oct 21

Vivek Sharma UCSD Physics

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Modern View of Photoelectric Effect

E hf KE ϕ = = +

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Is “h” same in Photoelectric Effect as in BBQ Radiation?

Slope h = 6.626 x 10-34 JS Einstein Nobel Prize!

No matter where you travel in this galaxy and beyond… h = Planck’s constant is the

SAME !!!

NOBEL PRIZE FOR Herr PLANCK

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Work Function (Binding Energy) In Metals

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2 2

Light of Intensity I = 1.0 W/cm inc A Photoelectric Effect on An Iron Surfa ssume Fe reflects 96% of ligh ce: further on ident on ly 3% of 1.0cm surfa incident li ce of ght i i F t e s V µ

2

(a) Intensity available for Ph. El eff I =3

  • let region ( = 250nm)

barely above thres ect (b) how m hold frequency for Ph any photo-electrons e . El effec mitted per t # s % 4% (1.0 W/c econd ? m )

  • f

λ µ × ×

8

9 34 2 9

Power = h f hc (250 10 )(1.2 10 / ) = (6.6 10 )(3.0 1 p 3% 4 / ) hoto % (1.0 W/c electro m n ) s m J s J s m s µ λ

− − −

= × × × × × × i

10

  • 15

9 15 1

  • 19

9

= (c) Current in Ammeter : i = (1.6 10 )(1.5 10 ) (d) Work Function = ( )( ) 2.4 10 h 4.14 1 1.5 10 f 1.1 10 = 4.5 eV C A s eV s

− −

× × = Φ = × × × × i

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Photon & Relativity: Wave or a Particle ?

  • Photon associated with EM waves, travel with speed =c
  • For light (m =0) : Relativity says E2 = (pc)2 + (mc2)2
  • ⇒E = pc
  • But Planck tells us : E = hf = h (c/λ)
  • Put them together : hc /λ = pc

– ⇒

p = h/λ – Momentum of the photon (light) is inversely proportional to λ

  • But we associate λ with waves & p with

particles ….what is going on??

–A new paradigm of conversation with the subatomic particles : Quantum Physics

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X Rays : “Bremsstrahlung”: Braking Radiation

  • EM radiation, produced by bombarding a metal target with energetic electrons.
  • Produced in general by ALL decelerating charged particles
  • X rays : very short λ ≅ 60-100 pm (10-12m), large frequency f
  • Very penetrating because very energetic E = hf !!

Useful for probing structure of sub-atomic Particles (and your teeth)

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An X-ray Tube from 20th Century

The “High Energy Accelerator” of 1900s: produced energetic light : X Ray , gave new optic to subatomic phenomena Xray e

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X Ray Spectrum in Molybdenum (Mo)

  • Braking radiation predicted by Maxwell’s eqn
  • decelerated charged particle will radiate

continuously

  • Spikes in the spectrum are characteristic of the

nuclear structure of target material and varies between materials

  • Shown here are the α and β lines for

Molybdenum (Mo)

  • To measure the wavelength, diffraction grating

is too wide, need smaller slits

  • An atomic crystal lattice as diffraction

grating (Bragg)

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Interference of Waves: A Reminder

' max

Two Identical waves travel along +x and interefere to give a resulting wave y ( , ). The resulting wave form depends on relative phase differen ( , ) sin(

  • )

ce between 2 waves. Shown f

i i i i

y x t y t x x k t ω φ = + 2 = 0 r 3

  • , ,

φ π π ∆

Read Ch17-8 from Resnick etal held in Ereserve

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Bragg Scattering: Probing Atoms With X-Rays 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

X-ray detector

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Xray picture of a DNA Crystal

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Proteins inside Rhinovirus reconstructed by x-ray diffraction

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  • 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<< ∆

  • X rays allows one probe at atomic size (10-10)m
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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

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Compton Effect: what should Happen Classically?

  • Plane wave [f,λ] incident on

a surface with loosely bound electrons interaction of E field of EM wave with electron: F = eE

  • Electron oscillates with

f = fincident

  • Eventually radiates spherical

waves with fradiated= fincident

– At all scattering angles, ∆f & ∆λ must be zero

  • Time delay while the

electron gets a “tan” : soaks in radiation

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Compton Scattering : Setup & Results

( ' ) (1 cos ) Scattered ' larger than incident λ λ λ θ λ ∆ = − ∝ −

(1 cos )

e

h m c θ λ ⎛ ⎞ ⎟ − ⎠ ∆ ⎜ ⎝ =

How does one explain this startling anisotropy?

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Compton Effect : Quantum (Relativistic) Pool

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Compton Scattering: Quantum Picture

2 e e e

E+m ' p = p'cos +p cos p'sin -p sin Use these to e Energy Conservation: Momentum Conserv liminate electron deflection angle (n

  • t measured

: )

e

c E E θ φ θ φ = + =

e e e 2 2 2 2 4 2 e 2 2 e e 2

p 2 'cos p cos 'cos p sin 'sin Square and add Eliminate p & using E & E ( ') '

e e e e

p c m c E E m p p p E p pp p c φ θ φ θ θ = = − + + = = + − = − ⇒

( )

2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2 2

( ') ' 2 ' 2( ') ( ' ) ( 2 'cos ( ) E For light p= c ' ( ') 'cos E-E' 1 )(1 co ' ' ' 2 co (1 cos ) EE' s s )

e e e e

E E m c EE E E m c E E EE E mc p pp p E E E E E mc h E E c c c c m m c c θ θ θ θ λ λ θ ⇒ = ⇒ − + − = − ⇒ = − − ⇒ − + = + ⎡ ⎤ − + + ⎣ − + − − = − ⎦ ⎡ ⎤ − + ⎢ ⎥ ⎣ ⎦

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Checking for h in Compton Scattering

Plot scattered photon data, calculate slope and measure h

∆λ

1-cos ϑ

( ' ) ( )(1 cos )

e

h m c λ λ θ − = −

It’s the same h !!

C

  • m

p t

  • n

w a v e l e n g t h λC = h / me c

Energy Quantization is a UNIVERSAL characteristic

  • f light (EM Waves)
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touched the trunk of the elephant, said elephant was like a branch of a tree. touched the tail of the elephant, said elephant was like a snake. touched an ear. He said elephant was a huge fan. felt a leg of the elephant., elephant was like a pillar. touched the side of the elephant, said the elephant was like a wall Gentlemen, all five of you have touched only one part of the elephant ..elephant is all of above LIKEWISE WITH LIGHT ! Blindmen & an Elephant