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Interference and DiffractionPowerPoint Presentation

Interference and Diffraction

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Two oscillators or two sources

To point P

d

dsin

Phase difference when arriving at P is

Original phase difference

phase from path difference

n equally spaced oscillators; equal amplitude; different

in phase (different starting phase, different path length)

E.g.

C

2

Plane

wave

1

n slits

equally spaced

A

B

a

E

D

Huygen’s

wavelets

What is the result of the sum?

n = 6

n = 6

C

2

1

A

B

a

….

….

E

D

Huygen’s

wavelets

Phase difference

Phase difference

….

….

1st Constructive Interference:

2nd Constructive Interference:

In general, constructive Interference:

I0

Width: W10 < W5 ; Height: n2; Integrated intensity?

a pair of wavelets

from the top and

center of the slit

}

0

d/2

C

B

d

next pair

x = 0 and x = d/2; path difference BC = dsin/2.

phase difference = (2/)*dsin/2 = dsin/

Destructive interference: dsin/ = , 2, 3, …= n.

dsin = n.

Resolution of single slit and circular aperture:

The Rayleigh Criterion

Well Resolved

Barely Resolved

http://www.kshitij-pmt.com/resolution-of-single-slit-and-circular-apertures

If d is very small, upper cap is more flat! a equals to a lot d!

1a’, 2a’

X

Y

1

1’

1a

2’

2

Plane normal

3

3’

2a

X’

Y’

K

P

M

N

d

L

S

2

Phase difference between different atoms interacted with X-ray.

Atoms in neighboring plane: 2dsin

Laue’s Equations:

a

0

acos0

acos

Integer

Constructive interference: |acos-acos0| = h

Similarly in the y direction: |bcos - bcos0| = k

Similarly in the y direction: |ccos - ccos0| = l

Reciprocal lattice and diffraction:

S

S0

OA= pa1+qa2+ra3

p, q, r:integers

S-S0

O

m

n

-S

Path difference:

uA + Av = Om+On

= S0OA + (-S) OA = (S0-S)OA.

v

u

A

b1, b2, b3: base vectors of G

If

constructive interference

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