6: biophysical and diffraction

0.0(0)
studied byStudied by 0 people
learnLearn
examPractice Test
spaced repetitionSpaced Repetition
heart puzzleMatch
flashcardsFlashcards
Card Sorting

1/62

encourage image

There's no tags or description

Looks like no tags are added yet.

Study Analytics
Name
Mastery
Learn
Test
Matching
Spaced

No study sessions yet.

63 Terms

1
New cards

describe spectroscopic vs diffraction methods

spectroscopy

  • rely on transition between energy levels

  • vary wavelength of radiation = absorption/emission occurs at given frequencies

  • sample (typically) in solution

diffraction

  • interaction with matter

  • keep wavelength fixed = measure variations in intensities with incident direction

  • sample in solid state

2
New cards

simply describe x-ray diffraction

x-rays = similar wavelength to the spacing between atoms in sample

x-rays are focused on sample. x-ray are reflected by electrons surrounding atoms of the sample, changing the direction by theta. these scattered x-rays constructively interfere to produce a diffraction pattern.

3
New cards

describe diffraction on different types of material

i.e. fibres, single crystals, powders

product different diffraction patterns = same theory applies to interpret them

4
New cards

what range are x-rays?

0.01 → 10 nm

~ distances between atoms

5
New cards

what kind of scattering is x-ray diffraction?

elastic

  • energy maintained

  • direction altered

6
New cards

describe the photoelectric effect

when a photon strikes an atom/molecule and transfers its energy to inner-shell electron.

if the photon has sufficient energy (≥ electron binding energy), the electron is ejected from its shell

ejected electron = photoelectron

7
New cards

describe the generation of x-rays

x-ray tube containing:

  • cathode (-ve) = source of electrons ~ tungsten

  • metal anode (+ve) = target ~ copper

  • vacuum

a current is passed through the cathode, which heats up and emits electrons. these electrons are accelerated through the vacuum to target, gaining kinetic energy. when electron hits the anode target, kinetic energy is converted to:

  • heat (major): anode must be cooled due to release of heat

  • x-rays (minor): if the incident electron has enough energy, it can knock out 1s electron from the K-shell (innermost electron shell) of the anode atom = ionisation. K-shell vacancy is filled from a higher energy shell (L-shell/M-shell), releasing energy in the form of an x-ray (photons with x-ray wavelength)

<p>x-ray tube containing:</p><ul><li><p>cathode (-ve) = source of electrons ~ tungsten</p></li><li><p>metal anode (+ve) = target ~ copper</p></li><li><p>vacuum</p></li></ul><p>a current is passed through the cathode, which heats up and emits electrons. these electrons are accelerated through the vacuum to target, gaining kinetic energy. when electron hits the anode target, kinetic energy is converted to:</p><ul><li><p>heat (major): anode must be cooled due to release of heat</p></li><li><p>x-rays (minor): if the incident electron has enough energy, it can knock out 1s electron from the K-shell (innermost electron shell) of the anode atom = ionisation. K-shell vacancy is filled from a higher energy shell (L-shell/M-shell), releasing energy in the form of an x-ray (photons with x-ray wavelength)</p></li></ul><p></p>
8
New cards

what are the two types of x-rays which can be produced by x-ray tubes?

  • characteristic x-rays

  • Bremsstrahlung radiation

<ul><li><p>characteristic x-rays</p></li><li><p>Bremsstrahlung radiation </p></li></ul><p></p>
9
New cards

what are characteristic x-rays?

x-rays produced by x-ray tube

= energy/wavelength is specific to size of X→K transition

= energy/wavelength is specific to anode element

10
New cards

what are the different shell labels?

K: n=1

L: n=2

M: n=3

11
New cards
<p>what gives rise to the different types of K radiation? </p>

what gives rise to the different types of K radiation?

due to SO coupling splitting the degenerate 2p/3p orbitals

= different size transitions

<p>due to SO coupling splitting the degenerate 2p/3p orbitals </p><p>= different size transitions </p>
12
New cards

describe Bremsstrahlung radiation

when electron decelerates rapidly as they interact with electric field of the nucleus, they can produce broad-spectrum X-rays that can vary in wavelength and are not specific to the anode element

13
New cards

what is the general equation for x-ray absorption? *not given*

I = intensity of radiation after passing through material

I(0) = intensity of incident radiation

µ = absorption coefficient of the material (dependent on material and X-ray wavelength)

t = path length 

<p>I = intensity of radiation after passing through material</p><p>I(0) = intensity of incident radiation</p><p>µ = absorption coefficient of the material (dependent on material and X-ray wavelength)</p><p>t = path length<span>&nbsp;</span></p>
14
New cards

describe filters

selectively remove unwanted x-ray radiation from spectrum, particular K(B)

K(B) = contributes to background noise/reduce image clarity

= have large absorption coefficients, µ, at certain wavelengths corresponding to K(B)

<p>selectively remove unwanted x-ray radiation from spectrum, particular K(B)</p><p>K(B) = contributes to background noise/reduce image clarity</p><p>= have large absorption coefficients, µ, at certain wavelengths corresponding to K(B)</p>
15
New cards

describe absorption edges

sudden increase in absorption of X-rays (absorption coefficient) above threshold energy to excite an electron from an inner atomic shell

<p>sudden increase in absorption of X-rays (absorption coefficient) above threshold energy to excite an electron from an inner atomic shell</p>
16
New cards

what are 3 types of x-ray interaction with material

  • Thompson scattering

  • Compton scattering

  • photoelectron absorption

17
New cards

describe scattering

the redirection of incoming radiation (photon in x-ray) due to interaction with matter (electrons in x-ray)

18
New cards

describe Thompson scattering

wave:

  • elastic scattering = no loss of energy

  • coherent scattering = no change in frequency/wavelength of photon = no energy transfer between photon and electron

  • wave is scattered in all directions = varying angles

electron:

no electron is ejected

<p>wave:</p><ul><li><p>elastic scattering = no loss of energy</p></li><li><p>coherent scattering = no change in frequency/wavelength of photon = no energy transfer between photon and electron</p></li><li><p>wave is scattered in all directions = varying angles</p></li></ul><p>electron:</p><p><strong>no electron is ejected</strong></p>
19
New cards

describe Compton scattering

wave:

  • inelastic scattering = loss of energy

  • incoherent scattering = decrease of frequency/increase in wavelength = energy transfer between photon and electron

  • wave is scattered in all direction = varying angles

electron:

outer shell (loosely bound) electron is ejected

<p>wave: </p><ul><li><p>inelastic scattering = loss of energy</p></li><li><p>incoherent scattering = decrease of frequency/increase in wavelength = energy transfer between photon and electron</p></li><li><p>wave is scattered in all direction = varying angles</p></li></ul><p>electron:</p><p><strong>outer shell (loosely bound) electron is ejected</strong></p>
20
New cards

describe photoelectron absorption

wave:

  • inelastic scattering = loss of energy

  • no scattering = complete energy transfer between photon and electron

  • no wave

electron:

inner shell electron is ejected = photoelectron

excess absorbed energy released as:

  • x-ray fluorescence (not scattered) = photoelectric effect

  • Auger electron = energy transferred to another electron and ejected

21
New cards

why are crystals used in x-ray diffraction?

electron scatter x-rays very weakly

= use ordered arrays of molecules

22
New cards

define structural units

structural unit = repeated by translation in 3 dimensions = all orientated identically

crystal lattice structure can be represented by structural units as single points

23
New cards

describe unit cell

smallest repeating unit of the lattice

 parallelepiped (6 parallelogram-faced structure) with:

  • three edges (a, b, and c i.e. x, y, and z)

  • three angles (a, B, and Y)

convention:

a < b

Y ~ 90°

contains 1 whole molecule in total

<p>smallest repeating unit of the lattice</p><p>&nbsp;parallelepiped (6 parallelogram-faced structure) with:</p><ul><li><p>three edges (a, b, and c i.e. x, y, and z)</p></li><li><p>three angles (a, B, and Y)</p></li></ul><p>convention:</p><p>a &lt; b</p><p>Y ~ 90°</p><p>contains 1 whole molecule in total </p>
24
New cards

what are the 14 distinct lattice types which symmetry operations yield?

Bravias lattices

25
New cards

what are the 7 crystal systems of Bravias lattices?

  • triclinic

  • monoclinic

  • orthorhombic

  • tetragonal

  • rhombohedral

  • hexagonal

  • cubic

26
New cards

what are the different labels within each crystal system?

P = primitive = only points in each corner

I = body-centred

F = centred in all 6 faces

C = centred on 2 opposite faces

<p>P = primitive = only points in each corner</p><p>I = body-centred</p><p>F = centred in all 6 faces</p><p>C = centred on 2 opposite faces</p>
27
New cards

define asymmetric unit

smallest section of the unit cell/crystal structure related by symmetry

28
New cards

summarise crystalline structure

asymmetric unit -(space group)→ unit cell → crystal

space group = symmetry operations which generate unit cell from asymmetric unit

<p>asymmetric unit -(space group)→ unit cell → crystal </p><p>space group = symmetry operations which generate unit cell from asymmetric unit</p>
29
New cards

what are 3 types of interference?

  • intermediate

  • constructive

  • destructive

30
New cards

describe constructive interference

  • waves in phase: phase difference = 0

  • total reinforcement

  • A = single wave + single wave = 2*single wave

<ul><li><p>waves in phase: phase difference = 0</p></li><li><p>total reinforcement</p></li><li><p>A = single wave + single wave = 2*single wave</p></li></ul><p></p>
31
New cards

describe destructive interference

  • waves out of phase: phase difference = λ/2 or 180°

  • complete cancellation

  • no resultant wave

<ul><li><p>waves out of phase: phase difference = <span>λ/2 or 180°</span></p></li><li><p>complete cancellation </p></li><li><p>no resultant wave </p></li></ul><p></p>
32
New cards

describe intermediate interference

  • waves partially in phase: i.e. phase difference = λ/4 or 90°

  • partial reinforcement

<ul><li><p>waves partially in phase: i.e. phase difference = λ/4 or 90°</p></li><li><p>partial reinforcement</p></li></ul><p></p>
33
New cards

what kind of interference is required for x-ray diffraction?

constructive interference

34
New cards

describe the features of a diffraction pattern

  • geometry

  • intensities

  • symmetry (of intensities)

<ul><li><p>geometry</p></li><li><p>intensities </p></li><li><p>symmetry (of intensities)</p></li></ul><p></p>
35
New cards

describe Braggs law

incident x-ray onto a crystal surface at angle θ will be reflected by different crystal ‘planes’ by angle θ.

when constructive interference of scattered x-rays occurs, the scattered x-rays are intense enough to be visible on the diffraction pattern.

when constructive interference does not occur, the scattered x-rays partially or completely destructively interfere.

Braggs law defines when constructive interference occurs

<p>incident x-ray onto a crystal surface at angle θ will be reflected by different crystal ‘planes’ by angle θ.</p><p>when constructive interference of scattered x-rays occurs, the scattered x-rays are intense enough to be visible on the diffraction pattern.</p><p>when constructive interference does not occur, the scattered x-rays partially or completely destructively interfere.</p><p>Braggs law defines when constructive interference occurs </p>
36
New cards

explain the derivation of Braggs law

constructive interferences will arise where the path difference is integer values of wavelength = Braggs law

<p>constructive interferences will arise where the path difference is integer values of wavelength = <strong>Braggs law</strong></p>
37
New cards

describe crystal planes

simple molecules = convenient

complex molecules = difficult to see how they arise

38
New cards

describe scattering from point

lattice points are used as reference rather than planes

d = distance between lattice points

39
New cards

describe first order vs higher order diffraction

first order: n=1: path difference = λ

higher order: n>1: path difference = 2λ, 3λ, etc.

40
New cards

how does the angle of diffraction vary for different orders of diffraction

higher order of diffraction = larger n = larger angle of diffraction

lower order of diffraction = smaller n = smaller angle of diffraction

<p>higher order of diffraction = larger n = larger angle of diffraction </p><p>lower order of diffraction = smaller n = smaller angle of diffraction </p>
41
New cards

describe the reciprocal lattice

inverse relationship between crystal lattice and lattice of reflections (diffraction pattern)

42
New cards

describe Miller indices

3 integers = h, k, l

= labels families of planes/points and reflection is corresponds to that give rise to diffraction spots due to constructive interference (also a label for the resulting reflection)

<p>3 integers = h, k, l</p><p>= labels families of planes/points and reflection is corresponds to that give rise to diffraction spots due to constructive interference (also a label for the resulting reflection)</p>
43
New cards

define the Laue equation *given*

used to determine d-spacing between planes/points of an given reflection

<p>used to determine d-spacing between planes/points of an given reflection</p>
44
New cards

what is the unit angstrom?

A = x10^-10 m

45
New cards

what controls the position vs intensity of diffraction pattern

position = d spacing and Bragg angle = arrangement of unit cells:

  • crystal structure

intensity = extent of constructive interference = arrangement within unit cells:

  • unit cell structure

46
New cards

describe the application of diffraction spot positions

can be used to determine the Bragg angle = used to determine d

  • crystal symmetry

  • unit cell dimensions

  • estimare molecules in asymmetric unit

47
New cards

define the structure factor, F, and its amplitude, |F|

F = mathematical function describing the amplitude and phase of a wave diffracted from crystal lattice planes characterised by Miller indices h,k,l.

|F| = strength/intensity of diffracted wave

48
New cards

describe the application of diffraction spot intensities

I(hkl) = intensity of diffraction spot ∝ extent of constructive interference

F(hkl) = structure factor for given (hkl) indices

| F(hkl) | = amplitude of the wave scattered by one unit cell at (hkl) indices

larger amplitude = more constructive interference

smaller amplitude = less constructive interference

hence, amplitude of scattered wave ∝ intensity of diffraction spot

<p>I(hkl) = intensity of diffraction spot ∝ extent of constructive interference</p><p>F(hkl) = structure factor for given (hkl) indices</p><p>| F(hkl) | = amplitude of the wave scattered by one unit cell at (hkl) indices</p><p>larger amplitude = more constructive interference</p><p>smaller amplitude = less constructive interference</p><p>hence, <strong>amplitude of scattered wave ∝ intensity of diffraction spot</strong></p>
49
New cards

describes waves represented as vectors

vector = F

amplitude = |F|

direction = φ

<p>vector = F</p><p>amplitude = |F|</p><p>direction = φ</p>
50
New cards

what equations define waves as vectors? *not given*

know the cos and sin

<p><strong>know the cos and sin</strong></p><p></p>
51
New cards

describe the phase problem

= phase information is lost during XRD

varying degrees of constructive interference between waves give rise to diffraction spots of varying intensities. the respective phases cannot be determined through the intensity of the diffraction spots.

there is no way to directly measure the phase (individual contribution to constructive interference) of the constituent waves

52
New cards

knowing the amplitude and phase of the initially scattered waves, how can the amplitude and phase of the final scattered wave be determined?

addition

find total A and total B

find total |F| and φ

53
New cards

describe structure factor vs structure factor amplitude

F = structure factor = complex

|F| = structure factor amplitude = not complex

<p>F = structure factor = complex</p><p>|F| = structure factor amplitude = not complex</p>
54
New cards

describe atomic scattering factor

= measure of scattering power of an isolated atom = unique to an atom

= f(Φ)

depends on:

  • scattering amplitude of an isolated atom

  • Bragg angle of scattering

55
New cards

describe f(Φ) when Φ=0 (forward direction)

all electron scatter x-rays exactly in phase = no path difference

all scattered waves combine constructively

maximum scattering

56
New cards

describe f(Φ) when Φ>0

partial destructive interference increases as Φ increases

= intensity falls of as Φ increases

<p>partial destructive interference increases as Φ increases</p><p>= intensity falls of as Φ increases </p>
57
New cards

describe the effect of temperature on f

increased T = increased vibrations = spread out electron density = increases interference effects = scattering factor (f) falls off faster

<p>increased T = increased vibrations = spread out electron density = increases interference effects = scattering factor (f) falls off faster </p>
58
New cards

what is U?

= isotropic displacement parameter

= describes how much an atom deviates from its ideal position within a crystal lattice due to thermal vibrations

∝ 1/f

<p>= isotropic displacement parameter</p><p>= describes how much an atom deviates from its ideal position within a crystal lattice due to thermal vibrations</p><p><span>∝ 1/f </span></p>
59
New cards
<p>define the structure factor equation </p>

define the structure factor equation

2, 3, 4 = sum of the scattered x-rays

5 = scattered waves from each atom have different relative phases in direction hkl which depends on positions of atoms

<p>2, 3, 4 = sum of the scattered x-rays</p><p>5 = scattered waves from each atom have different relative phases in direction hkl which depends on positions of atoms</p>
60
New cards

what is required to calculate structure factor, F?

  • chemical type (f)

  • position (xyz)

of each atom is known

61
New cards

describe the Fourier series

any periodic function can be described as a sum of simple series sin/cos functions

<p>any periodic function can be described as a sum of simple series sin/cos functions</p>
62
New cards

describe how the diffraction pattern is related to real space lattice

diffraction pattern → reciprocal lattice -(Fourier transform)→ real space lattice

63
New cards