nuclear materials midterm

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105 Terms

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Materials

metals

ceramics

polymers /plastics

composites

nuclear materials

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metals

strong & ductile

high thermal and electrical conductivity

opaque & reflective

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ductile meaning

-material can be stretched/deformed without breaking

-ability to undergo plastic deformation (permanent) without breaking

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opaque meaning

light does not pass through the material (not see-through)

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ceramics

ionic bonding (refactory)

oxides, carbides, nitrides, silfides

brittle, glassy, elastic

non-conducting (insulators)


examples: building brick, glass vase, a teacup

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ionic bonding

bonding of oppositely charged ions

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refactory meaning

refactory = heat resistant

material is able to withstand very high temps without melting or breaking down

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brittle meaning

material breaks with little deformation

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elastic

returns to its original shape after deformation

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polymers / plastics

covalent bonding

soft, ductile, low strength, low density

thermal & electrical insulators

translucent or transparent (see-through)

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covalent bonding

sharing of electrons between atoms

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insulators

does not conduct heat or electricity very easily

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composite materials

materials composed of two or more individual materials (metals + polymers + ceramics)

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composite purpose

to achieve a combination of properties that a single material cannot provide and combine the best characteristics of its components

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naturally occurring composites

wood and bone

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composite materials Examples

fiberglass & CFRP (carbon fiber-reinforced polymer)


fiberglass: glass fiber + polymer (epoxy) = strong, stiff, and flexible

CFRP: carbon fiber + polymer (epoxy) = Stronger and stiffer but expensive

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stiff meaning

resists deformation

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what does the nuclear reactor do?

nuclear reactions produce a large amount of thermal energy through fission CHAIN REACTIONS


nuclear reactors are simply heat-generating units

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nuclear reactor process

reactor —> heat —>(produces steam)—> turbine rotates —> generator rotates —> electricity

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what is the purpose of steam

steam is needed to rotate the turbines

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what is the purpose of turbines

to rotate electrical generators which produces electricity

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nuclear reactor primary loop

reactor side

contains components responsible for generating and managing heat


components:

-fuel: material where nuclear fission occurs

-neutron source

-moderator: slows down neutrons

-reflector: redirects escaping neutrons towards reactor

-control rods: controls the chain reaction

-coolant: removes heat

-shield: protection from radiation

-supporting structure

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nuclear reactor secondary loop

power generation side

contains components responsible for converting heat into electrical power


components:

-heat exchanger: transfers heat between fluids

-turbines

-electrical generators

-condenser: converts steam back into liquid water

-cooling tower

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material selection

general consideration

-Fabricability

-dimensional stability

-corrosion resistance

-design

-heat transfer

-availability and cost

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fabricability

a) definition

b) why is it important?

a) how easily the material can be made into the required shape/component (forming, welding, machining)


b) if fabricability issues are not dealt with during the first stage, it may cause problems at later stages.

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dimensional stability definition

the material should keep its shape and properties over time, especially at high temperatures

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corrosion resistance definition

corrosion: electrochemical process that causes metals/alloys to degrade in a chemical environment

corrosion resistance: the ability to resist corrosion degradation

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design definition

components designs’ should avoid stress concentration shapes such as sharp corners or holes.

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heat transfer definition

in a reactor, heat must move safely from the fuel through the cladding


high thermal conductivity is important

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material selection

special consideration

-neutronic properties

-susceptibility to induced radioactivity

-radiation stability

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neutronic properties

how the material interacts with neutrons


fuel cladding materials should have low neutron absorption cross section - so that is why zirconium alloys are used in LWR (light water reactor)


control materials need high neutron absorption to control the chain reaction

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susceptibility to induced radioactivity

when some materials absorb neutrons, they become radioactive themselves. which produces radioactive isotopes that can emit alpha, beta, or gamma radiation.

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radiation stability

how well a material withstands radiation damage


fast neutrons can displace atoms from their positions, creating defects inside the material.

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fuel cladding

material that surrounds and contains the nuclear fuel


zirconium-based materials are suitable for fuel cladding in LWR

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advantages of zirconium-based materials for fuel cladding

low neutron absorption cross section

corrosion resistance

thermal conductivity

high melting point

high-temp strength

ductility

fuel compatibility

fabricability

abundance

cost

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semiconductors

material whose electrical properties are intermediate between conductors and insulators

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doping

adding impure atoms to a semiconductor


adding even a tiny amount of another element to a semiconductor can greatly change how well it conducts electricity

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types of doped semiconductors

-N-type (extra electrons)

example: Si doped with phosphorus (P) leaves one extra electron which conducts more electricity


-P-type (missing electrons=creates holes)

example: Si doped with boron (B) leaves us with one electron missing which creates a hole.

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semiconductors advantages

reliability

compactness

low cost

controlled electrical conduction

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applications of semiconductors

transistors

diodes

photosensors

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superconductors

allows current to flow unimpeded (without being opposed/obstructed)


has zero electrical resistance

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biomaterials

materials used in components which are implanted into the human body to replace diseased/damaged body parts


must be non-toxic and biocompatible (compatible with body tissues and doesn’t cause opposing biological reactions)

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biomaterials materials

metals

ceramics

polymers

composites

semiconductors

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crystalline materials

materials whose atoms are arranged in a regular, repeating three-dimensional pattern over large atomic distances.


this is called long-range order


examples: metals, many ceramics, some polymers

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noncrystalline materials

also called amorphus


materials whose atoms dont have a periodic arrangement over large distances


noncrystalline arrangements can occur in complex structures or with rapid cooling

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unit cell

the basic repeating block of a a crystal structure

<p>the basic repeating block of a a crystal structure </p>
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lattice

a periodic arrangement of points in 3D space

<p>a periodic arrangement of points in 3D space</p>
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basis

atom or group of atoms associated with each lattice point

<p>atom or group of atoms associated with each lattice point</p>
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crystal structure

the way atoms are arranged in a space


lattice + basis = crystal structure

<p>the way atoms are arranged in a space</p><p></p><p>lattice + basis = crystal structure</p>
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crystal system

crystal system classifies lattice geometry (edge lengths: a,b,c) and symmetry (angles: alpha, beta, gamma)

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primative unit cell

contains one lattice point

<p>contains one lattice point</p>
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non-primative unit cell

contains more than one lattice point

<p>contains more than one lattice point</p>
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SC

simple cubic

-atoms at the 8 corners

-1 atom per unit cell (N=1)

-coordination number = 6

-a = 2R

-APF=0.52

<p><strong>simple cubic</strong></p><p>-atoms at the 8 corners</p><p>-1 atom per unit cell (N=1)</p><p>-coordination number = 6</p><p>-a = 2R</p><p>-APF=0.52</p>
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SC

simple cubic

-atoms at the 8 corners

-1 atom per unit cell (N=1)

-coordination number = 6

-a = 2R

-APF=0.52

<p><strong>simple cubic</strong></p><p>-atoms at the 8 corners</p><p>-1 atom per unit cell (N=1)</p><p>-coordination number = 6</p><p>-a = 2R</p><p>-APF=0.52</p>
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BCC

body-centered cubic

-atoms at the 8 corners + 1 body center

-2 atom per unit cell (N=2)

-coordination number = 8

-a = 4R/root(3)

-APF=0.68

<p><strong>body-centered cubic</strong></p><p>-atoms at the 8 corners + 1 body center</p><p>-2 atom per unit cell (N=2)</p><p>-coordination number = 8</p><p>-a = 4R/root(3)</p><p>-APF=0.68</p>
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FCC

Face-centered cubic

-atoms at the 8 corners + 6 face centers

-4 atom per unit cell (N=4)

-coordination number = 12

-a = 2root(2)R

-APF=0.74

<p><strong>Face-centered cubic</strong></p><p>-atoms at the 8 corners + 6 face centers</p><p>-4 atom per unit cell (N=4)</p><p>-coordination number = 12</p><p>-a = 2root(2)R</p><p>-APF=0.74</p>
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how to count atoms (N)

corner atomic position —> 1/8


face center —> ½
body center —> 1

<p>corner atomic position —&gt; 1/8</p><p></p><p>face center —&gt; ½ <br>body center —&gt; 1</p>
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coordination number

number of nearest-neighbor atoms surrounding a given atom

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drawing FCC

1- draw a cube

2- put one atom at each of the eight corners

3- put one atom at the center of each of the six faces, including the hidden faces

<p>1- draw a cube</p><p>2- put one atom at each of the eight corners</p><p>3- put one atom at the center of each of the six faces, including the hidden faces</p>
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which of the three structures (SC, FCC, BCC) is the most efficient

FCC has the highest atomic packing factor of the three structures

so its atoms are packed most efficiently

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HCP

hexagonal close-packed structure

-atoms at the 12 corners + 2 face centers + 3 body centers

(N = 12×1/6 + 2×1/2 + 3) = 6

-6 atoms per unit cell (N=6)

-coordination number = 12

-APF=0.74

<p><strong>hexagonal close-packed structure</strong></p><p>-atoms at the 12 corners + 2 face centers + 3 body centers</p><p>(N = 12×1/6 + 2×1/2 + 3) = 6</p><p>-6 atoms per unit cell (N=6)</p><p>-coordination number = 12</p><p>-APF=0.74</p>
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Diamond

N=8

coordination number = 4

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HCP stacking sequence

ABABAB…

<p>ABABAB…</p>
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miller indices

miller indices are used to identify crystallographic directions and planes in a crystal

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miller indices notations

(x, y , z) — coordinates of a point

[uvw] — one crystal direction

〈uvw〉 — family of equivalent directions

(hkl) — one crystal plane

{hkl} — family of equivalent planes

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family of directions

directions that are equivalent due to crystal symmetry


example:

in a cubic crystal: [100], [010], and [001] belong to the same family — 〈100〉

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how to calculate miller indices for directions

  1. identify the starting point (tail) and the ending point (head)

  2. subtract head by tail (head-tail)

  3. if necessary, convert coordinates to unit-cell length by dividing x by a, y by b, and z by c.

  4. if we have a fraction, divide all components by the same number to get the smallest whole number.

  5. if we have a negative number, replace the negative symbol with a bar (line) above it in the final answer

  6. write the results in square brackets [uvw]


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what if direction doesnt pass through the origin (0, 0, 0)

draw a straight line through the origin


two parallel arrows pointing the same way have the same direction indices. meaning translating an arrow without rotating, doesnt change its direction.

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Bragg’s law

n: order of reflection

Lamda: x-ray wavelength

d: distance between parallel crystal planes

Theta: angle between x-ray beam and crystal plane

<p>n: order of reflection</p><p>Lamda: x-ray wavelength</p><p>d: distance between parallel crystal planes</p><p>Theta: angle between x-ray beam and crystal plane</p>
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What causes constructive interference

Path difference equals an integer number of wavelengths

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BBC reflection rule

h+k+l must be even

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FFC reflection rule

h, k, l must all be odd or all even

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Crystal defects

An irregularity or imperfections in the normal crystal lattice


Some defects help improve material properties

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Defect types

Point defects

Line defects

Interfacial defects

Volume (bulk) defects

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Line defects

1D


Examples:

Dislocations (edge, screw, mixed)

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Line defects

1D


Examples:

Dislocations (edge, screw, mixed)

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Interfacial defects

2D


Examples:

Grain boundaries, phase boundaries

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Volume defects

3D


Examples:

Cavities, voids, precipitates

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Vacancy

An unoccupied lattice site where an atom should normally exist


Vacancies increase entropy which can lower free energy of the crystal

<p>An unoccupied lattice site where an atom should normally exist</p><p></p><p>Vacancies increase entropy which can lower free energy of the crystal</p>
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Self insistial

A host atom occupies an interstitial space instead of a normal lattice site


Self interstitials produce large lattice distortions because the atom is crowded into a small space

<p>A host atom occupies an interstitial space instead of a normal lattice site</p><p></p><p>Self interstitials produce large lattice distortions because the atom is crowded into a small space</p>
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Divacancy and binding energy

A pair if neighboring vacancies


BE: the energy required to separate a divacancy into two isolated vacancies

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<p>Frenkel defects</p>

Frenkel defects

An ion moves from its normal position into an interstitial site, creating a vacancy-interstitial pair


-vacancy + interstitial

Volume, mass, density = unchanged


Important for ionic crystals and nuclear materials exposed to radiation damage

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Schottky defect

A positive ion (cation) and a negative (anion) leave their lattice sites, creating paired vacancies


-two vacancies = mass+volume increase = density decreases

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Frenkel and schottky defect

Both defects preserve electrical neutrality

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Temperature effect on vacancy

As temp increases, vacancy concentration increases

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Vacancy concentration formula

N(v): number of vacancies

N: number of atomic sites (per m³)

Q(v): vacancy formation energy (J/mol or eV/atom)

K: boltzmann constat

T: temp in kelvin


<p>N(v): number of vacancies</p><p>N: number of atomic sites (per m³)</p><p>Q(v): vacancy formation energy (J/mol or eV/atom)</p><p>K: boltzmann constat</p><p>T: temp in kelvin</p><p></p>
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Vacancy fraction

The ratio of vacancies to total atomic sites

<p>The ratio of vacancies to total atomic sites</p>
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Number of atomic sites (or number of atoms)

p: density

N(A): avogadro’s number (6.022E23)

A: atomic weight

<p>p: density</p><p>N(A): avogadro’s number (6.022E23)</p><p>A: atomic weight</p>
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Celsius to kelvin

T(k)=T(C)+273

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Scattering

The change in direction of a wave when it interacts with an obstacle such as atoms in a crystal

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Diffraction

Waves scatter by regularly spaced obstacles interfere with one another, producing reinforcement under suitable conditions

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Edge-dislocation Burgers-vector relationship

The burger vector is perpendicular to the dislocation line

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Screw-dislocation

Burger-vector

Relationship

The vector is parallel to the dislocation line

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mixed dislocation

Burgers-vector

Relationship

The burger vector is at an oblique angle to the dislocation line

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Grain boundary

A boundary separating two neighboring crystals with different orientations

<p>A boundary separating two neighboring crystals with different orientations </p>
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Low angle grain boundary

Boundary with small misorientation angle

Modeled as an array of dislocations

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High angle grain boundary

A boundary with large misorientation angle and greater atomic mismatch

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Grain size effects

Smaller grains provide more grain-boundary area and generally increases yield strength

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Hall-patch Strengthening

The strengthing effect cause by grain boundaries

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Cause of screw dislocation

A shear stress that displaced one part of the crystal relative to another