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CHE 333 Class 12 Defects in Crystals.

CHE 333 Class 12 Defects in Crystals.. Perfect Structure Perfect Structure for FCC, BCC and HCP crystals – all atom sites filled with an atom. Reality

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Page 1: CHE 333 Class 12 Defects in Crystals.. Perfect Structure Perfect Structure for FCC, BCC and HCP crystals – all atom sites filled with an atom. Reality

CHE 333 Class 12

Defects in Crystals.

Page 2: CHE 333 Class 12 Defects in Crystals.. Perfect Structure Perfect Structure for FCC, BCC and HCP crystals – all atom sites filled with an atom. Reality

Perfect Structure

Perfect Structure for FCC, BCC and HCP crystals – all atom sites filled with an atom.

Reality – this does not happen.

Defects occur in the crystal structure. These can range from small to large, that is a missing atom or many missing atoms to form a void in the material.

Missing Atom – called a “vacancy”. There is an equilibrium number of vacancies in any

Crystal. For aluminum at room temperature it is about one vacancy for every 1010 atoms.

At around 500C , the number is one in 104, as the relationship is exponential with

Temperature.

Processes such as self and substitutional diffusion, in which atoms move around in a

Solid, depend on vacancies, so these are a function of temperature, and increase with it.

Many high temperature processes are controlled by the movement of vacancies in the

Crystal structure.

Page 3: CHE 333 Class 12 Defects in Crystals.. Perfect Structure Perfect Structure for FCC, BCC and HCP crystals – all atom sites filled with an atom. Reality

Vacancy

Page 4: CHE 333 Class 12 Defects in Crystals.. Perfect Structure Perfect Structure for FCC, BCC and HCP crystals – all atom sites filled with an atom. Reality

Line or Two Dimensional Defects

A dislocation in a crystal structure. An extra half plane of atoms is present in the crystal structure.The end of the extra half plane determines the slip plane, which is also the plane of densest packing, andThe dislocation line. The atomic motion is determined by the Burgers vector of the dislocation “b”. The Burgers vector is determinedBy counting around the dislocation an equal number of steps in each direction. For example,,going clockwiseAround the dislocation from atom number 1. One right is followed by 3 down, followed by 3 left, then 3 up. ForAn equal number of atoms, then only two steps to the right is allowed, to finish at atom 2. The BurgersVector is then the distance needed to close the loop, as shown in the figure.One of the features of an edge dislocation is that the Burgers vector is 90 degrees to the dislocation line,But parallel to the overall motion of the dislocation.

2 1

Page 5: CHE 333 Class 12 Defects in Crystals.. Perfect Structure Perfect Structure for FCC, BCC and HCP crystals – all atom sites filled with an atom. Reality

Screw Dislocation

A second type of dislocation is a SCREW dislocation. The properties in this case are that theBurgers vector is parallel to the line, but 90 degrees to the movement of the dislocation line.Note that the Burgers vector is a constant along the dislocation line. However if the line curvesThen a mixed dislocation will exist, with both edge and screw characteristics.

Page 6: CHE 333 Class 12 Defects in Crystals.. Perfect Structure Perfect Structure for FCC, BCC and HCP crystals – all atom sites filled with an atom. Reality

Dislocation

Page 7: CHE 333 Class 12 Defects in Crystals.. Perfect Structure Perfect Structure for FCC, BCC and HCP crystals – all atom sites filled with an atom. Reality

Dislocation Movement.Dislocations have a displacement associated with them, the Burgers vector. The Burgers vector is

The direction of densest packing in a crystal, so for FCC it is <110>, for BCC it is <111> and for HCP

It is <1120>. The combination of a slip plane and a slip direction is called a slip system. So the

Movement of a dislocation along a slip plane in a slip direction produces physical displacements.

A force is required to move the dislocations, which comes from stressing a material.

Page 8: CHE 333 Class 12 Defects in Crystals.. Perfect Structure Perfect Structure for FCC, BCC and HCP crystals – all atom sites filled with an atom. Reality

Twins – Atomic Arrangement

Atomic Structure of Twins

Page 9: CHE 333 Class 12 Defects in Crystals.. Perfect Structure Perfect Structure for FCC, BCC and HCP crystals – all atom sites filled with an atom. Reality

Twins

Twins in 70-30 Brass

Page 10: CHE 333 Class 12 Defects in Crystals.. Perfect Structure Perfect Structure for FCC, BCC and HCP crystals – all atom sites filled with an atom. Reality

Twins and Dislocations

The same displacements can be achieved by either dislocation motion onSlip planes or by twins.

Page 11: CHE 333 Class 12 Defects in Crystals.. Perfect Structure Perfect Structure for FCC, BCC and HCP crystals – all atom sites filled with an atom. Reality

Grain Boundaries.

1

2

3

Page 12: CHE 333 Class 12 Defects in Crystals.. Perfect Structure Perfect Structure for FCC, BCC and HCP crystals – all atom sites filled with an atom. Reality

Grain SIze

ASTM has a grain size number from 1 to 10. It is determined by preparing aSample for examination at 100 times magnification and measuring the numberOf grains per square inch.

N=2(n-1)

Where N= average number of grains per square inch at x100 mag and N = grain number.Usually charts can be used which are standards against which a sample iscompared. The chart most closely resembling the test samples is the grain size.

Page 13: CHE 333 Class 12 Defects in Crystals.. Perfect Structure Perfect Structure for FCC, BCC and HCP crystals – all atom sites filled with an atom. Reality

Pores

Al 356 Casting alloy with pores.

Page 14: CHE 333 Class 12 Defects in Crystals.. Perfect Structure Perfect Structure for FCC, BCC and HCP crystals – all atom sites filled with an atom. Reality

Homeworks

1. Age Hardening.

An alloy contains 10% B in A. + solvus temp is 475 C. + Liquid solidus temp is 525 C. Detail the temperature and time needed to age harden this alloy. From this data what would be the maximum service temperature for this alloy.

Page 15: CHE 333 Class 12 Defects in Crystals.. Perfect Structure Perfect Structure for FCC, BCC and HCP crystals – all atom sites filled with an atom. Reality

Homeworks

2. Dislocations.For an edge dislocation, provide a Burgers circuit to indicate how a Burgers vector is determined. From the notes from class 9, Precipitation Hardening, what is the actual distance for the Burgers vector for aluminum and copper?

Atomic radius for Fe 0.124nm, Ti 0.145,Al0.143,Cu0.128,Zn 0.133. Calculate Burgers vectors for

these. Also for 0.01mm movement how many Dislocations are needed?