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The Ductile-to-Brittle Transition and Crystal Structure

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Materials Science: 10 Things Every Engineer Should Know

Universidad de California, Davis

4.6 (989 calificaciones) | 32K estudiantes inscritos

We explore “10 things” that range from the menu of materials available to engineers in their profession to the many mechanical and electrical properties of materials important to their use in various engineering fields. We also discuss the principles behind the manufacturing of those materials. By the end of the course, you will be able to: * Recognize the important aspects of the materials used in modern engineering applications, * Explain the underlying principle of materials science: “structure leads to properties,” * Identify the role of thermally activated processes in many of these important “things” – as illustrated by the Arrhenius relationship. * Relate each of these topics to issues that have arisen (or potentially could arise) in your life and work. If you would like to explore the topic in more depth you may purchase Dr. Shackelford's Textbook: J.F. Shackelford, Introduction to Materials Science for Engineers, Eighth Edition, Pearson Prentice-Hall, Upper Saddle River, NJ, 2015

Destrezas que aprenderás

Materials, Mechanical Engineering, Engineering Design, Electrical Engineering

Revisiones

4.6 (989 calificaciones)

5 stars
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PC

Mar 05, 2018

This course was alot more educational then I thought it would be but now I compare what has shaped me in in life to creep deformation. I especially loved the lecture " a play on good and evil".

AP

Jun 24, 2018

Beautiful course. Helped me a lot in the selection of materials for our rocketry team. I'll be sure to suggest this course to my fellow teammates. A big thumbs-up to UCDAVIS for this course.

De la lección

Creep Deformation / The Ductile-to-Brittle Transition

Welcome to week 3! In lesson five we’ll explore creep deformation and learn to analyze a creep curve. We’ll apply the Arrhenius Relationship to creep deformation and identify the mechanisms of creep deformation. In lesson six we find that the phenomenon of ductile-to-brittle transition is related to a particular crystal structure (the body-centered cubic). We’ll also learn to plot the ductile-to-brittle transition for further analysis.

The Ductile-to-Brittle Transition and Crystal Structure7:16

Plotting the Ductile-to-Brittle Transition5:03

Impartido por:

James Shackelford
Distinguished Professor Emeritus

And welcome back once again to the materials teaching laboratories here in

Kemper Hall on the University of California Davis Campus.

Today we're gonna talk about ductile to brittle transition and

find out how small changes in ambient temperature can make a big difference in

terms of mechanical performance.

[MUSIC]

And so I'm standing here today in front of a Charpy tester.

This is a long time traditional mechanical testing

machine that basically does in one very quick swoop.

And you'll see an example of that, In our segment today,

in that one swing of a large pendulum hammer arm

the breaking of a material by impact.

And essentially what it's doing in that split second

is doing the same thing we did in the Instron machines in our earlier segment,

talking about the big four mechanical properties.

But in this case, we're doing it in a very rapid sequence.

We're taking the material to a very quick elastic deformation,

then well on to substantial plastic deformation and then final failure.

And as we'll emphasize in our next segment, we've notched that sample,

put a small defect in the surface, in order to control where it fractures and

to ensure that it does fracture in an efficient manner.

So it reminds us,

actually of the discovery of what we call the ductile-to-brittle transition.

Back in the World War II era, there were some ships called the Liberty Ships,

which were a British design, but manufactured largely in the United States.

Utilitarian, not terribly attractive Navy vessel that was meant to provide

resources during the war to our allies in Europe, hence the name liberty ship.

But in the process, when these ships were

sent into very cold North Atlantic waters, some failed.

Some literally split in half.

They fractured catastrophically.

At first it was thought that perhaps there were bad weld nuts to explain the failure.

But when the materials themselves were sent back to Cambridge University

in England for analysis,

is when metalers then discovered this ductile to brittle transition concept.

And it's a case in which a material that performed just fine in a room temperature,

ambient, atmosphere of the laboratory,

in a very cold environment became brittle, like a piece of glass.

So today we're looking at an impact energy measuring device, the Charpy tester.

And in order to appreciate why that is so, we need to look at

three crystal structures in this brief introduction to material science.

But we certainly don't expect you to learn all the details of crystallography and

the nature of the structures

on the atomic scale of these important metallurgical alloys.

But keep in mind three main structures which are representative of most

of the commercial metal alloys that we deal with in everyday engineering.

The face centered cubic crystal structure, the body

centered cubic crystal structure and the hexagonal close packed crystal structure.

Most common metals fall into one of those three categories.

And what we see in a very careful analysis of the crystallography

of these materials is that these highly densely packed atomic arrangements,

the face center cubic structure has, what we call, 12 slip systems.

A slip system is nothing more than a combination of

the high atomic density planes and

high atomic density directions, in which dislocations move.

And remember that segment in which we talked about how dislocations are at

the basis of plastic deformation.

Well, for face-centered cubic alloys that dislocation motion is an easy one because,

again, of the large number of slip systems.

By contrast, in the hexagonal close-packed structure, equally highly dense

arrangement of atoms because of the geometry of the hexagonal arrangement,

a limited number of slip systems, that material is relatively brittle.

So those HCP or hexagonal close packed crystal structure alloys

tend to be brittle in nature over a wide temperature range.

Face center cubic materials tend to be ductile over a wide temperature range.

But the body center cubic crystal structure alloys which include so

many of the common ferris alloys, the common structural steels that we make so

many things from in everyday engineering practice, those are somewhat intermediate.

They also, as with the FCC, have 12 flip systems,

so they have the ability to be very ductile.

And so again the Liberty ship materials that were tested at room temperature

in the laboratories in England initially were just fine.

However, when they were retested at Cambridge University at very low

temperatures representative of the cold,

north Atlantic sea temperatures, they turned out to be very brittle.

And for the simple reason that the body-centered cubic

crystal structure is one, in which the dislocation motion is slower.

And so as a result, as the material is cooled down to a lower temperature,

that cold North Atlantic Sea ambient temperature then,

that material behaves in a very brittle way.

The dislocations can't move, plastic deformation is choked off and

as a result the material was brittle, almost like a piece of glass.

Well in appreciating those differences then, again,

we can monitor that now routinely in laboratories, by simply measuring

the performance of various metal alloys at various temperatures.

And again, it's critically important to monitor these body centered cubic alloys,

such as the common structural steels, at a range of temperatures from

well above room temperature to well below room temperature.

The plot of those then will very often show a transition,

very low impact energy corresponding to brittle fracture at low temperatures and

then high impact energies corresponding to

ductile fracture at relatively higher temperatures.

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