MSE203 Mechanical Behaviour:  Continuum Mechanics

In second year, I teach a 10-lecture course on stress tensors in the spring term.  Here we learn how to deal with stress states in materials. So we define stress tensors and examine how to rotate them, both using tensor rotations and Mohr’s circle. We look at how to analyse stresses in simple bodies like shafts and pressure vessels. Then we look at strain, elasticity and how to measure strains by diffraction. We can then look at anisotropic elasticity, particularly in crystalline materials. We finish up by studying yielding and yield criteria.

As with MSE104, the course is taught by Peer Instruction, supported by notes and videos on YouTube.

The notes are here, which are also accompanied by examples here. In the tutorials, we will go through some of these examples (Tutorial 1: Q5,6,8,9 and Tutorial 2: Q20, 23,24,25); the others are discussed in the videos. Solutions are provided with the examples (but don’t look until you’ve tried them :-).

If you like lectures, then they are online on YouTube.  The video numbering corresponds to the ‘lecture’ classes in which we will discuss that material.  As with MSE104, there is no intention to re-lecture the material in class: instead students should review the material before class in their own time, ready to discuss and explore it in the class session.

After the end of the lectures, there is a short 1-hr test to prepare students for the exam in June.

Lecture 1.  1a: Defining Stress States  1b: Rotations in 2D – the inclined plane

Lecture 2. 2a: Rotations in 2D – Principal stresses and axes. 2b: Mohr’s circle

Lecture 3. 3a: Pressure Vessels  3b: Q1-4 Pressure Vessels and Using Mohr’s Circle

Lecture 4. 4a: 3D Stress Tensors. 4Q7 – Q7 hollow rotating power transmission shaft. 4Q10 – biaxial test specimen.

Lecture 5. 5a: More 3D Stress Tensors. 5b Q11-12 A Mohr’s circle and some eigenvalues.

Lecture 6. 6a: Strain and 6b Isotropic Elasticity. Also Q15, Q16 and Q27.

Lecture 7. 7a: Anisotropic Elasticity

Lecture 8. 8a: Strain Measurement

Lecture 9. 9a: Yield Surfaces and Criteria

Additional Resources

Dieter (Ch2) is really great for this course, and is probably the core reference. But, the main drawback of Dieter is that he soft-pedals the tensor mathematics.

To go further, particularly for anisotropic elasticity, the Nye’s book is the core reference. But, its quite dense and written in the style of the time.

If you are struggling to conceive of what a tensor is as a mathematical object, then I quite like this video.

15 Responses to MSE203

  1. Bedanta Lath says:

    Hello Sir.
    May i know the complete name of the Nye’s book

  2. Bedanta Lath says:

    Hello Sir
    I am an engineering student.I really want to know some practical applications of these concepts,or in other sense, why these concepts are developed?

    • dyedavid says:

      (i) Real materials are subjected to mutliaxial stress situations – and you want to know how they will respond (elastically strain, yield, flow), and therefore if your structure will respond to the loading in a safe manner.
      (ii) Real materials are anistropic, and often if you want to measure these properties, you need to understand how to manipulate stress and strain states.
      (iii) You can’t always measure the loads applied, but its relatively easy to apply strain gauges to a surface and measure the strains – which you will then have to convert into the stress state somehow.
      (iv) Most materials are made up of many individual single crystals, so measurements and modelling of how these respond is very important to developing better materials – which means understanding and working with stress and strain states.

      –> All these considerations mean that its very difficult to work with stresses and strains meaningfully without treating them properly as tensors. Sure, you can work on idealised pin-jointed beams, but surely we want to do more than that?

  3. 314singh says:

    Hello sir,
    First of all I would like to sincerely thank you for your videos. Your way of explaining a concept is really commendable. After watching them I really have started to develop an appreciation for the subject. I was wondering whether you would consider uploading lectures on Shear force and Bending moment diagrams as well in the near future.

  4. dk says:

    Dear Professor Dye. First of all thanks a lot for putting up the course material for this course. This is a very important course for people interested in mechanical metallurgy, espescially because in conventional materials science and metallurgy curriculum, not much of the emphasis is given to mechanics or the mathematics of it. I believe in order to grow further in this field knowledge of Linear Algebra becomes very important.
    There is one doubt that I would like to clarify from you. In a uniaxial tensile test cylindrical specimen, at any point inside the cylinder, is it theoretically possible to achieve a uniaxial state of stress? Or, is our notion of uniaxial stress in the specimen just an assumption based on the fact that the length of the specimen is very big in comparison to its diameter (cross-section) which would lead to stress state closer to uniaxial one?

    • dyedavid says:

      For a uniaxial testing machine that is perfectly aligned, then for a well behaved material the stress state will be uniaxial. Real machines and load trains aren’t perfectly aligned or perfectly rigid, so avoiding bending moments can be tricky. The ASTM HCF and LCF test standards contain good advice.

  5. dk says:

    Dear Professor Dye,
    Is it possible to get access to the notes “A Mostofi, MSE201 notes on Tensors”, which are mentioned in your notes?


  6. dyedavid says:

    If you are in Imperial, they are on blackboard. Otherwise, they aren’t publicly downloadable that I know of.

  7. Molurus Devalles says:

    Hello Mr. David,

    I am glad for all your lectures. I am attending “Stress Tensors” lectures of yours. However, I would like to ask “where can I find derivation for direction cosines of maximum shear stresses as mentioned in Dieter?”

    it is like:

    l1 0 +- 1/(2)^(1/2) +- 1/(2)^(1/2)
    same for l2 and l3

    In anticipation of your urgent response.

    • dyedavid says:

      If you mean equation 2-20 in Dieter, then this is found by doing a 45 degree rotation between each of the pairs of principal axes. Probably the easiest way to prove it is to simply do the tensor rotation, or by sketching it out.

  8. Ravi says:

    The state of stress at a point is given as ( all in Mpa ) sigma xx= 40 .sigma yy= -40 sigma zz= 60 . Tau xx=20 taught yz=20 taught yz=25 tau xz =15 .find the resultant stress on an oblique plane equally inclined to the three axes also.find the normal shear stress component.

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