Taylor’s expansion - 2.1 | 15. Need for stress-strain relation | Solid Mechanics
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2.1 - Taylor’s expansion

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Interactive Audio Lesson

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Introduction to Stress-Strain Relation

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0:00
Teacher
Teacher

Welcome class! Today, we will discuss the stress-strain relation. Can anyone tell me why it’s important to understand this relationship?

Student 1
Student 1

Isn't it to ensure that materials don’t fail under stress?

Teacher
Teacher

Exactly! Knowing how materials respond to stress helps us design safer structures. Now, what happens if we know stress but not strain?

Student 2
Student 2

We can't predict how the material will deform, right?

Teacher
Teacher

Correct! That’s where the stress-strain relationship comes in. Let’s delve into the Taylor’s expansion next.

Taylor's Expansion

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Teacher
Teacher

The Taylor’s expansion of stress components allows us to express stress in terms of strain. Can anyone summarize what this means?

Student 3
Student 3

It means we can relate stress directly to strain using a mathematical series, right?

Teacher
Teacher

Spot on! We take derivatives at the zero-strain state, which simplifies our calculations. What do we call the stress at that state?

Student 4
Student 4

Residual stress!

Teacher
Teacher

Great! And what do we assume for this course regarding residual stress?

Student 1
Student 1

That it is zero.

Teacher
Teacher

Exactly! That leads us to our linear stress-strain relation.

Linear Stress-Strain Relation

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Teacher
Teacher

Now, let’s derive the linear stress-strain relation. When we neglect higher-order terms, what do we get?

Student 2
Student 2

We get that stress is approximately proportional to strain!

Teacher
Teacher

Correct! Specifically, we express this relationship as σ = C * ε, where C is the stiffness tensor. Does anyone remember why it’s important to evaluate these derivatives at the reference configuration?

Student 3
Student 3

Because it captures the material's initial behavior.

Teacher
Teacher

Precisely! Now, let’s talk about the stiffness tensor next.

Stiffness Tensor and Its Symmetries

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0:00
Teacher
Teacher

The stiffness tensor C has many components, but due to symmetrical properties, not all are independent. Can anyone tell me how many independent components we start with?

Student 4
Student 4

81, because there are 3 indices ranging from 1 to 3.

Teacher
Teacher

Exactly! And after applying minor symmetry, how many do we reduce to?

Student 1
Student 1

36 independent components!

Teacher
Teacher

Correct again! And through major symmetry, we can further reduce it to how many?

Student 2
Student 2

21!

Teacher
Teacher

Right! This reduction is crucial for understanding material behavior.

Introduction & Overview

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Quick Overview

This section explores Taylor's expansion as a method to relate stress to strain in solid mechanics.

Standard

In this section, we discuss the Taylor's series expansion of stress with respect to strain components, explaining how it leads to the linear stress-strain relationship. The concepts of residual stress, stiffness tensor, and the significance of evaluating derivatives at zero strain state are also highlighted.

Detailed

Taylor’s Expansion

Taylor's expansion provides a framework to express stress components in terms of strain components, crucial for deriving the stress-strain relation in solid mechanics. The relationship begins with the definition of stress tensors and how they can depend on strain components. All derivatives in this expansion are evaluated at the zero strain state, denoted as "residual stress". We typically assume this residual stress is zero for simpler calculations.

The linear stress-strain relation simplifies to a first-order approximation, where we neglect higher-order terms of strain that are much smaller than linear terms.

In solid mechanics, these derivatives represent the components of the stiffness tensor, which captures the material's response to stress. Given the symmetry in stress and strain tensors, the total number of independent components in the stiffness tensor can be reduced significantly from 81 to 21 through symmetry arguments, namely minor and major symmetries. This underpins our understanding of material properties crucial for predicting the behavior of various materials under load.

Audio Book

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Overview of Taylor’s Expansion

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The Taylor’s expansion of σ with respect to strain components will be as follows:

(8)

All the derivatives have been evaluated at zero strain state, i.e., ϵ = 0.

Detailed Explanation

Taylor's expansion is a mathematical method to approximate a function. In this case, we are using Taylor's expansion to express stress (σ) in terms of strain components (ϵ). The formula provided indicates that at the zero strain state, the derivatives used in the equation give us the rates of change of stress with respect to strain. This is foundational in material science as it allows us to relate how materials deform under stress.

Examples & Analogies

Think of Taylor's expansion like estimating the height of a roller coaster at various points. If you start from a point where you know the height (zero strain state), you can use the slopes (derivatives) at that point to predict the height at nearby points, just like using the behavior of stress at a zero strain state to predict how it will behave at small strains.

Residual Stress and Linear Relation

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The first term (denoted as σ0) is called the residual stress and gives the stress in the zero strain state or the reference configuration. The reference configuration is typically chosen such that the stress in the body is zero in this state. Accordingly, we will assume σ0 to be zero for this course. The second term is linear in strain while the third term is quadratic in strain. We had also said earlier that for this course, we will work with very small strains only. Thus, we can neglect the terms which are quadratic or higher order in strain components as they are much smaller than the linear term. Thus, we are left with:

(9) This is called the linear stress-strain relation.

Detailed Explanation

In this chunk, we discuss the residual stress, which represents the state of stress when there is no deformation (zero strain). For this course, we simplify our analysis by assuming this residual stress is zero. The stress can then be approximated using only the linear term based on small strains, which gives us a solid foundation for working with the linear stress-strain relation. By ignoring higher-order terms, we make our calculations simpler and more practical while ensuring significant accuracy for small deformations.

Examples & Analogies

Imagine stretching a rubber band. When you first stretch it slightly, the relationship between how much you stretch it and the tension you feel is straightforward (linear). However, if you stretch it too much, the behavior becomes complex and non-linear. For small stretches (small strains), we only care about that simple relationship, making it easier to predict how the rubber band will behave.

Significance of Derivatives

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These derivatives have a special significance in solid mechanics: they denote the components of the stiffness tensor. It is a fourth-order tensor because it has four indices all running from 1 to 3 and is denoted as C:

(10)

Thus, we can write:

(11)

Detailed Explanation

The derivatives obtained from the Taylor expansion are crucial as they correspond to the stiffness tensor components. This tensor characterizes how a material resists deformation under stress. As a fourth-order tensor, it encompasses a wide range of material behaviors, indicating that the relationship between stress and strain is influenced by material properties and the direction of applied forces. Knowing these components allows engineers to predict and design materials that will perform well under specified conditions.

Examples & Analogies

Think of the stiffness tensor like a fabric that holds its shape when stretched. Different materials (like cotton versus steel) have different stiffness properties. When you pull on the fabric, the way each type responds differs based on its stiffness tensor. Understanding that tensor helps you know how that fabric will behave in a quilt or a tent.

Definitions & Key Concepts

Learn essential terms and foundational ideas that form the basis of the topic.

Key Concepts

  • Stress-Strain Relation: Essential for predicting material failure.

  • Taylor's Expansion: A means to express stress in terms of strain.

  • Residual Stress: Assumed to be zero in many analyses for simplification.

  • Stiffness Tensor: Represents material properties and reduces complexity in calculations.

Examples & Real-Life Applications

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Examples

  • Example of a simple one-dimensional spring experiencing stress and strain.

  • Illustration of how Taylor's expansion can simplify the calculation of material responses.

Memory Aids

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🎵 Rhymes Time

  • Stress and strain, in harmony they play, Taylor's series helps us see the way.

📖 Fascinating Stories

  • Imagine a stretchy rubber band; it can only stretch so far without breaking. Just like in mechanics, if we understand its limits through linear relations, we can use Taylor's expansion to predict when it will snap!

🧠 Other Memory Gems

  • Remember: SRT - Stress, Residual, Taylor. These are key concepts in relating stress with strain.

🎯 Super Acronyms

C for **C**onstitutive, T for **T**wo-way relation; keep in mind Stress and Strain's communication!

Flash Cards

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Glossary of Terms

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  • Term: Stress

    Definition:

    The internal resistance offered by a material when subjected to an external load.

  • Term: Strain

    Definition:

    The measure of deformation representing the displacement between particles in a material.

  • Term: Residual Stress

    Definition:

    The stress present in a material in the absence of external loading.

  • Term: Stiffness Tensor

    Definition:

    A fourth-order tensor that relates stress to strain in a material.

  • Term: Taylor's Expansion

    Definition:

    A mathematical expansion that approximates a function as a sum of terms calculated from the values of its derivatives.

  • Term: Linear StressStrain Relation

    Definition:

    The relationship between stress and strain where stress is directly proportional to strain.