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Timothy A. Philpot - Mechanics of materials _ an integrated learning system-John Wiley (2017)

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Stress Invariance

The normal stress acting on the n face of the stress element shown in Figure 12.11 can be

determined from Equation (12.5). The normal stress acting on the t face can also be obtained

from Equation (12.5) by substituting θ + 90° in place of θ, giving the following equation:

σx + σ y σx − σ y

σ t = − cos2θ − τxy

sin2θ

(12.7)

2 2

If the expressions for σ n and σ t [Equations (12.5) and (12.7)] are added, the following relationship

is obtained:

σn + σt = σx + σ y

(12.8)

Equation (12.8) shows that the sum of the normal stresses acting on any two orthogonal

faces of a plane stress element is a constant value, independent of the angle θ. This mathematical

characteristic of stress is termed stress invariance.

Stress is expressed with reference to specific coordinate systems. The stress transformation

equations show that the n–t components of stress are different from the x–y components,

even though both are representations of the same stress state. However, certain functions

of stress components are not dependent on the orientation of the coordinate system.

These functions, called stress invariants, have the same value regardless of which coordinate

system is used. Two invariants, denoted I 1 and I 2 , exist for plane stress:

Sign conventions

I

I

= σ + σ (or I = σ + σ )

1 x y 1 n t

2

2

2

= σσ − τ (or I = σ σ − τ )

x y xy 2 n t nt

(12.9)

The sign conventions used in the development of the stress transformation equations must

be rigorously followed. The sign conventions can be summarized as follows:

1. Tensile normal stresses are positive; compressive normal stresses are negative. All of the

normal stresses shown in Figure 12.11 are positive.

2. A shear stress is positive if it

• acts in the positive coordinate direction on a positive face of the stress element or

• acts in the negative coordinate direction on a negative face of the stress element.

All of the shear stresses shown in Figure 12.11 are positive. Shear stresses pointing in

opposite directions are negative.

An easy way to remember the shear stress sign convention is to use the directions

associated with the two subscripts. The first subscript indicates the face of the stress

element on which the shear stress acts. It will be either a positive face (plus) or a negative

face (minus). The second subscript indicates the direction in which the stress acts,

and it will be either a positive direction (plus) or a negative direction (minus).

• A positive shear stress has subscripts that are either plus–plus or minus–minus.

• A negative shear stress has subscripts that are either plus–minus or minus–plus.

3. Angles measured counterclockwise from the reference x axis are positive. Conversely,

angles measured clockwise from the reference x axis are negative.

4. The n–t–z axes have the same order as the x–y–z axes. Both sets of axes form a righthand

coordinate system.

493

gENERAL EQuATIONS OF PLANE

STRESS TRANSFORMATION

t

σt

σn

τtn

θ

τnt

y

FIGURE 12.11

τnt

τtn

σt

σn

mecmovies 12.5 presents

an animated discussion of

terminology used in stress

transformations.

mecmovies 12.2 presents an

interactive activity that focuses

on the proper determination of

the angle θ.

mecmovies 12.3 presents a

game that tests understanding

of the proper sign conventions

and their use in the stress

transformation equations.

θ

n

x

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