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

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Also, Equation (13.17) becomes, simply,

γ

xy

1

= τxy

(13.25)

G

567

gENERALIzEd HOOkE’S LAw

FOR ISOTROPIC MATERIALS

Then, solving Equation (13.24) for the stresses in terms of the strains gives the following result:

σ

σ

E

= ( ε

1 −

2

ν

+ νε )

E

= ( ε

2

1 − ν

+ νε )

x x y

y y x

(13.26)

Equation (13.26) can be used to calculate normal stresses from measured or computed

normal strains.

Note that the out-of-plane normal strain ε z is generally not equal to zero for the plane

stress condition. An expression for ε z in terms of ε x and ε y was stated in Equation (13.15).

This equation can be derived by substituting Equation (13.26) into the expression

to give

ν =−

E ( σ + σ )

ε z x y

ν ν E

ε z =− ( σ x + σ y)

= − [( εx + νεy) + ( εy + νε x )]

2

E

E1

− ν

ν

=−

[(1 + νε ) x + (1 + νε ) y]

(1 − ν)(1 + ν) ν

=− ( x y)

1 ν ε + ε −

(13.27)

ExAmpLE 13.7

On the free surface of an aluminum [E = 10,000 ksi; ν = 0.33] component, three strain

gages arranged as shown record the following strains: ε a = −420 µε, ε b = 380 µε, and

ε c = 240 µε.

Determine the normal stress that acts along the axis of gage b (i.e., at an angle of

θ = 45° with respect to the positive x axis).

Plan the Solution

At first glance, one might be tempted to use the measured strain in gage b and the elastic

modulus E to compute the normal strain acting in the specified direction. However, that approach

is not correct because a state of uniaxial stress does not exist. In other words, the

normal stress acting in the 45° direction is not the only stress acting in the material. To solve

this problem, first reduce the strain rosette data to obtain ε x , ε y , and γ xy . The stresses σ x , σ y ,

and τ xy can then be calculated from Equations (13.26) and (13.25). Finally, the normal stress

in the specified direction can be calculated from the stress transformation equation.

c

y

45°

45°

b

a

x

SolutioN

From the geometry of the rosette, gage a measures the strain in the x direction and gage c

measures the strain in the y direction. Therefore, ε x = −420 µε and ε y = 240 µε. To compute

the shear strain γ xy , write a strain transformation equation for gage b:

2 2

380 = ε cos (45 ° ) + ε sin (45 ° ) + γ sin(45 ° )cos(45 ° )

x y xy

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