Beer F.P., Johnston E.R., DeWolf J.T., Mazurek D.F. Mechanics of Materials

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467

*7.7 YIELD CRITERIA FOR DUCTILE MATERIALS UNDER

PLANE STRESS

Structural elements and machine components made of a ductile

material are usually designed so that the material will not yield under

the expected loading conditions. When the element or component is

under uniaxial stress (Fig. 7.36), the value of the normal stress s

that will cause the material to yield can be obtained readily from a

tensile test conducted on a specimen of the same material, since the

test specimen and the structural element or machine component are

in the same state of stress. Thus, regardless of the actual mechanism

that causes the material to yield, we can state that the element or

component will be safe as long as s

, s

, where s

is the yield

strength of the test specimen.

7.7 Yield Criteria for Ductile Materials

under Plane Stress

Fig. 7.36 Structural element under

uniaxial stress.



On the other hand, when a structural element or machine com-

ponent is in a state of plane stress (Fig. 7.37a), it is found convenient

to use one of the methods developed earlier to determine the principal

stresses s

and s

at any given point (Fig. 7.37b). The material can

then be regarded as being in a state of biaxial stress at that point. Since

this state is different from the state of uniaxial stress found in a speci-

men subjected to a tensile test, it is clearly not possible to predict

directly from such a test whether or not the structural element or

machine component under investigation will fail. Some criterion regard-

ing the actual mechanism of failure of the material must first be estab-

lished, which will make it possible to compare the effects of both states

of stress on the material. The purpose of this section is to present the

two yield criteria most frequently used for ductile materials.

Maximum-Shearing-Stress Criterion. This criterion is based on

the observation that yield in ductile materials is caused by slippage

of the material along oblique surfaces and is due primarily to shear-

ing stresses (cf. Sec. 2.3). According to this criterion, a given struc-

tural component is safe as long as the maximum value t

max

of the

shearing stress in that component remains smaller than the corre-

sponding value of the shearing stress in a tensile-test specimen of

the same material as the specimen starts to yield.

Recalling from Sec. 1.11 that the maximum value of the shear-

ing stress under a centric axial load is equal to half the value of the

corresponding normal, axial stress, we conclude that the maximum

shearing stress in a tensile-test specimen is

as the specimen

starts to yield. On the other hand, we saw in Sec. 7.6 that, for plane

stress, the maximum value t

max

of the shearing stress is equal to

max

if the principal stresses are either both positive or both nega-

tive, and to

max

2 s

min

if the maximum stress is positive and the

(b)



(a)

Fig. 7.37 Structural element in

state of plane stress.

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468

Transformations of Stress and Strain

minimum stress negative. Thus, if the principal stresses s

and s

have the same sign, the maximum-shearing-stress criterion gives

, s

(7.23)

If the principal stresses s

and s

have opposite signs, the maximum-

shearing-stress criterion yields

2 s

, s

(7.24)

The relations obtained have been represented graphically in Fig. 7.38.

Any given state of stress will be represented in that figure by a point

of coordinates s

and s

, where s

and s

are the two principal

stresses. If this point falls within the area shown in the figure, the

structural component is safe. If it falls outside this area, the component

will fail as a result of yield in the material. The hexagon associated

with the initiation of yield in the material is known as Tresca’s hexagon

after the French engineer Henri Edouard Tresca (1814–1885).

Maximum-Distortion-Energy Criterion. This criterion is based

on the determination of the distortion energy in a given material,

i.e., of the energy associated with changes in shape in that material

(as opposed to the energy associated with changes in volume in the

same material). According to this criterion, also known as the von

Mises criterion, after the German-American applied mathematician

Richard von Mises (1883–1953), a given structural component is safe

as long as the maximum value of the distortion energy per unit vol-

ume in that material remains smaller than the distortion energy per

unit volume required to cause yield in a tensile-test specimen of the

same material. As you will see in Sec. 11.6, the distortion energy per

unit volume in an isotropic material under plane stress is

2 s

1 s

(7.25)

where s

and s

are the principal stresses and G the modulus of

rigidity. In the particular case of a tensile-test specimen that is start-

ing to yield, we have s

5 s

, s

5 0, and

5 s

6G. Thus,

the maximum-distortion-energy criterion indicates that the structural

component is safe as long as u

, (u

)

, or

2 s

1 s

, s

(7.26)

i.e., as long as the point of coordinates s

and s

falls within the area

shown in Fig. 7.39. This area is bounded by the ellipse of equation

2 s

1 s

5 s

(7.27)

which intersects the coordinate axes at s

56s

and s

56s

We can verify that the major axis of the ellipse bisects the first and

third quadrants and extends from A (s

5 s

) to B (s

5 s

), while its minor axis extends from C (s

5 2s

5 20.577s

)

to D (s

5 2s

5 0.577s

The maximum-shearing-stress criterion and the maximum-

distortion-energy criterion are compared in Fig. 7.40. We note that

the ellipse passes through the vertices of the hexagon. Thus, for the

states of stress represented by these six points, the two criteria give









Fig. 7.38 Tresca’s hexagon.

Fig. 7.39 Von Mises criterion.













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469

the same results. For any other state of stress, the maximum-shearing-

stress criterion is more conservative than the maximum-distortion-

energy criterion, since the hexagon is located within the ellipse.

A state of stress of particular interest is that associated with yield

in a torsion test. We recall from Fig. 7.22 of Sec. 7.4 that, for torsion,

min

5 2s

max

; thus, the corresponding points in Fig. 7.40 are located

on the bisector of the second and fourth quadrants. It follows that yield

occurs in a torsion test when s

52s

560.

according to the

maximum-shearing-stress criterion, and when s

52s

560.

577

according to the maximum-distortion-energy criterion. But, recalling

again Fig. 7.22, we note that s

and s

must be equal in magnitude

to t

max

, that is, to the value obtained from a torsion test for the yield

strength t

of the material. Since the values of the yield strength s

tension and of the yield strength t

in shear are given for various ductile

materials in Appendix B, we can compute the ratio t

for these

materials and verify that the values obtained range from 0.55 to 0.60.

Thus, the maximum-distortion-energy criterion appears somewhat

more accurate than the maximum-shearing-stress criterion as far as

predicting yield in torsion is concerned.

*7.8 FRACTURE CRITERIA FOR BRITTLE MATERIALS

UNDER PLANE STRESS

As we saw in Chap. 2, brittle materials are characterized by the fact

that, when subjected to a tensile test, they fail suddenly through

rupture—or fracture—without any prior yielding. When a structural

element or machine component made of a brittle material is under

uniaxial tensile stress, the value of the normal stress that causes it to

fail is equal to the ultimate strength s

of the material as determined

from a tensile test, since both the tensile-test specimen and the

element or component under investigation are in the same state of

stress. However, when a structural element or machine component

is in a state of plane stress, it is found convenient to first determine

the principal stresses s

and s

at any given point, and to use one of

the criteria indicated in this section to predict whether or not the

structural element or machine component will fail.

Maximum-Normal-Stress Criterion. According to this criterion,

a given structural component fails when the maximum normal stress

in that component reaches the ultimate strength s

obtained from

the tensile test of a specimen of the same material. Thus, the struc-

tural component will be safe as long as the absolute values of the

principal stresses s

and s

are both less than s

, s

(7.28)

The maximum-normal-stress criterion can be expressed graphically

as shown in Fig. 7.41. If the point obtained by plotting the values

and s

of the principal stresses falls within the square area shown

in the figure, the structural component is safe. If it falls outside that

area, the component will fail.

The maximum-normal-stress criterion, also known as Coulomb’s

criterion, after the French physicist Charles Augustin de Coulomb

7.8 Fracture Criteria for Brittle Materials

under Plane Stress













Torsion

0.577



0.5

Fig. 7.40











Fig. 7.41 Coulomb’s criterion.

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470

Transformations of Stress and Strain

(1736–1806), suffers from an important shortcoming, since it is based

on the assumption that the ultimate strength of the material is the

same in tension and in compression. As we noted in Sec. 2.3, this is

seldom the case, because of the presence of flaws in the material,

such as microscopic cracks or cavities, which tend to weaken the

material in tension, while not appreciably affecting its resistance to

compressive failure. Besides, this criterion makes no allowance for

effects other than those of the normal stresses on the failure mecha-

nism of the material.†

Mohr’s Criterion. This criterion, suggested by the German engi-

neer Otto Mohr, can be used to predict the effect of a given state

of plane stress on a brittle material, when results of various types of

tests are available for that material.

Let us first assume that a tensile test and a compressive test have

been conducted on a given material, and that the values s

and s

of the ultimate strength in tension and in compression have been

determined for that material. The state of stress corresponding to the

rupture of the tensile-test specimen can be represented on a Mohr-

circle diagram by the circle intersecting the horizontal axis at O and

(Fig. 7.43a). Similarly, the state of stress corresponding to the

failure of the compressive-test specimen can be represented by the

circle intersecting the horizontal axis at O and s

. Clearly, a state of

stress represented by a circle entirely contained in either of these cir-

cles will be safe. Thus, if both principal stresses are positive, the state

of stress is safe as long as s

, s

and s

, s

; if both principal

stresses are negative, the state of stress is safe as long as |s

| , |s

and |s

| , |s

|. Plotting the point of coordinates s

and s

(Fig. 7.43b), we verify that the state of stress is safe as long as that

point falls within one of the square areas shown in that figure.

In order to analyze the cases when s

and s

have opposite signs,

we now assume that a torsion test has been conducted on the material

and that its ultimate strength in shear, t

, has been determined. Draw-

ing the circle centered at O representing the state of stress correspond-

ing to the failure of the torsion-test specimen (Fig. 7.44a), we observe

that any state of stress represented by a circle entirely contained in

that circle is also safe. Mohr’s criterion is a logical extension of this

observation: According to Mohr’s criterion, a state of stress is safe if

it is represented by a circle located entirely within the area bounded

†Another failure criterion known as the maximum-normal-strain criterion, or Saint-

Venant’s criterion, was widely used during the nineteenth century. According to this cri-

terion, a given structural component is safe as long as the maximum value of the normal

strain in that component remains smaller than the value P

of the strain at which a tensile-

test specimen of the same material will fail. But, as will be shown in Sec. 7.12, the strain

is maximum along one of the principal axes of stress, if the deformation is elastic and the

material homogeneous and isotropic. Thus, denoting by P

and P

the values of the normal

strain along the principal axes in the plane of stress, we write

0, P

(7.29)

Making use of the generalized Hooke’s law (Sec. 2.12), we could express these relations

in terms of the principal stresses s

and s

and the ultimate strength s

of the material.

We would find that, according to the maximum-normal-strain criterion, the structural

component is safe as long as the point obtained by plotting s

and s

falls within the area

shown in Fig. 7.42 where n is Poisson’s ratio for the given material.





(a)

(b)

Fig. 7.43



1 





1 









Fig. 7.42 Saint-Venant’s criterion.

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471

by the envelope of the circles corresponding to the available data.

The remaining portions of the principal-stress diagram can now be

obtained by drawing various circles tangent to this envelope, deter-

mining the corresponding values of s

and s

, and plotting the points

of coordinates s

and s

(Fig. 7.44b).

More accurate diagrams can be drawn when additional test

results, corresponding to various states of stress, are available. If, on

the other hand, the only available data consists of the ultimate

strengths s

and s

, the envelope in Fig. 7.44a is replaced by the

tangents AB and A9B9 to the circles corresponding respectively to

failure in tension and failure in compression (Fig. 7.45a). From the

similar triangles drawn in that figure, we note that the abscissa of

the center C of a circle tangent to AB and A9B9 is linearly related

to its radius R. Since s

5 OC 1 R and s

5 OC 2 R, it follows

that s

and s

are also linearly related. Thus, the shaded area cor-

responding to this simplified Mohr’s criterion is bounded by straight

lines in the second and fourth quadrants (Fig. 7.45b).

Note that in order to determine whether a structural compo-

nent will be safe under a given loading, the state of stress should be

calculated at all critical points of the component, i.e., at all points

where stress concentrations are likely to occur. This can be done in

a number of cases by using the stress-concentration factors given in

Figs. 2.60, 3.29, 4.27, and 4.28. There are many instances, however,

when the theory of elasticity must be used to determine the state of

stress at a critical point.

Special care should be taken when macroscopic cracks have

been detected in a structural component. While it can be assumed

that the test specimen used to determine the ultimate tensile strength

of the material contained the same type of flaws (i.e., microscopic

cracks or cavities) as the structural component under investigation,

the specimen was certainly free of any detectable macroscopic cracks.

When a crack is detected in a structural component, it is necessary

to determine whether that crack will tend to propagate under the

expected loading condition and cause the component to fail, or

whether it will remain stable. This requires an analysis involving the

energy associated with the growth of the crack. Such an analysis is

beyond the scope of this text and should be carried out by the meth-

ods of fracture mechanics.

7.8 Fracture Criteria for Brittle Materials

under Plane Stress





(a)



(b)

Fig. 7.44 Mohr’s criterion.





(a)

(b)

Fig. 7.45 Simplified Mohr’s criterion.

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SAMPLE PROBLEM 7.4

The state of plane stress shown occurs at a critical point of a steel machine

component. As a result of several tensile tests, it has been found that the

tensile yield strength is s

5 250 MPa for the grade of steel used. Determine

the factor of safety with respect to yield, using (a) the maximum-shearing-

stress criterion, and (b) the maximum-distortion-energy criterion.

SOLUTION

Mohr’s Circle. We construct Mohr’s circle for the given state of

stress and find

ave

5 OC 5

1 s

180 2 4025 20 MPa

5 R 5 2

5 2

5 65 MPa

Principal Stresses

5 OC 1 CA 5 20 1 65 5185 MPa

5 OC 2 BC 5 20 2 65 5245 MPa

a. Maximum-Shearing-Stress Criterion. Since for the grade of steel

used the tensile strength is s

5 250 MPa, the corresponding shearing

stress at yield is

250 MPa

5 125 MPa

For t

5 65 MPa:

F.S. 5

125 MPa

65 MPa

F.S. 5 1.92

◀

b. Maximum-Distortion-Energy Criterion. Introducing a factor of

safety into Eq. (7.26), we write

2 s

1 s

F.S.

For s

5 185 MPa, s

5 245 MPa, and s

5 250 MPa, we have

1852

2 1852124521 1452

250

F.S.

114.3 5

250

F.S.

F.S. 5 2.19

◀

Comment. For a ductile material with s

5 250 MPa, we have drawn

the hexagon associated with the maximum-shearing-stress criterion and the

ellipse associated with the maximum-distortion-energy criterion. The given

state of plane stress is represented by point H of coordinates s

5 85 MPa

and s

5 245 MPa. We note that the straight line drawn through points

O and H intersects the hexagon at point T and the ellipse at point M. For

each criterion, the value obtained for F.S. can be verified by measuring the

line segments indicated and computing their ratios:

1a2 F.S. 5

5 1.92

1b2 F.S. 5

5 2.19

472

40 MPa

80 MPa

25 MPa

40 MPa

25 MPa

80 MPa

20 MPa







 250 MPa



 250 MP



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PROBLEMS

473

7.67 For the state of plane stress shown, determine the maximum shear-

ing stress when (a) s

5 0 and s

5 12 ksi, (b) s

5 21 ksi and

5 9 ksi. (Hint: Consider both in-plane and out-of-plane shearing

stresses.)

7.68 For the state of stress shown, determine the maximum shearing

stress when (a) s

5 40 MPa, (b) s

5 120 MPa. (Hint: Consider

both in-plane and out-of-plane shearing stresses.)

7.69 For the state of stress shown, determine the maximum shearing

stress when (a) s

5 20 MPa, (b) s

5 140 MPa. (Hint: Consider

both in-plane and out-of-plane shearing stresses.)

7.70 and 7.71 For the state of stress shown, determine the maximum

shearing stress when (a) s

5 14 ksi, (b) s

5 24 ksi, (c) s

5 0.

7.66 For the state of plane stress shown, determine the maximum shear-

ing stress when (a) s

5 6 ksi and s

5 18 ksi, (b) s

5 14 ksi

and s

5 2 ksi. (Hint: Consider both in-plane and out-of-plane

shearing stresses.)

8 ksi

Fig. P7.66 and P7.67

80 MPa

140 MPa

Fig. P7.68 and P7.69

6 ksi

7 ksi

2 ksi

Fig. P7.70

6 ksi

5 ksi

10 ksi

Fig. P7.71

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474

Transformations of Stress and Strain

7.72 and 7.73 For the state of stress shown, determine the maxi-

mum shearing stress when (a) s

5 0, (b) s

5 145 MPa, (c) s

245 MPa.

7.74 For the state of stress shown, determine two values of s

for which

the maximum shearing stress is 10 ksi.

75 MPa

100 MPa

20 MPa

Fig. P7.72

75 MPa

150 MPa

70 MPa

Fig. P7.73

8 ksi

14 ksi

Fig. P7.74

7.75 For the state of stress shown, determine two values of s

for which

the maximum shearing stress is 73 MPa.

7.76 For the state of stress shown, determine the value of t

for which

the maximum shearing stress is (a) 10 ksi, (b) 8.25 ksi.

48 MPa

50 MPa

Fig. P7.75

3 ksi

15 ksi

Fig. P7.76

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475

Problems

7.77 For the state of stress shown, determine the value of t

for which

the maximum shearing stress is (a) 60 MPa, (b) 78 MPa.

40 MPa

100 MPa

Fig. P7.77

7.78 For the state of stress shown, determine two values of s

for which

the maximum shearing stress is 80 MPa.

7.79 For the state of stress shown, determine the range of values of

for which the maximum shearing stress is equal to or less than

60 MPa.

*7.80 For the state of stress of Prob. 7.69, determine (a) the value of s

for which the maximum shearing stress is as small as possible,

(b) the corresponding value of the shearing stress.

7.81 The state of plane stress shown occurs in a machine component

made of a steel with s

5 325 MPa. Using the maximum-distortion-

energy criterion, determine whether yield will occur when (a) s

200 MPa, (b) s

5 240 MPa, (c) s

5 280 MPa. If yield does not

occur, determine the corresponding factor of safety.

7.82 Solve Prob. 7.81, using the maximum-shearing-stress criterion.

7.83 The state of plane stress shown occurs in a machine component

made of a steel with s

5 45 ksi. Using the maximum-distortion-

energy criterion, determine whether yield will occur when (a) t

9 ksi, (b) t

5 18 ksi, (c) t

5 20 ksi. If yield does not occur,

determine the corresponding factor of safety.

90 MPa

60 MPa

Fig. P7.78

Fig. P7.79

 100 MPa

60 MPa

100 MP

Fig. P7.81

7.84 Solve Prob. 7.83, using the maximum-shearing-stress criterion.

21 ksi

36 ksi

Fig. P7.83

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476

Transformations of Stress and Strain

7.85 The 36-mm-diameter shaft is made of a grade of steel with a 250-MPa

tensile yield stress. Using the maximum-shearing-stress criterion,

determine the magnitude of the torque T for which yield occurs

when P 5 200 kN.

7.86 Solve Prob. 7.85, using the maximum-distortion-energy criterion.

7.87 The 1.75-in.-diameter shaft AB is made of a grade of steel for which

the yield strength is s

5 36 ksi. Using the maximum-shearing-

stress criterion, determine the magnitude of the force P for which

yield occurs when T 5 15 kip ? in.

36 mm

Fig. P7.85

1.75 in.

Fig. P7.87

7.88 Solve Prob. 7.87, using the maximum-distortion-energy criterion.

7.89 a nd 7.90 The state of plane stress shown is expected to occur

in an aluminum casting. Knowing that for the aluminum alloy used

5 80 MPa and s

5 200 MPa and using Mohr’s criterion,

determine whether rupture of the casting will occur.

100 MPa

60 MPa

10 MP

Fig. P7.89

75 MPa

32 MP

Fig. P7.90

7.91 and 7.92 The state of plane stress shown is expected to occur

in an aluminum casting. Knowing that for the aluminum alloy used

5 10 ksi and s

5 30 ksi and using Mohr’s criterion, deter-

mine whether rupture of the casting will occur.

7 ksi

8 ksi

Fig. P7.91

9 ksi

15 ksi

2 ksi

Fig. P7.92

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