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stress transformation and mohr's circle - Foundation Coalition

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124 CHAPTER 5. STRESS TRANSFORMATION AND MOHR’S CIRCLE<br />

y-face<br />

(0,0)<br />

σ x ′ y ′<br />

B<br />

C<br />

2.5<br />

5MPa<br />

x-face<br />

z<br />

2.5<br />

y<br />

2.5<br />

σ x ′ x ′<br />

Figure 5.22:<br />

• Maximum shear traction at 45 ◦ from x-axis<br />

• Maximum normal traction along x-axis<br />

Example 5-6<br />

x<br />

45<br />

C B<br />

σxx<br />

σ x ′ x ′ = σn =2.5<br />

σ x ′ y ′ = τ s =2.5<br />

Given: The state of <strong>stress</strong> at each point in a bar can be represented by the <strong>stress</strong> tensor [σ]:<br />

Required :<br />

⎡<br />

[σ] = ⎣<br />

z<br />

σxx 0 0<br />

0 0 0<br />

0 0 0<br />

y<br />

⎤ ⎡<br />

⎦ = ⎣<br />

x<br />

Figure 5.23:<br />

a) Construct Mohr’s Circle for the given <strong>stress</strong> tensor.<br />

10 kN<br />

m 2 0 0<br />

0 0 0<br />

0 0 0<br />

b) What are the traction vectors experienced each face of the cube?<br />

⎤<br />

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