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The stresses shown in the figure act at a point in a stressed body. Using the equilibrium equation approach, determine the normal and shear stresses at this point on the inclined plane shown. 12.1
Fig. P12.1 Solution Σ Fn = σ n dA − (215 σ n
189.10 1021 21 MPa MPa = = 189.
Σ Ft = τ nt dA + ( 215 τ nt
MPa) co cos 25 25°(dA cos 25 25° ) − (70 MPa) sin 25 25° (dA sin 25 25° ) = 0
= −55.5382
189. 189.1 1 MPa (T)
Ans.
MPa) sin 25 25°(dA cos 25 25° ) − (70 MPa) cos 25 25° (dA sin 25 25° ) = 0
MP MPa =
− 55.5
MPa
Ans.
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The stresses shown in the figure act at a point in a stressed body. Using the equilibrium equation approach, determine the normal and shear stresses at this point on the inclined plane shown. 12.2
Fig. P12.2 Solution
000 Σ Fn = σ n dA + (3, 00 σ n
,061.902 022 2 = 1,061.9
psi psi = 1,062 psi psi (T)
Σ Ft = τ nt dA + (3, 00 000 τ nt
psi) co cos 70 70°(dA cos 70 70° ) − (1, 60 600 psi) si sin 70 70° (dA sin 70 70° ) = 0
,478.4115 = −1,478
Ans.
psi) si sin 70 70°(dA cos 70 70°) + (1, 60 600 psi) co cos 70 70° (dA sin 70 70° ) = 0
psi =
,478 − 1,478
psi
Ans.
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The stresses shown in the figure act at a point in a stressed body. Using the equilibrium equation approach, determine the normal and shear stresses at this point on the inclined plane shown. 12.3
Fig. P12.3 Solution Σ Fn = σ n dA − (190 σ n
= −20.7197
MP MPa = 20.7 MP MPa (C (C)
Σ Ft = τ nt dA − (190 τ nt
=
MP MPa) co cos 40 40° (dA cos 40 40° ) + (320 MP MPa) sin 40 40° (dA sin 40 40° ) = 0 Ans.
MP MPa) sin 40 40°(dA cos 40 40°) − (320 MP MPa) co cos 40 40° (dA sin 40 40° ) = 0
251.1260 MPa = 251 MPa
Ans.
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The stresses shown in the figure act at a point in a stressed body. Using the equilibrium equation approach, determine the normal and shear stresses at this point on the inclined plane shown. 12.4
Fig. P12.4 Solution Σ Fn = σ n dA + ( 21.0 σ n
15.296 964 4 = −15.2
ksi ksi = 15.3 15.30 0 ksi ksi (C)
Σ Ft = τ nt dA − ( 21.0 τ nt
= 3.9937
ks ksi) co cos 55 55°(dA cos 55 55° ) + (12.5 ksi) sin 55 55° (dA sin 55 55° ) = 0 Ans.
ks ksi) sin 55 55°(dA cos 55 55°) + (12.5 ksi) co cos 55 55° (dA sin 55 55° ) = 0
ks ksi = 3.99 ks ksi
Ans.
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The stresses shown in the figure act at a point in a stressed body. Using the equilibrium equation approach, determine the normal and shear stresses at this point on the inclined plane shown. 12.5
Fig. P12.5 Solution Σ Fn = σ n dA − (270 −(125 σ n
= 310.7 0.7532
MPa) sin 30 30°(dA cos 30°) − (125 MPa) co cos 30 30° (dA sin 30 30° ) = 0 MPa = 311 MPa (T)
Σ Ft = τ nt dA + ( 270 −(125 τ nt
= −54.4134
MPa) co cos 30 30° (dA cos 30 30° )
Ans.
MPa) si sin 30 30°(dA cos 30 30°)
MPa) co cos 30 30° (dA cos 30 30° ) + (125 MPa) sin 30 30° (dA sin 30 30° ) = 0 MPa =
− 54.4
MPa
Ans.
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The stresses shown in the figure act at a point in a stressed body. Using the equilibrium equation approach, determine the normal and shear stresses at this point on the inclined plane shown. 12.6
Fig. P12.6 Solution
300 Σ Fn = σ n dA − (2, 30 + ( 400 σ n
.7089 = 984.70
psi) sin 55 55°(dA cos 55°) + (400 psi) cos 55°(dA sin 55 55° ) = 0 ps psi = 985 985 ps psi (T)
300 Σ Ft = τ nt dA + ( 2, 30 + ( 400 τ nt
= −520.9768
psi) co cos 55 55°(dA cos 55 55° ) − (900 psi) si sin 55 55° (dA sin 55 55° )
Ans.
psi) si sin 55 55°(dA cos 55 55°) − (900 psi) co cos 55 55° (dA sin 55 55° )
ps psi) co cos 55°(dA cos 55° ) − (400 ps psi) sin 55 55° (dA sin 55 55° ) = 0
psi =
− 521 psi
Ans.
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The stresses shown in the figure act at a point in a stressed body. Using the equilibrium equation approach, determine the normal and shear stresses at this point on the inclined plane shown. 12.7
Fig. P12.7 Solution Σ Fn = σ n dA − (35 + ( 25 σ n
=
MPa) sin 75 75°(dA cos 75° ) + (25 MPa) cos 75° (dA sin 75 75° ) = 0
20.15 .1554 MPa = 20.2 MPa (T)
Σ Ft = τ nt dA + (35 −( 25 τ nt
MP MPa) si sin 75 75°(dA sin 75 75°)
= −30.4006
Ans.
MP MPa) co cos 75 75°(dA sin 75 75°)
MPa) cos 75 75°(dA cos 75° ) + (25 MP MPa) sin 75 75° (dA sin 75 75° ) = 0 MPa =
− 30.4
MPa
Ans.
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The stresses shown in the figure act at a point in a stressed body. Using the equilibrium equation approach, determine the normal and shear stresses at this point on the inclined plane shown. 12.8
Fig. P12.8 Solution Σ Fn = σ n dA + (7.4 −(9.3 σ n
ksi) sin 25 25°(dA cos 25 25°) − (9.3 ksi) cos 25 25° (dA sin 25 25° ) = 0
.6535 = 3.65
ks ksi = 3.65 ks ksi (T)
Σ Ft = τ nt dA + (7.4 + (9.3 τ nt
= −14.4044
ksi) co cos 25 25°(dA cos 25 25° ) − (14.6 ksi) si sin 25 2 5° (dA sin 25 2 5° )
Ans.
ksi) si sin 25 2 5°( dA cos 25 25°) + (14.6 ksi) co cos 25 25° (dA sin 25 2 5° )
ksi) cos 25 25°(dA cos 25 25°) − (9.3 ksi) sin 25 25°(dA sin 25 25° ) = 0 ks ksi =