Week 1-3 slides
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Transcript of Week 1-3 slides
Mechanics of Solids
Internal Resultant Loadings
Example Determine the resultant internal loadings at D, E and F.
4 kN
4 kN
4 kN
D
E
F
B
A
1.2 m 1.2 m
1.8 m
1.8 m
D:
Free-body diagram D
ND
MB_D
VD
x
y
Equations of equilibrium
VD = 0
ND = 0
MB_D = 0
C
D
Internal resultant loadings
F:
Free-body diagram
Equations of equilibrium 4 kN
4 kN
4 kN
D
E
F
B
A
1.2 m 1.2 m
1.8 m
1.8 m
NF
MB_F
VF
4 kN
4 kN
4 kN
F
B
A
x
y
VF = 0
FFy – 4 – 4 – 4 = 0 NF =12 kN
MB_F – 4 x 1.2 – 4 x 1.2 + 4 x 1.2 = 0 MB_F = 4.8 kN m
C
Example Determine the resultant internal loadings at D, E and F.
F
Internal resultant loadings
E:
Free-body diagram
Equations of equilibrium 4 kN
4 kN
4 kN
D
E
F
B
A
1.2 m 1.2 m
1.8 m
1.8 m
NE
ME
VE
E
A
x
y
FAy
FAx (Support reactions)
C
4 kN
4 kN 4 kN
B
A
C
A:
F’Ay
F’Ax
FCy
FCx
x
y
F’Ax + FCx = 0
F’Ay + Fcy – 12 = 0
F’Ax = - FCx
MAC – 4 x 1.2 – 4 x 1.2 + 4 x 1.2 = 0 MAC = Fax x 1.8
MAC = 4.8 kN m F’Ax = - 2.67 kN
Example Determine the resultant internal loadings at D, E and F.
C
Internal resultant loadings
D
E:
Free-body diagram
Equations of equilibrium 4 kN
4 kN
4 kN
D
E
F
B
A
1.2 m 1.2 m
1.8 m
1.8 m
NE
MB_E
VE
E
A
x
y
FAy
FAx (Support reactions)
C
4 kN
4 kN
B
A
A:
F’Ay
F’Ax FBy
FBx x
y
F’Ay x 1.2 – (-2.67 x 0.9) – 4 x 2.4 = 0
F’Ay = 6 kN
F’Ax = - 2.67 kN
FAy = - F’Ay = - 6 kN
FAx = - F’Ax = 2.67 kN
F’Ax = - 2.67 kN
Example Determine the resultant internal loadings at D, E and F.
B
Internal resultant loadings
Internal resultant loadings
E:
Free-body diagram
Equations of equilibrium 4 kN
4 kN
4 kN
D
E
F
B
A
1.2 m 1.2 m
1.8 m
1.8 m
NE
MB_E
VE
E
A
x
y
FAy
FAx (Support reactions)
C
FAy = - F’Ay = - 6 kN
FAx = - F’Ax = 2.67 kN
VE + FAx = 0
NE + FAy = 0 NF = 6 kN
MB_E – 2.67 x 0.9 = 0 MB_E = 2.4 kN m
VE = - 2.67 kN
Example Determine the resultant internal loadings at D, E and F.
a
a
Internal resultant loadings
Fx : Shear Force (V)
3-D
Mx : Bending Moment
FZ : Normal Force (N)
Fy : Shear Force (V)
My: Bending Moment
Mz : Torsional Moment or torque (T)
Mechanics of materials: external loads and intensity of internal forces F1
F2
a
a
z
y
x
o
Mz
My
Fx
Fy
Mx
Fz
F1
F2
Mechanics of Solids
Stress
Stress
Stress: the intensity of the internal force on a specific plane passing through a point
The material is continuous (no voids) and cohesive (no cracks, breaks and defects)
Shear Stress, τ,
Normal Stress, σ Tensile Stress:
Compressive Stress:
[MPa]
Stress
Stress: the intensity of the internal force on a specific plane passing through a point
The material is continuous (no voids) and cohesive (no cracks, breaks and defects)
Average Normal Stress: (Uniform Uniaxial Stress) a
a
a-a
A
The beam is prismatic bar.
σ
F
Average Shear Stress:
Stress
When the stress (intensity of force) of an element exceeds some level, the structure will fail. For convenience, we usually adopt allowable force or allowable stress to measure the threshold of safety in engineering.
Stress: the intensity of the internal force on a specific plane passing through a point
An 80 kg lamp is supported by a single electrical copper cable. if the maximum allowable stress for copper is σCu,allow=50MPa, please determine the minimum size of the wire/cable from the material strength point of view.
σ ≤ σallow
Stress
Factor of Safety, F.S., a ratio of failure load Ffail (found from experimental testing) divided by the allowable one Fallow
Uniform uniaxial stress,
An 80 kg lamp is supported by a single electrical copper cable. if the maximum allowable stress for copper is σCu,fail=50MPa, and the factor of safety of 2 it be achieved, please determine the minimum size of the wire/cable from the material strength point of view.
σCu,allow= σCu,fail/F.S. = 25 MPa
Stress Analysis Engineering Design
Stress
1-71 w = 2.5 kN/m. Member AB has a square cross section of 12 mm. Determine the average normal stress and average shear stress acting at sections a-a and b-b. (p. 45)
w
C
A
b
b
1.2 m B 60o