Theory of Structures + Stability of Structures
February 4th, 2021(the solution should be delivered within February 4th, 2021, h. 13:00)
Theory of Structures
Problem T1
The problem is referred to a parabolic arch, whose geometry is depicted in the figure. The material is homogeneous (E = 30 GPa, v = 0.2) and the keystone section is square (side length 150 cm). The variation of the cross-section properties with respect to the arch inclination is A = A0/cos α, I = I0/cos α, where A0 and I0 are the keystone cross-section area and inertia, respectively. The external load is represented by a concentrated force (P = 150 kN). The student should solve the problem by making use of symbolic variables and, finally, should obtain the numerical values of the reaction forces and the diagrams of shear, axial force and bending moment.
Problem T2
The above figure represents a multi-cellular section with uniform thickness 50 mm (all the measurements are in mm). The students should obtain the stress field for a shear force V = 200 kN, applied in the upper left corner of the middle line. Moreover, the position of the shear center should be computed. G = 18 GPa.
Theory of Structures + Stability of Structures
February 4th, 2021
(the solution should be delivered within February 4th, 2021, h. 13:00)
Theory of Structures
Problem T1
The problem is referred to a parabolic arch, whose geometry is depicted in the figure. The material is homogeneous (E = 30 GPa, ν = 0.2) and the keystone section is square (side length 150 cm). The variation of the cross-section properties with respect to the arch inclination is A = Ao/cos α, I = Io/cos α, where Ao and Io are the keystone cross-section area and inertia, respectively. The external load is represented by a concentrated force (P = 150 kN). The student should solve the problem by making use of symbolic variables and, finally, should obtain the numerical values of the reaction forces and the diagrams of shear, axial force and bending moment.
Problem T2
The above figure represents a multi-cellular section with uniform thickness 50 mm (all the measurements are in mm). The students should obtain the stress field for a shear force V = 200 kN, applied in the upper left corner of the middle line. Moreover, the position of the shear center should be computed. G = 18 GPa.
THEORY OF STRUCTURES
PROBLEM T1
P = 150 kN
- REDUNDANT STRUCTURE:
- Add a redundant action in B substituting the hinge with a roller
- CASE 0: external load:
HAO = 0
Focus on a part:
Equilibrium
∑H = 0: HAO = 0
∑V = 0: VAO + VBO = P → VAO = 3/4 P
∑MA = 0: VBO L - P e/4 = 0 → VBO = P/4
Check ∑MB = 0: 3/4 PL - P. 3/4 e = 0 ✓
No = ∫ - 3/4 P sen α, z < e/4
(3/4 P + P) sen α, z ≥ e/4
To = ∫ - 3/4 P cos α, z < e/4
(1/4 P + P) cos α, z ≥ e/4
Mo = ∫ 3/4 P z z < e/4
[3/4 P z - P(z - e/4)] z ≥ e/4
3) CASE 1: Horizontal unitary thrust x̅ = 1
EQUILIBRIUM
∑H=0: HA1 - 1
∑V=0: VA1 + VB1 = 0
VA1 = VB1 = 0
Focus on a part
N1 = 1cosα
T1 = -1senα
M1 = 1·y
4) PRINCIPLE OF VIRTUAL WORK:
Le = 1 · δHB
because, since in real structure we have an hinge in B, we can't have any horizontal displacement.
Li = ∫ξξ (Nt Mt It t + Mt xt) ds
FOR AN ARCH:
- M = NRED / EA
- t = I / GAmod
- χ = M / EIred - Nred / REA
where
- Nred = reduced axial
- Amod = modified area
- Ired = reduced inertia
IF B/R < 0.10, arch is sufficiently slender:
R(z) = [1+(y'(z))2]3/2 / |y''(z)|
R / Rmin = 0.275 < 0.10 →
Rmin = R(z - ξ/2) = [1+0]3/2 / | - δ / ξ2
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