Question 7 of 7: C1 — Glulam column under dead, live and wind loads
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. National Examinations, May 2018 — 16-Civ-A2 Elementary Structural Design. Three hours, CLOSED BOOK (handbooks and textbooks permitted). Seven questions in three parts: Part A (A1–A3, steel), Part B (B1–B3, reinforced concrete), Part C (C1, timber). A candidate submits five solutions — two from Part A, two from Part B and the one question in Part C — all of equal value. All seven questions are solved below, because this set is a study resource rather than an exam script. Page 1 states that all loads shown are unfactored, so every load case is factored here before any resistance is compared against it.
Reference texts.
CSA S16:19, Design of Steel Structures — and CISC, Handbook of Steel Construction, 11th ed. (section tables, Table 2 class limits, Table 7 minimum fillet sizes).
CSA A23.3:19, Design of Concrete Structures — and Cement Association of Canada, Concrete Design Handbook, 4th ed.
CSA O86:19, Engineering Design in Wood — and Canadian Wood Council, Wood Design Manual.
Kulak & Grondin, Limit States Design in Structural Steel, 11th ed., Chs. 4, 5, 8, 9.
National Building Code of Canada 2015, Table 4.1.3.2 (load combinations).
Check — one dimension is missing from the source. Question A2 describes a stub cantilever welded to a column but the paper contains no Figure A2 and never states the cantilever projection. The projection is therefore taken as L = 1.5 m from the column face throughout question A2; every result below is also given in the general form so any other projection can be substituted directly. All other data are read from the printed text and from Figure A3, B1, B2 and B3 on page 3.
Question 7: C1 — Glulam column under dead, live and wind loads (8 + 6 + 6 marks)
fb = 25.6, fc = 25.2, fv = 1.75 MPa; E = 10 300, E05 = 8600 MPa
Height, L
5.0 m, pin-ended, restrained in the weak direction
Axial loads (specified)
10 kN dead + 35 kN live
Wind
10 kN concentrated at mid-height
Service conditions
dry, untreated: KS = KT = KH = 1.0
Find. Pf, Pr, Mf and Mr for the dead-plus-live-plus-wind case, and the resulting interaction check.
Figure 7.1 — Glulam column: axial load at the head, wind as a point load at mid-height bending the member about its strong (228 mm) axis.
Approach. Form the NBCC load combinations that contain all three loads, take the governing one, compute the compressive and bending resistances with the appropriate duration factor, then apply the O86 combined-loading interaction.
Load combinations (NBCC 2015 Table 4.1.3.2). Two combinations contain dead, live and wind together:
Both are evaluated below; Case 4, with wind as the principal load, proves to govern by a wide margin. The moment comes from a central point load on a pin-ended member, M = WL/4.
Section properties and duration factor. A = 130(228) = 29 640 mm2, S = bd2/6 = 1.126 × 106 mm3, I = bd3/12 = 128.4 × 106 mm4. With wind as the principal load the duration factor is KD = 1.15, so the factored strengths are
$$F_{c}=f_{c}K_{D}=25.2(1.15)=28.98\ \text{MPa},\qquad F_{b}=f_{b}K_{D}=25.6(1.15)=29.44\ \text{MPa}$$
Compressive resistance (O86 Cl. 7.5.8). The column is restrained in the weak direction, so buckling can only occur about the strong axis and the slenderness ratio uses the 228 mm dimension:
$$C_{c}=\frac{L_{e}}{d}=\frac{5000}{228}=21.9\ \ (\le 50)$$
The size factor for glulam in compression uses the member volume Z = 0.130(0.228)(5.0) = 0.148 m3:
$$K_{Zcg}=0.68Z^{-0.13}=0.68(0.148)^{-0.13}=0.872$$
$$K_{c}=\left[1+\frac{F_{c}K_{Zcg}C_{c}^{3}}{35E_{05}}\right]^{-1}=\left[1+\frac{28.98(0.872)(10\,545)}{35(8600)}\right]^{-1}=0.531$$
$$P_{r}=\phi F_{c}AK_{Zcg}K_{c}=0.80(28.98)(29\,640)(0.872)(0.531)=\boxed{318\ \text{kN}}$$
Bending resistance (O86 Cl. 7.5.6). Because the member is restrained in the weak direction, lateral-torsional buckling is prevented and KL = 1.0. The bending size factor
$$K_{Zbg}=\left(\frac{130}{b}\right)^{0.1}\left(\frac{610}{d}\right)^{0.1}\left(\frac{9100}{L}\right)^{0.1}=1.17\ \Rightarrow\ \text{taken as }1.0$$
so the resistance is governed by strength:
$$M_{r}=\phi F_{b}SK_{Zbg}K_{L}=0.90(29.44)(1.126\times10^{6})=\boxed{29.8\ \text{kN}\cdot\text{m}}$$
Combined loading (O86 Cl. 7.5.12). The Euler load about the bending axis is
$$P_{E}=\frac{\pi^{2}E_{05}I}{L_{e}^{2}}=\frac{\pi^{2}(8600)(128.4\times10^{6})}{5000^{2}}=436\ \text{kN}$$
and the interaction equation for a glulam member in combined bending and compression is
$$\left(\frac{P_{f}}{P_{r}}\right)^{2}+\frac{M_{f}}{M_{r}\left(1-\dfrac{P_{f}}{P_{E}}\right)}\le 1.0$$
$$\left(\frac{30.0}{318}\right)^{2}+\frac{17.5}{29.8\left(1-\dfrac{30.0}{436}\right)}=0.009+0.630=\boxed{0.64\ \le 1.0}$$
Check the companion combination. For Case 3 the duration factor drops to KD = 1.0, giving Pr = 294 kN and Mr = 26.0 kN·m against Pf = 65.0 kN and Mf = 5.0 kN·m, so the interaction returns 0.049 + 0.226 = 0.28. Case 4 therefore governs, and the higher KD of the wind case does not offset the far larger moment.
The column is adequate, working at 64 % of capacity, and the result is overwhelmingly a bending problem: the axial term contributes barely 1 % of the unity check because it enters squared and the applied load is under a tenth of Pr. Reducing the depth would be the first economy to explore, but 228 mm is already close to the minimum that keeps the interaction below unity.