Question 2 of 7: A2 — Moments of resistance of a built-up plate section
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. National Examinations, May 2017 — 16-Civ-A2 Elementary Structural Design. Three hours, closed book (handbooks and textbooks permitted). Seven questions in three parts: Part A (A1–A3, structural steel to CSA S16), Part B (B1–B3, reinforced concrete to CSA A23.3) and Part C (C1, timber to CSA O86). A candidate answers two from Part A, two from Part B and the one question in Part C — five solutions of equal value. All seven are solved here, because the set is a study resource rather than a sitting.
Reference texts.
CSA S16:19, Design of Steel Structures — Clauses 11 (section class), 13.3 (compression), 13.5 (bending), 13.8 (axial force and bending), 13.13 (welds), 14.3 (concentrated forces).
CISC, Handbook of Steel Construction — rolled-section dimensions and properties, weld tables.
CSA A23.3:19, Design of Concrete Structures — Clauses 10 (flexure and axial load), 11 (shear).
CSA O86:19, Engineering Design in Wood — Clause 6 (sawn lumber), Tables 6.3.1B and 6.4.5.
Canadian Wood Council, Wood Design Manual; National Building Code of Canada 2020 (load combinations).
Load factors. NOTE 6 on page 1 states that all loads shown are unfactored. The point loads drawn on Figures A1, B1 and B2 are occupancy loads, so they are factored by 1.5; the only dead load anywhere in this paper is the concrete self-weight of the Question B2 beam, which takes 1.25. This follows NBCC combination 2, 1.25D + 1.5L.
Check — figure page. Two figure readings are flagged where they arise: in Figure B1 the 350 kN load acts at midspan of beam BA (3.5 m from B), not at joint B; and the 80 kN horizontal load acts 4 m below B, i.e. 6 m above the pin at C.
Question 2: A2 — Moments of resistance of a built-up plate section (8 + 12 marks)
Given. From the figure, all plates 25 mm thick, G40.21-350W (Fy = 350 MPa):
Element
Size (mm)
Area (mm2)
Position
Top flange
600 × 25
15 000
300 + 300 about the y–y centreline
Webs (2)
25 × 250
12 500
at x = ±200 mm (100 + 400 + 100 = 600)
Bottom flanges (2)
200 × 25
10 000
centred on each web
Overall depth
300
37 500
25 + 250 + 25
Find.Mrx and Mry, the factored moments of resistance of the cross-section about its two centroidal axes.
Figure A2 — built-up section from 25 mm plates; C is the elastic centroid.
Approach. Locate the elastic centroid, compute Ix and Iy, classify every plate element under S16 Table 2, then — the section being Class 1 — find each plastic modulus from the equal-area axis and take Mr = φZFy.
Locate the centroid. Measuring y upward from the underside of the bottom flanges,
$$\bar{y} = \frac{10\,000(12.5) + 12\,500(150) + 15\,000(287.5)}{37\,500} = \boxed{168.3\ \text{mm}}$$
so the x–x axis sits 168.3 mm above the bottom and 131.7 mm below the top. The section is symmetric about y–y, so that axis is the vertical centreline.
Second moments of area. Summing Iown + Ad2 over the five plates,
$$I_x = 526.5\times10^{6}\ \text{mm}^{4}, \qquad I_y = 1384.0\times10^{6}\ \text{mm}^{4}$$
This is the first thing to notice about the section: it is wide and shallow, so Iy is 2.6 times Ix and y–y is the strong axis, not x–x. The corresponding radii of gyration are rx = 118.5 mm and ry = 192.1 mm, both needed in Question A3.
Classify the elements. With √Fy = 18.71, the Class 1 limits of S16 Table 2 are 145/√Fy = 7.75 for a flange outstand, 525/√Fy = 28.1 for a plate supported on both edges in uniform compression, and 1100/√Fy = 58.8 for a web in flexure. The actual ratios are
Element
b/t or h/w
Class 1 limit
Top-flange outstand past a web, 87.5/25
3.5
7.75
Top flange between the webs, 375/25
15.0
28.1
Web, 250/25
10.0
58.8
Bottom-flange outstand, 87.5/25
3.5
7.75
Every element is comfortably Class 1, so the full plastic moment may be used about both axes.
Locate the plastic neutral axis for x–x. The plastic axis divides the section into equal areas, not equal first moments. Half the area is 18 750 mm2; the two bottom flanges supply 10 000 mm2, and the two webs then supply 50 mm2 for every millimetre of height:
$$y_p = 25 + \frac{18\,750 - 10\,000}{2 \times 25} = \boxed{200\ \text{mm from the bottom}}$$
This sits 31.7 mm above the elastic centroid — the two axes coincide only in a doubly symmetric section.
Plastic modulus about x–x. Taking each part's area times the distance from its own centroid to yp,
$$Z_x = 10\,000(187.5) + 8750(87.5) + 3750(37.5) + 15\,000(87.5) = \boxed{4.094\times10^{6}\ \text{mm}^{3}}$$
Plastic modulus about y–y. Symmetry puts the plastic axis on the centreline, so
$$Z_y = 2(7500)(150) + 2(6250)(200) + 2(5000)(200) = \boxed{6.750\times10^{6}\ \text{mm}^{3}}$$
Moments of resistance. The question asks for the resistance of the cross-section, so no lateral-torsional reduction applies:
$$M_{rx} = \phi Z_x F_y = 0.90 \times 4.094\times10^{6} \times 350 = \boxed{1290\ \text{kN}\cdot\text{m}}$$
$$M_{ry} = \phi Z_y F_y = 0.90 \times 6.750\times10^{6} \times 350 = \boxed{2126\ \text{kN}\cdot\text{m}}$$
Sanity-check with the elastic moduli.Sx = 526.5×106/168.3 = 3.128×106 mm3 to the bottom fibre and Sy = 1384.0×106/300 = 4.613×106 mm3, giving shape factors of 1.31 and 1.46. Both are far above the 1.12 typical of a rolled I-shape, which is exactly what one expects when so much of the area sits close to the neutral axis.