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16-Civ-B2 Advanced Structural Design · December 2017

Question 6 of 7: Limit states design of the reinforced concrete member ABC

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

Paper format. National Exams, December 2017, 16-Civ-B2 Advanced Structural Design — 3 hours, open book (design handbooks and textbooks permitted). Seven design questions of equal value; any five constitute a complete paper. All seven are solved here because the set is a study resource. Page 1 supplies the design data used throughout: concrete $f'_c = 30$ MPa; structural steel $F_y = 350$ MPa; rebar $f_y = 400$ MPa; prestressed concrete $f_{ci} = 35$ MPa at transfer, $f'_c = 50$ MPa, $n = 6$, $f_{ult} = 1750$ MPa, $f_{py} = 1450$ MPa, $f_{initial} = 1200$ MPa, losses $= 240$ MPa. Page 1 also states that all loads shown are unfactored.

Reference texts. CSA S16:19 Design of Steel Structures (Cl 8.5, 13.4, 13.6, 13.8, 14.3–14.6, 17); CISC Handbook of Steel Construction, 11th ed.; CSA A23.3:19 Design of Concrete Structures (Cl 9.8, 10, 11, 15, 18); CSA S6:19 Canadian Highway Bridge Design Code; Kulak & Grondin, Limit States Design in Structural Steel, 10th ed.; MacGregor & Bartlett, Reinforced Concrete: Mechanics and Design (Canadian ed.); Collins & Mitchell, Prestressed Concrete Structures.

Check: load factors. The paper states only that the loads are unfactored and gives no dead/live split. Throughout, the printed loads are taken as one variable-load case and factored by $1.5$, while self weight that the solver introduces (concrete frames, the prestressed girder, the bridge deck) is factored by $1.25$, per NBCC 2020 Table 4.1.3.2. The mechanisms, section classifications and interaction equations are unaffected by that choice; only the magnitudes scale.

Question 6: Limit states design of the reinforced concrete member ABC (14 + 6 marks)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Given. From Figure 5: an L-frame whose horizontal member A–B–C is built into a wall at A and spans $6 + 6 = 12$ m to joint C, from which a 10 m column runs down to a pinned base at D. Point loads of 400 kN act at B and 600 kN at C. Materials are $f'_c = 30$ MPa and $f_y = 400$ MPa.

QuantitySymbolValue
Beam A–B–C span$L$12 m (B at mid-span)
Column C–D height$h$10 m, pinned at D
Load at B / at C (unfactored)$P_B$ / $P_C$400 / 600 kN
Trial beam section$b \times h$500 × 1200 mm
Trial column section$b \times h$600 × 800 mm
Concrete / steel$f'_c$ / $f_y$30 / 400 MPa
Beam self weight$w$14.4 kN/m

Find. Flexural and shear reinforcement for member ABC, with a layout drawing.

400 kN 600 kN A B C D 6 m 6 m 10 m -1456 1178 -436 A C Beam moments (kN.m) sagging plotted downwards Figure 5 - L-frame; loads printed unfactored, moments factored
Figure 5: the horizontal member ABC is built in at A and propped at C by the 10 m column, which is pinned at D. Factored beam moments are shown alongside.

Approach. Analyse the twice-redundant frame by the force method using the Cl 10.14.1.2 cracked-section stiffnesses, take the envelope of hogging and sagging moments and the peak shear, then proportion the section with the rectangular stress block and detail the stirrups.

  1. Factor the loads. $$\begin{gathered}P_B = 1.5(400) = 600\ \text{kN}, \\ P_C = 1.5(600) = 900\ \text{kN}, \\ w = 1.25(14.4) = 18.0\ \text{kN/m}.\end{gathered}$$ The 900 kN at C acts directly over the column and does no work on the beam except through the joint.
  2. Set up the analysis. A is fully fixed (3 restraints) and D is pinned (2), so with three equations of equilibrium the frame is twice redundant. Cl 10.14.1.2 gives the stiffnesses to use in a frame analysis: $0.35I_g$ for the beam and $0.70I_g$ for the column, i.e. $$I_b = 0.35\frac{500(1200)^3}{12} = 2.52\times10^{10},\qquad I_c = 0.70\frac{600(800)^3}{12} = 1.792\times10^{10}\ \text{mm}^4 .$$
  3. Solve for the redundants. Releasing the horizontal and vertical reactions at D and applying the unit-load method over both members gives $$\begin{gathered}V_D = 1222.9\ \text{kN}, \\ H_D = 43.6\ \text{kN}, \\ V_A = 493.1\ \text{kN}.\end{gathered}$$ Because the column base is pinned, the horizontal reaction is simply the column shear, $H = |M_C|/h$.
  4. Design moments and shear. The resulting beam diagram is $$\begin{gathered}M_A = -1456\ \text{kN}\cdot\text{m}\ \text{(hogging)}, \\ M_B = +1178\ \text{kN}\cdot\text{m}\ \text{(sagging)}, \\ M_C = -436\ \text{kN}\cdot\text{m},\end{gathered}$$ with the maximum shear $V_f = 493.1$ kN at A. The value at A sits between the propped-cantilever bound (1674 kN·m, a pin at C) and the fixed-fixed bound (1116 kN·m, a rigid support at C), as it must — the column supplies partial rotational restraint.
  5. Effective depth. With 40 mm cover, 10M stirrups and 30M bars, $$d = 1200 - 40 - 11.3 - \tfrac{29.9}{2} = 1134\ \text{mm}.$$
  6. Flexural steel at A. Solving $\phi_s A_s f_y(d - a/2) = M_f$ with $a = \phi_s A_s f_y/(\alpha_1\phi_c f'_c b)$ and $\alpha_1 = 0.805$: $$A_s = 4099\ \text{mm}^2 \;\Rightarrow\; \boxed{\text{6 – 30M top}} \ (4200\ \text{mm}^2).$$ Then $a = 181.9$ mm, $c/d = 0.179 \ll 0.5$, so the section is comfortably tension-controlled, and $M_r = 1489$ kN·m against $M_f = 1456$ kN·m. Six 30M bars fit in one layer: they need $6(29.9) + 5(42) = 389$ mm against the 400 mm clear width.
  7. Flexural steel at B and at C. The same solve gives $A_s = 3259$ mm$^2$ at B, so provide 5 – 30M bottom ($3500$ mm$^2$, $M_r = 1259$ kN·m). At C the demand is only $A_s = 1155$ mm$^2$, below the minimum $$A_{s,min} = \frac{0.2\sqrt{f'_c}}{f_y}b_t h = \frac{0.2\sqrt{30}}{400}(500)(1200) = 1643\ \text{mm}^2,$$ so minimum steel governs: provide 3 – 30M top ($2100$ mm$^2$) across the joint and anchor it into the column.
  8. Shear. With $d_v = \max(0.9d, 0.72h) = 1020$ mm and the simplified method ($\beta = 0.18$, $\theta = 35^\circ$), $$V_c = \phi_c\lambda\beta\sqrt{f'_c}\,b_w d_v = 0.65(0.18)\sqrt{30}(500)(1020)/10^3 = 327\ \text{kN},$$ so the stirrups must carry $V_s = 493.1 - 327 = 166$ kN. Ten-millimetre double-leg stirrups ($A_v = 200$ mm$^2$) would satisfy strength at $$s = \frac{\phi_s A_v f_y d_v \cot\theta}{V_s} = 597\ \text{mm}.$$
  9. Detailing limits govern the stirrup spacing. Because $V_f = 493$ kN is far below $0.125\phi_c f'_c b_w d_v = 1244$ kN, Cl 11.3.8.1 caps the spacing at $\min(0.7d_v, 600) = 600$ mm; but the minimum-shear- reinforcement rule $A_v \ge 0.06\sqrt{f'_c}\,b_w s/f_y$ caps it at 487 mm. Adopt $$\boxed{\text{10M double-leg stirrups at 450 mm throughout}},$$ tightened to 250 mm over the first 1.5 m from A where the shear is largest.
6-30M top 3-30M top 5-30M bottom 10M double-leg stirrups @ 450 mm A C 500 mm 1200 Section at A Reinforcement layout for member ABC
Reinforcement layout for member ABC: 6-30M top at A, 5-30M bottom through the span, 3-30M top at C, with 10M double-leg stirrups.
QuantityValue
Beam section500 × 1200 mm, $d = 1134$ mm
Factored moments $M_A$ / $M_B$ / $M_C$−1456 / +1178 / −436 kN·m
Maximum shear493.1 kN at A
Top steel at A6 – 30M ($A_{s,req} = 4099$ mm$^2$), $M_r = 1489$ kN·m
Bottom steel at B5 – 30M ($A_{s,req} = 3259$ mm$^2$), $M_r = 1259$ kN·m
Top steel at C3 – 30M (minimum steel, 1643 mm$^2$, governs)
$c/d$ at A0.179 — tension-controlled
Concrete shear resistance$V_c = 327$ kN
Stirrups10M double leg at 450 mm (250 mm near A)