Question 5 of 7: B2. Design of column CD (4 + 4 + 12 marks)
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. National Examinations, May 2014 — 98-Civ-A2
Elementary Structural Design, 3 hours, closed book (handbooks and textbooks permitted).
Seven questions in three parts: Part A (A1–A3, steel), Part B (B1–B3, reinforced concrete)
and Part C (C1, timber). The candidate answers two from Part A, two from Part B and the single
Part C question — five solutions in all, of equal value. All seven are solved here,
because the set is intended as a study resource. Page 1 states that
all loads shown are unfactored, so the load factors are applied below rather than assumed
to be built in.
CISC, Handbook of Steel Construction — section property tables and the standard
beam load/moment diagrams referenced by Question A1.
CSA A23.3, Design of Concrete Structures — Clauses 10 (flexure and axial load) and
11 (shear, simplified method).
CSA O86, Engineering Design in Wood — Clause 6 (sawn lumber), Tables 6.3.1B
(Beam and Stringer specified strengths) and 6.4.2 (service-condition factors).
National Building Code of Canada — load combinations
1.25D + 1.5L.
Check: the figures on page 3 of the paper are hand-drawn; every dimension, support type and load below was read from the printed figures. The 300 kN, 250 kN, 300 kN and 80 kN forces are treated as
live load (factor 1.5) because the paper labels them only as unfactored applied loads;
concrete self-weight is the sole dead load and carries 1.25.
Question 5 — B2. Design of column CD (4 + 4 + 12 marks)
Figure B1 — determinate reinforced concrete frame: roller at A, internal hinge at B, rigid joint at C, fixed base at D. Loads shown are unfactored.
Given.
Quantity
Value
Column
CD, 6.0 m high, fixed at D, rigidly connected to beam ABC at C
Horizontal load
80 kN unfactored, at mid-height (3 m above D)
Actions from Question B1
beam end shear 233.1 kN, beam end moment 653.6 kN·m
Joint load
300 kN unfactored applied directly at C
Materials
$f_c' = 35$ MPa, $f_y = 400$ MPa; column assumed short (no magnification)
Find. Cross-sectional dimensions, longitudinal steel and ties for column CD.
Approach. Assemble the axial force and the moment diagram down the column from
the beam-end actions plus the mid-height horizontal load, design at the base where the moment peaks,
and check the chosen symmetric section by strain compatibility at the actual axial load.
Axial load on the column. The column carries the 450 kN factored load applied at
the joint, the 233.1 kN beam end shear, and its own weight. Trying a 500 mm × 800 mm section,
$$P_f = 450 + 233.1 + 1.25(24)(0.5)(0.8)(6.0) = 755.1\ \text{kN}$$
Moment diagram down the column. The rigid joint at C delivers the beam's hogging
moment of 653.6 kN·m into the column top. Below that, the 120 kN factored horizontal load at
mid-height adds a further $120(3.0)$ kN·m by the time the base is reached:
$$M_{top} = 653.6\ \text{kN}\cdot\text{m}, \qquad
M_{base} = 653.6 + 120(3.0) = 1\,013.6\ \text{kN}\cdot\text{m}$$
$$\boxed{P_f = 755.1\ \text{kN}, \qquad M_f = 1\,013.6\ \text{kN}\cdot\text{m at D}}$$
The eccentricity is $M_f/P_f = 1\,342$ mm — far outside the section — so this member is
overwhelmingly flexural, with the axial load acting as a modest bonus rather than the dominant
action.
Set up the strain-compatibility check. For a symmetrically reinforced section
with $A_s$ in each face at $d' = 66.3$ mm from the near face,
$$P_r = \alpha_1\phi_cf_c'b a + \phi_sA_s'f_s' - \phi_sA_sf_s, \qquad
M_r = \alpha_1\phi_cf_c'ba\!\left(\frac{h}{2}-\frac{a}{2}\right) + \phi_sA_s'f_s'\!\left(\frac{h}{2}-d'\right)
+ \phi_sA_sf_s\!\left(d-\frac{h}{2}\right)$$
with $a = \beta_1 c$ and the steel stresses from $\varepsilon_{cu} = 0.0035$ linear strain,
capped at $f_y$.
Solve for the neutral axis at the applied axial load. Trying 10–30M in
total (5 per face, $A_s = 3\,500$ mm$^2$ each face, $\rho = 1.75$ %), the value of $c$ that makes
$P_r = 755.1$ kN is $c = 123.0$ mm. At that neutral-axis depth the tension steel is well past yield
and the compression steel is not, and the corresponding moment resistance is
$$\boxed{M_r = 1\,058\ \text{kN}\cdot\text{m} > M_f = 1\,013.6\ \text{kN}\cdot\text{m}}$$
a utilisation of 0.96 — efficient without being tight.
Check the code limits on the reinforcement. The 1 % minimum for a column
requires $0.01(500)(800) = 4\,000$ mm$^2$; the 7 000 mm$^2$ provided sits comfortably between that and
the 4 % maximum. Five 30M bars per face fit easily across the 500 mm width. Ties must be at least
10M (for 30M longitudinals) at a spacing not exceeding
$\min(16d_b, 48d_{tie}, b) = \min(478, 542, 500) = 478$ mm, so use 10M ties at
400 mm, tightened to 200 mm over a distance $h$ either side of the joint at C and above the
base at D where the moment gradient is steepest.
Check shear on the column. The column shear is the 120 kN horizontal load. With
$d_v = 660.4$ mm,
$V_c = 0.65(0.18)(5.916)(500)(660.4) = 229$ kN, which alone exceeds the demand, so the tie spacing
above is governed by confinement and not by shear.
Because the eccentricity is so large, the section behaves essentially as a doubly reinforced beam:
the concrete compression block is only 109 mm deep, and almost the whole resistance comes from the
steel couple. That is also why symmetric reinforcement is the right choice here even though the
moment always acts in one direction — the wind-type horizontal load can reverse, and a symmetric
column is detailed once and works either way.