Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. 07-Str-A1 Elementary Structural Analysis,
National Examinations, May 2017. Three hours, CLOSED BOOK (an approved Sharp or
Casio calculator is permitted). Page 1 states that six questions
constitute a complete paper: Questions 1–5 are compulsory and the candidate
answers one only of Questions 6, 7 or 8. All eight questions are worked
below.
Sign conventions used throughout. Sagging bending moment is
positive and is plotted above the axis; shear is the sum of the upward forces on
the portion to the left of the section. Truss member forces are quoted as
T for tension and C for compression. In the slope-deflection
work of Question 7 the member-end moments follow the usual convention —
clockwise on the member end taken as positive — so the sagging moment is
$+M_{ij}$ at the left end of a member and $-M_{ji}$ at its right end. For the
bent members of Questions 2(c) the diagrams are developed: the abscissa
is distance measured along the member axis, not the horizontal projection.
Given. A 24 m truss carrying its load on the top chord.
Top chord $U_1 \ldots U_5$ at 6 m centres (so the panel points are at 0, 6, 12,
18, 24 m), bottom chord $L_1$, $L_2$, $L_3$ directly below $U_2$, $U_3$, $U_4$,
depth 2.5 m. Pin at $U_1$, roller at $U_5$. The web comprises the verticals
$U_2L_1$, $U_3L_2$, $U_4L_3$ and the diagonals $U_1L_1$, $U_2L_2$, $L_2U_4$ and
$L_3U_5$. Each diagonal spans 6 m by 2.5 m, so its length is
$\sqrt{6^2+2.5^2} = 6.5$ m — a scaled 5–12–13 triangle.
Find. The influence lines for $U_3L_2$, $U_3U_4$ and
$L_2U_4$, with the ordinates at the quarter, mid and three-quarter points
(6 m, 12 m and 18 m).
5(a): the truss, loaded along the top chord, with a pin at $U_1$ and a roller at $U_5$. Thirteen members, eight joints, three reactions: determinate.
5(a): the three influence lines. Ordinates are member force per unit load; positive is tension. Each line is straight between panel points because the load is delivered through the top-chord stringers.
Approach. For the vertical, inspect joint $U_3$; for the
chord and the diagonal, cut the panel $U_3U_4$ and use moments about $L_2$ and
vertical resolution respectively, once with the unit load left of the cut and
once with it right of it.
The vertical $U_3L_2$ — inspection of joint $U_3$.
Only three members meet at $U_3$: the collinear chord members $U_2U_3$ and
$U_3U_4$, and the vertical $U_3L_2$. Neither adjacent diagonal touches $U_3$.
Vertical equilibrium of the joint therefore reads
$$-F_{U_3L_2} - P_{U_3} = 0 \;\Rightarrow\; F_{U_3L_2} = -P_{U_3}$$
so the member force equals minus the load standing at $U_3$ and is zero for a
unit load at any other panel point. The influence line is a single triangle:
$$\boxed{\text{IL}(U_3L_2):\quad 0,\ 0,\ -1.000,\ 0,\ 0
\ \text{at } U_1 \ldots U_5}$$
Set up the section for the other two. Cut vertically
between $U_3\,(12,0)$ and $U_4\,(18,0)$. The cut severs the top chord $U_3U_4$,
the diagonal $L_2U_4$ and the bottom chord $L_2L_3$ — exactly three
members. The two chords are horizontal and intersect at infinity; the bottom
chord and the diagonal both pass through $L_2\,(12,-2.5)$.
Top chord $U_3U_4$ — moments about $L_2$. With the
unit load to the right of the cut, the left free body carries only
$R_{U_1}$, whose lever arm about $L_2$ is 12 m, against the chord force acting
at the 2.5 m depth:
$$-12R_{U_1} - 2.5\,F_{U_3U_4} = 0 \;\Rightarrow\; F_{U_3U_4} = -4.8\,R_{U_1}$$
With the load to the left, the right free body gives the mirror result
$F_{U_3U_4} = -4.8\,R_{U_5}$. Evaluating with
$R_{U_1} = (24-x)/24$ and $R_{U_5} = x/24$:
$$\boxed{\text{IL}(U_3U_4):\quad 0,\ -1.200,\ -2.400,\ -1.200,\ 0}$$
Compression throughout, as a top chord should be.
Diagonal $L_2U_4$ — vertical resolution on the same
section. The two cut chords are horizontal, so only the diagonal
carries vertical force across the cut. Its vertical direction cosine is
$2.5/6.5$. Unit load left of the cut:
$$R_{U_5} - \tfrac{2.5}{6.5}F_{L_2U_4} = 0 \;\Rightarrow\;
F_{L_2U_4} = 2.6\,R_{U_5}$$
Unit load right of the cut: $F_{L_2U_4} = -2.6\,R_{U_1}$. Hence
$$\boxed{\text{IL}(L_2U_4):\quad 0,\ +0.650,\ +1.300,\ -0.650,\ 0}$$
The sign reversal between the mid point and the three-quarter point is the
diagonal changing from tension to compression as the load crosses the panel,
which is exactly what an influence line for a web diagonal is for.
Sense check on the numbers. The three ratios are pure
geometry: $4.8 = 12/2.5$ is half the span over the depth, $2.6 = 6.5/2.5$ is the
diagonal length over the depth, and the vertical's peak is exactly $-1$ because
a unit load standing on the joint must be carried straight down the hanger.
Change the depth and only the first two move.
Member
¼ point (6 m)
½ point (12 m)
¾ point (18 m)
Peak
$U_3L_2$ (vertical)
0
−1.000
0
−1.000 at $U_3$ (C)
$U_3U_4$ (top chord)
−1.200
−2.400
−1.200
−2.400 at mid-span (C)
$L_2U_4$ (diagonal)
+0.650
+1.300
−0.650
+1.300 at $U_3$ (T)
5(b) Shear influence line and a moving uniform load
Given. A simply supported beam of span 25 m, pin at the left
support and roller at the right. Section ①–① is 5 m from the
left support. The vehicle is idealised as a uniformly distributed load of
$20\ \text{kN}\,\text{m}^{-1}$ over a length of 10 m, travelling from left to
right.
Find. The influence line for shear at the section with its
ordinates, and the maximum absolute shear the vehicle can produce there.
5(b): the shear influence line at the section 5 m from the left support, and the governing position of the 10 m vehicle.
Approach. Write the influence line from the two support
reactions, then place the 10 m load block where it captures the greatest area
under the line; the shear is the load intensity times that area.
Ordinates of the influence line. For a unit load at
distance $x$ from the left support, $R_{\text{left}} = (25-x)/25$. Taking the
shear as the upward force on the left portion,
$$V = -\frac{x}{25}\ \ (x < 5), \qquad V = \frac{25-x}{25}\ \ (x > 5)$$
so the line runs from 0 at the left support down to
$$V_{\text{left of section}} = -\frac{5}{25} = \boxed{-0.200}$$
jumps by unity across the section to
$$V_{\text{right of section}} = \frac{20}{25} = \boxed{+0.800}$$
and returns linearly to zero at the right support.
Governing position for positive shear. The positive lobe is
the triangle from 5 m to 25 m with its peak $+0.800$ at the section, so the 10 m
block should sit hard against the section, occupying 5 m to 15 m. The ordinates
at its ends are $0.800$ and $(25-15)/25 = 0.400$, so the area under the line is
$$A^{+} = \frac{0.800 + 0.400}{2}\,(10) = 6.00\ \text{m}$$
Maximum positive shear.
$$V^{+}_{\max} = w A^{+} = 20(6.00) = \boxed{120.0\ \text{kN}}$$
Governing position for negative shear. The negative lobe is
only 5 m long and its deepest ordinate is $-0.200$, so at best the vehicle
covers it entirely (front axle at the section, the rear 5 m still off the span)
and picks up an area of $\tfrac12(0.200)(5) = 0.50$ m:
$$V^{-}_{\max} = 20(0.50) = -10.0\ \text{kN}$$
Pushing the vehicle further on only adds positive area, so this is as negative as
it gets. If the vehicle is required to sit wholly on the beam, the most adverse
position it can reach is 0 m to 10 m, which already gives $+60.0$ kN.
Answer. Comparing the two,
$$|V|_{\max} = \max(120.0,\ 10.0) = \boxed{120.0\ \text{kN}}$$
with the vehicle occupying 5 m to 15 m, i.e. its rear immediately at the
section.