Question 1 of 8: Stability and Determinacy of Six Structures
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
Paper format. National Exams, December 2018 — 07-Str-A1
Elementary Structural Analysis; 3 hours, CLOSED BOOK (an approved Casio or Sharp
calculator is permitted). Six questions constitute a complete paper: answer all of
Questions 1–5, then one only of Questions 6, 7 or 8. Marks are shown in the
left margin (6, 18, 18, 18, 18, then 22 for the optional question). Every question is
worked below, including all three alternatives, because the full set is the more useful
study resource.
Reference texts. R. C. Hibbeler, Structural Analysis (Ch. 2
determinacy and stability; Ch. 4 influence lines; Ch. 6–9 deflections and virtual work;
Ch. 12 moment distribution); A. Kassimali, Structural Analysis (Ch. 3, 6, 8, 13, 16);
K. Leet, C.-M. Uang and A. Gilbert, Fundamentals of Structural Analysis;
J. C. McCormac, Structural Analysis: Using Classical and Matrix Methods. For Canadian
practice the companion documents are the National Building Code of Canada (Part 4 load
combinations) and CSA S16 Design of Steel Structures; this paper is pure analysis, so no
design code is invoked in the answers.
Check — two figure readings that the printed figures leave open,
both stated where they are used. (i) In Question 2(c) the hatched plane under the
upper roller is drawn parallel to the inclined member, so the reaction is taken
normal to the member. That reading makes every result an integer
(R = 28 kN, shears 32 / −4 / −28 kN, axial forces
25 / 10 / 0 kN), whereas a vertical-plane reading gives nothing round; and because the two
readings differ only by a force acting along the member axis, the shear and moment
diagrams are identical either way. (ii) In Question 7 both wall supports are drawn as
triangles on hatching. The truss is analysable only if one of them releases a component;
taking the pin at U₂ and the horizontal-only roller at L₃ gives
δ = 29.0 mm, and the same value follows if the thin vertical
line between the two wall joints is a dimension witness line rather than a member. The
alternative (pin at L₃) would give 31.8 mm.
Question 1: Stability and Determinacy of Six Structures (6 marks)
Given. Six planar structures: (a) a continuous beam on a pin and three
rollers carrying a full-length UDL, with two internal hinges (labelled TYPICAL HINGE) in the
bay between the second and third supports; (b) a trapezoidal frame with rigid knees, fixed
bases and one internal hinge at mid-beam; (c) a two-storey single-bay frame, columns fixed at
their bases, rigid beam-to-column joints, and two internal hinges in each of the two
loaded beams; (d) the same trapezoid as (b) but with pinned bases and no hinge;
(e) a triangulated truss with a pin and a roller, whose central panel carries both of its
diagonals (not connected where they cross); (f) an irregular truss on two pinned bases
carrying two horizontal loads.
Find. The classification of each structure, with the degree of
indeterminacy where it applies.
(c) two-storey frame — fixed bases, 2 hinges per beam
(d) pinned bases, rigid knees, no hinge
Question 1, structures (c) and (d).
(e) truss — pin + roller, central panel double-diagonalled
(f) truss — two pinned bases, horizontal loads
Question 1, structures (e) and (f).
Approach. Count first, then interrogate the arrangement: for
beam-type and framed structures use $i = 3m + r - 3j - c$ and for pin-jointed trusses
$i = m + r - 2j$, and afterwards ask of every partitioned piece "what motion is still free?",
because a favourable count never by itself proves stability.
Part (a) — a Gerber beam: count the release equations, then check that the
suspended span is genuinely carried. One continuous member, $r = 2 + 1 + 1 + 1 = 5$
and $c = 2$, so
$$i = r - 3 - c = 5 - 3 - 2 = \boxed{0}$$
The count alone is not enough here, because the two hinges bracket a length of beam that
carries no support of its own. Writing the four independent equations (global $\Sigma F_y$ and
$\Sigma M$, plus zero moment at each hinge) and solving symbolically gives a non-singular
coefficient matrix, so the piece between the hinges is a suspended span carried by the two
cantilevered ends — the classic Gerber arrangement. Statically determinate.
Part (b) — an open frame with fixed bases and one release.
$m = 3$ (leg, beam, leg), $j = 4$, $r = 3 + 3 = 6$, $c = 1$, hence
$$i = 3(3) + 6 - 3(4) - 1 = 9 + 6 - 12 - 1 = \boxed{2}$$
Statically indeterminate to the second degree. The hinge buys one equation back from
the three redundants a two-fixed-base open frame would otherwise carry.
Part (c) — two closed panels, four releases. Taking joints at both
bases, both mid-height beam-to-column intersections and both roof corners gives $j = 6$ and
$m = 6$ (two column lengths each side, two beams); $r = 6$ and $c = 4$:
$$i = 3(6) + 6 - 3(6) - 4 = 18 + 6 - 18 - 4 = \boxed{2}$$
Each closed rectangle contributes three redundants and each hinge removes one:
$3 + 3 = 6$ against four hinges. Statically indeterminate to the second degree.
Part (d) — the same geometry with pins instead of fixed bases and no
hinge. $m = 3$, $j = 4$, $r = 2 + 2 = 4$, $c = 0$:
$$i = 3(3) + 4 - 3(4) - 0 = \boxed{1}$$
Statically indeterminate to the first degree — the familiar two-hinged arch or
portal. Comparing (b) with (d) is the point of the pair: releasing both base moments removes
two redundants, adding the crown hinge removes one more, and only the order in which you
remove them changes.
Part (e) — a truss whose central panel carries two diagonals.
Counting the members gives six bottom-chord bars, one horizontal top chord, the two rafter
segments each side of the apex, two verticals and two crossing diagonals, i.e. $m = 12$ over
$j = 7$ joints with $r = 3$:
$$i = m + r - 2j = 12 + 3 - 14 = \boxed{1}$$
The redundancy is easy to name: the quadrilateral panel bounded by the two verticals, the
horizontal top chord and the bottom chord needs only one diagonal to be rigid, and it is
given both. Statically indeterminate to the first degree.
Part (f) — the deliberately deficient one. The bars are
$A\!-\!C$, $C\!-\!E$, $E\!-\!D$, $D\!-\!B$, $C\!-\!D$, $E\!-\!F$ and $F\!-\!B$, so $m = 7$,
$j = 6$ and $r = 2 + 2 = 4$:
$$i = m + r - 2j = 7 + 4 - 12 = \boxed{-1}$$
A negative index means the assembly is a mechanism, and the motion is easy to identify: the
four bars $A\!-\!C$, $C\!-\!D$, $D\!-\!B$ with pins at $A$ and $B$ form a four-bar linkage
with one degree of freedom; joint $E$ is then tied rigidly to bar $C\!-\!D$ by the triangle
$C\!-\!D\!-\!E$, and joint $F$ is located by its two bars to $E$ and $B$. Counting freedoms
instead of bars says the same thing — four movable joints give eight degrees of freedom
against only seven bar constraints. Unstable.