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07-Str-A1 · December 2013

Question 7 of 8: Influence lines for a truss and for a hinged frame under a moving vehicle

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

Notes on this paper

Paper format. National Examinations, December 2013 — 07-Str-A1 Elementary Structural Analysis. Three hours, CLOSED BOOK, an approved Sharp or Casio calculator permitted. Six questions constitute a complete paper: candidates answer ALL of Questions 1 to 5 and ONE of Questions 6, 7 or 8. Marks are shown in the left margin (6 + 18 + 18 + 18 + 20 + 20 = 100). All eight questions are solved below, because the three alternatives test different topics and the whole set is useful for study.

Reference texts.

Sign conventions used throughout. For beams and for each individual frame member, shear is positive when the resultant of the forces to the left of (or below) a section acts upward, and bending moment is positive when it sags the member, that is when it puts the underside of a beam or the inside face of a frame member in tension. Member end moments in the slope-deflection work of Question 5 are clockwise-positive on the member, which is the usual convention for that method. Truss forces are quoted as tension or compression rather than by sign. Reactions are drawn in blue and applied loads in red on every figure.

A note on reading this paper. The figures are hand drawn and carry no dimensions that are not on the drawings, so the geometry of every structure below was read from the support symbols one at a time. Two readings materially affect the answers and are flagged where they arise: the plane on which the roller of Question 2(c) bears, and the position of the 50 kN load in Question 8.

Question 7: Influence lines for a truss and for a hinged frame under a moving vehicle (20 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.

Part (a)ValuePart (b)Value
Bottom chord$L_1$ to $L_5$ at 6 m centres, 24 m overallBeamA at 0 m, B at 6 m, C at 8 m, D at 10 m, E at 16 m
Top chord$U_1$ to $U_4$ at 6 m centres, offset 3 m, height 4 mInternal hingesat B and at D
Supportspin at $L_2$, roller at $L_4$; 6 m overhang each endSupportsrollers at A and E; column of 5 m built in beneath C
Travelunit load along the bottom chordVehicle10 kN/m over a length of 4 m

Find. (a) Three influence lines with the largest influence coefficient of each. (b) The influence line for bending moment immediately left of C, and the largest negative bending moment the vehicle can produce there.

L1L2L3L4L5U1U2U3U44 m6 m6 m6 m6 mthe unit load travels along the bottom chord
Part (a): the truss, pinned at $L_2$ and on a roller at $L_4$ with a 6 m overhang at each end.
+1.500L1L2L3L4L5IL for U1U2
−1.125+0.375−0.375L1L2L3L4L5IL for L2L3
+0.625+0.625−0.625L1L2L3L4L5IL for U2L3
Part (a) influence lines, ordinates plotted against the position of the unit load on the bottom chord.
ABCDE6 m2 m2 m6 m5 m10 kN/m over 4 m of decktravels to the right
Part (b): the frame, with hinges at B and D and a 5 m column built in below C.
−2.00 m−1.00−1.00ABCEvehicle at its worst position, 3 m to 7 m
Part (b) influence line for the bending moment immediately left of C, with the critical 4 m position of the vehicle marked.

Approach. For the truss, place the unit load at each bottom-chord joint in turn and analyse; because the load is transferred at panel points the influence line is straight between them. For the frame, work out the ordinate as a function of the load position from the two free bodies the hinges create, then slide the 4 m block to the position that maximises the area of the negative lobe.

  1. Part (a) — how the truss carries a unit load. The pin at $L_2$ and the roller at $L_4$ are 12 m apart with a 6 m overhang beyond each. For a unit load at bottom joint $L_i$ the reactions follow from moments about the far support, so a load on an overhang lifts the far reaction. For example a unit load at $L_1$ gives $V_{L_2} = 1.5$ upward and $V_{L_4} = 0.5$ downward, while a load at $L_3$ splits equally, 0.5 at each support.
  2. Part (a) — influence line for the top chord $U_1U_2$. Cut just to the right of $L_2$, severing $U_1U_2$, $L_2U_2$ and $L_2L_3$, and take moments about $L_2$, which lies on the line of the other two cut members. With the top chord 4 m above the bottom chord, its lever arm about $L_2$ is 4 m. With the load on the span the left part carries nothing but the reaction at $L_2$, which has no lever arm, so the ordinate is zero at $L_2$ and everywhere to its right. With the unit load at $L_1$, $$4\,F_{U_1U_2} = 1\,(6) \;\Rightarrow\; \eta = +1.500$$ The influence line is therefore a straight fall from $+1.500$ at $L_1$ to zero at $L_2$ and zero thereafter, so $$\eta_{\max} = \boxed{+1.500\ \text{at}\ L_1\ \text{(tension)}}$$
  3. Part (a) — influence line for the bottom chord $L_2L_3$. Cut between $L_2$ and $L_3$ and take moments about $U_2$ at $(9,\,4)$, the point where the top chord and the diagonal $L_2U_2$ meet. The lever arm of the bottom chord about $U_2$ is 4 m. Placing the unit load in turn at each joint gives ordinates $$\eta_{L_1} = -1.125, \quad \eta_{L_2} = 0, \quad \eta_{L_3} = +0.375, \quad \eta_{L_4} = 0, \quad \eta_{L_5} = -0.375$$ so the largest coefficient is $$\eta_{\max} = \boxed{-1.125\ \text{at}\ L_1\ \text{(compression)}}$$ The chord goes into compression whenever the load is on either overhang and into tension when it is inside the span, which is the signature of a bottom chord in a beam with two cantilevers.
  4. Part (a) — influence line for the diagonal $U_2L_3$. Move the cut to the right of $U_2$, between $x = 9$ m and $x = 12$ m, where it severs $U_2U_3$, $U_2L_3$ and $L_2L_3$. Both chords are horizontal, so vertical equilibrium of the left part isolates the diagonal alone. It runs from $(9,\,4)$ to $(12,\,0)$, so its vertical direction cosine is $4/5$ and the panel shear divided by $0.8$ gives the force. Evaluating at each joint, $$\eta_{L_1} = +0.625, \quad \eta_{L_2} = 0, \quad \eta_{L_3} = +0.625, \quad \eta_{L_4} = 0, \quad \eta_{L_5} = -0.625$$ so the largest absolute coefficient is $$|\eta|_{\max} = \boxed{0.625}$$ reached in tension with the load at $L_1$ or at $L_3$ and in compression with the load at $L_5$.
  5. Part (b) — what the hinges do. The beam is in three pieces: A to B on the roller at A and hanging from the hinge at B, the rigid tee B to C to D carried by the built-in column, and D to E on the hinge at D and the roller at E. A load between D and E, or between C and D, is carried entirely by parts that lie to the right of the section just left of C, so it produces no moment there at all. Only a load between A and C can register.
  6. Part (b) — build the ordinate. With the unit load at distance $a$ from A, the piece A to B is a simple 6 m span between the roller and the hinge, so $$\begin{aligned} R_{A} &= \frac{6 - a}{6} \quad (0 \le a \le 6) \\ R_{A} &= 0 \quad (a > 6) \end{aligned}$$ Taking the free body to the left of the section just left of C, which is 8 m from A, $$\begin{aligned} \eta &= 8R_{A} - (8 - a) \quad (a < 8) \\ \eta &= 8R_{A} \quad (a \ge 8) \end{aligned}$$ Substituting the two ranges, $$\begin{aligned} \eta &= -\frac{a}{3} \quad (0 \le a \le 6) \\ \eta &= -(8 - a) \quad (6 \le a \le 8) \\ \eta &= 0 \quad (a \ge 8) \end{aligned}$$
  7. Part (b) — the influence line. The result is a triangle, entirely negative, running from zero at A down to $$\eta_{B} = \boxed{-2.00\ \text{m}}$$ at the hinge B and back to zero at C, and flat at zero from C to E. The peak sits at the hinge, not at the section, because the hinge is where the left-hand piece hands its load to the cantilevering tee.
  8. Part (b) — position the vehicle. A uniform load of intensity $q$ covering a length of the influence line produces $q$ times the area beneath that length, so the worst 4 m position is the one that maximises the negative area. Differentiating the area with respect to the position of the leading wheel shows the maximum occurs where the ordinates at the two ends of the block are equal, that is where $$-\frac{s}{3} = -(8 - s - 4) \;\Rightarrow\; s = 3\ \text{m}$$ so the vehicle occupies 3 m to 7 m from A, with $\eta = -1.00$ m at each end.
  9. Part (b) — the largest negative moment. The area under that 4 m of influence line is one trapezium from 3 m to 6 m and a second from 6 m to 7 m: $$A = -\tfrac{1}{2}(1.00 + 2.00)(3) - \tfrac{1}{2}(2.00 + 1.00)(1) = -4.50 - 1.50 = -6.00\ \text{m}^{2}$$ so the largest negative bending moment immediately left of joint C is $$M = qA = 10\,(-6.00) = \boxed{-60.0\ \text{kN}\cdot\text{m}}$$ For comparison, a vehicle long enough to cover the whole triangle would give $10(-8.00) = -80$ kN·m, so the 4 m length captures three quarters of the worst possible effect.
QuantityValuePosition of the load
$\eta_{\max}$ for $U_1U_2$+1.500 (tension)unit load at $L_1$
$\eta_{\max}$ for $L_2L_3$−1.125 (compression)unit load at $L_1$
$|\eta|_{\max}$ for $U_2L_3$0.625+0.625 at $L_1$ and $L_3$; −0.625 at $L_5$
Peak ordinate of the frame influence line−2.00 munit load at the hinge B
Largest negative moment left of C−60.0 kN·mvehicle occupying 3 m to 7 m from A