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07-Str-A1 · December 2016

Question 2 of 8: Reactions, Shear and Bending Moment Diagrams

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

Notes on this paper

Paper format. National Exams, December 2016 — 07-Str-A1 Elementary Structural Analysis, 3 hours, CLOSED BOOK (an approved Sharp or Casio calculator is permitted). Six questions constitute a complete paper: Questions 1–5 are compulsory and one only of Questions 6, 7 or 8 is attempted, for 100 marks (6 + 18 + 18 + 20 + 18 + 20). Marks are shown in the left margin. All eight questions are worked below, because the three alternatives exercise three quite different methods — three-hinged-frame statics, influence lines and virtual work — and the complete set is the more useful study resource.

Every structure on this paper is defined by a hand-drawn figure and nothing else: the printed text states the task, the drawing carries the geometry, the loads and the support types.

Sign conventions used throughout. Shear force is positive when the resultant of the forces to the left of a section acts upwards along the positive local normal of the member; bending moment is positive when it sags the member (tension on the underside), and sagging ordinates are plotted above the axis in every diagram. Truss member forces are quoted as T for tension and C for compression. In the slope-deflection work of Question 5 the member-end moments follow the usual convention, clockwise on the member end taken as positive, so that the sagging moment is $+M_{ij}$ at the left end of a member and $-M_{ji}$ at its right end.

Reference texts.

Question 2: Reactions, Shear and Bending Moment Diagrams (18 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.

(a) Simply supported beam with an overhang

Given. A straight beam 16 m long measured from the left-hand pin. The concentrated load and the distributed load are read from the figure as follows.

Given data, structure 2(a)
QuantityValue
Pin support Ax = 0
Concentrated load60 kN downward at x = 6 m
Uniformly distributed load6 kN/m from x = 6 m to the right-hand end at x = 16 m
Roller support Bx = 12 m
Overhang4 m, from x = 12 m to x = 16 m

The extent of the load block is the reading that decides the whole answer. Its left edge sits exactly on the 60 kN arrow and its right edge on the end of the member line, so the ruling covers 10 m and not the 6 m bay between the load and the roller. The reactions that follow are integers, which is the usual confirmation that a hand-drawn extent has been read correctly.

Find. The two reactions, and the shear and bending moment diagrams with the maximum and minimum ordinates labelled.

6 kN/m60 kNR_A = 35 kNR_B = 85 kN6 m6 m4 mV (kN)+35-25-61+24M (kN.m)+210-48
Structure 2(a): loading, reactions, shear force diagram and bending moment diagram. Sagging moments are plotted above the axis.

Approach. Take moments about the pin to find the roller reaction, then build the shear diagram from the left by accumulating the loads and read the moment diagram off it, the moment being the running area under the shear curve.

  1. Resolve the loading into two resultants. The distributed load acts over $16 - 6 = 10$ m, so $$W = w L = (6\ \text{kN/m})(10\ \text{m}) = 60\ \text{kN}$$ acting at the centroid of the block, $x = 11$ m. Together with the 60 kN concentrated load at $x = 6$ m the total applied load is 120 kN.
  2. Take moments about A to find the roller reaction. With $R_B$ acting at $x = 12$ m, $$\sum M_A = 0: \quad 12 R_B = (60)(6) + (60)(11) = 360 + 660 = 1020$$ $$R_B = \boxed{85\ \text{kN} \uparrow}$$
  3. Vertical equilibrium gives the pin reaction. $$R_A = 120 - 85 = \boxed{35\ \text{kN} \uparrow}$$ Both reactions are integers, which is the arithmetic check on the load extent read in the Given. block.
  4. Build the shear diagram from the left. Over $0 \le x \lt 6$ m no load acts, so $V = +35$ kN, constant. At $x = 6$ m the 60 kN load drops the shear to $35 - 60 = -25$ kN, after which the ruling removes 6 kN per metre: $$V(x) = -25 - 6(x - 6)\ \text{kN}, \qquad 6 \le x \lt 12\ \text{m}$$ so that just left of the roller $V = -25 - 36 = -61$ kN. The roller adds 85 kN, lifting the shear to $+24$ kN, and it then falls linearly to zero at the free end, as it must.
  5. Locate the maximum sagging moment. The shear does not pass through zero inside a span here; it jumps straight from $+35$ kN to $-25$ kN at the concentrated load, so the peak sagging moment is at $x = 6$ m: $$M_{\max} = R_A x = (35)(6) = \boxed{+210\ \text{kN}\cdot\text{m}}$$
  6. Compute the hogging moment over the roller. The tidiest route is from the right, using the overhang alone: $$M_B = -\frac{w a^{2}}{2} = -\frac{(6)(4)^{2}}{2} = \boxed{-48\ \text{kN}\cdot\text{m}}$$ Working from the left gives the same figure, $M = (35)(12) - (60)(6) - 3(6)^{2} = 420 - 360 - 108 = -48\ \text{kN}\cdot\text{m}$, which is the check that the shear diagram and the reactions agree.
  7. Find the point of contraflexure. Between the load and the roller the moment is $M = 210 - 25u - 3u^{2}$ with $u = x - 6$; setting this to zero gives $3u^{2} + 25u - 210 = 0$, so $u = 5.18$ m and the moment changes sign at $x = 11.18$ m. The diagram is therefore positive (sagging) from the pin to $x = 11.18$ m and negative (hogging) from there to the free end.

(b) Propped cantilever with an internal hinge and an overhang

Given. A beam 14 m long built into a wall at the left-hand end, with an internal hinge 4 m from the wall, a roller 6 m beyond the hinge (at x = 10 m) and a free end 4 m beyond the roller. A uniformly distributed load of 6 kN/m covers the whole 14 m — the load block on the figure runs from the wall face to the free end.

Find. The reactions at the built-in end and at the roller, and the shear and bending moment diagrams with maximum and minimum ordinates.

6 kN/mhingeR_1 = 34 kNM_1 = 88 kN.mR_2 = 50 kN4 m6 m4 mV (kN)+34-26+24M (kN.m)-88+8.33-48hinge: M = 0
Structure 2(b): loading, reactions, shear force diagram and bending moment diagram. The moment is zero at the internal hinge.

Approach. The hinge makes the beam determinate, so start with the free body to the right of the hinge, which contains only one unknown reaction; the force it transmits back through the hinge then loads the cantilever portion.

  1. Free body of the beam to the right of the hinge. That piece runs from $x = 4$ m to $x = 14$ m, carries $W = (6)(10) = 60$ kN at $x = 9$ m, and is held by the roller at $x = 10$ m and by the vertical force $F$ that the hinge transmits. Moments about the roller give $$6F = (60)(1) \quad\Rightarrow\quad F = \boxed{10\ \text{kN}}$$
  2. Vertical equilibrium of the same piece gives the roller reaction. $$R_2 = 60 - 10 = \boxed{50\ \text{kN} \uparrow}$$
  3. Transfer the hinge force to the cantilever. The 4 m piece between the wall and the hinge carries its own $6 \times 4 = 24$ kN of ruling plus the 10 kN reaction the right-hand piece pushes down through the hinge: $$R_1 = 24 + 10 = \boxed{34\ \text{kN} \uparrow}$$ $$M_1 = -\left[ (24)(2) + (10)(4) \right] = -48 - 40 = \boxed{-88\ \text{kN}\cdot\text{m}}$$ the negative sign meaning a hogging moment, tension on the top of the beam at the wall.
  4. Write the shear as one expression. Because the ruling is continuous the shear is simply $$V(x) = 34 - 6x\ \text{kN}, \qquad 0 \le x \lt 10\ \text{m}$$ falling from $+34$ kN at the wall through $+10$ kN at the hinge to $-26$ kN just left of the roller, where the 50 kN reaction lifts it to $+24$ kN. Over the overhang it falls to zero at the free end.
  5. Locate and evaluate the peak sagging moment. The shear vanishes at $$x_{0} = \frac{34}{6} = 5.667\ \text{m}$$ and the moment there is $$M(x_{0}) = -88 + 34(5.667) - 3(5.667)^{2} = \boxed{+8.33\ \text{kN}\cdot\text{m}}$$
  6. Check the two other controlling ordinates. At the hinge $M(4) = -88 + 136 - 48 = 0$, exactly as a hinge requires, which validates $R_1$ and $M_1$ together. Over the roller the overhang gives $M = -(6)(4)^{2}/2 = -48\ \text{kN}\cdot\text{m}$, and the moment is negative from the wall to $x = 4$ m, positive from $x = 4$ m to $x = 7.33$ m, and negative again to the free end.

(c) Bent member on a pin and a roller

Given. A single bent member. The pin is taken as the origin; the knee sits 12 m to the right of it and 9 m above it, and the member then falls 4 m over a further 3 m to a roller resting on a horizontal plane. A uniformly distributed load of 10 kN/m acts on the horizontal projection over the whole 15 m width.

Given data, structure 2(c)
QuantityValue
Pin support, node 1(0, 0)
Knee, node 2(12 m, 9 m); member 1-2 length 15 m, slope 3:4
Roller support, node 3(15 m, 5 m); member 2-3 length 5 m, slope 4:3
Distributed load10 kN/m on the horizontal projection, x = 0 to 15 m
Roller planehorizontal, so the reaction is vertical

Check: the roller at node 3 is drawn on horizontal hatching, so its reaction is taken as vertical. That reading is worth stating because a roller on a plane parallel to the inclined member would give a reaction normal to the member instead. It happens not to matter for the diagrams: two such readings differ by a force acting along the member axis, which produces neither shear nor bending moment anywhere, so only the reaction components and the axial force would change.

Find. The reactions, and the shear and bending moment diagrams developed along the member axis with maximum and minimum ordinates.

10 kN/m (on horizontal projection)9 m4 m12 m3 mH = 0V = 75 kNR = 75 kNs measured along the member axis: 0 to 15 m on member 1-2, 15 to 20 m on member 2-3.V (kN)+60-36-27-45M (kN.m)+281.25+180
Structure 2(c): geometry and reactions, with the shear and bending moment diagrams developed along the member axis. The abscissa s runs 0 to 15 m on member 1-2 and 15 to 20 m on member 2-3.

Approach. Because the roller reaction and every applied load are vertical, the pin can carry no horizontal force; the bending moment at any section is then simply the moment of the vertical forces to its left, and the shear is the component of that same resultant taken perpendicular to whichever member the section lies on.

  1. Establish that the pin carries no thrust. The only applied loading is vertical and the roller reaction is vertical, so horizontal equilibrium gives $H_1 = \boxed{0}$. This is what makes the rest of the question short.
  2. Find the reactions. The total load is $W = (10)(15) = 150$ kN acting at the centroid of the projection, $x = 7.5$ m. Moments about the pin, with the roller 15 m away horizontally, give $$15 R_3 = (150)(7.5) = 1125 \quad\Rightarrow\quad R_3 = \boxed{75\ \text{kN} \uparrow}$$ $$V_1 = 150 - 75 = \boxed{75\ \text{kN} \uparrow}$$
  3. Write the bending moment as a function of the horizontal coordinate. Since all forces are vertical, the height of the section does not enter and $$M(x) = 75x - \frac{10x^{2}}{2} = 75x - 5x^{2}\ \text{kN}\cdot\text{m}$$ holds over the entire structure, both members included.
  4. Evaluate the peak moment. Differentiating, $\mathrm{d}M/\mathrm{d}x = 75 - 10x = 0$ at $x = 7.5$ m, which lies on the inclined member at $s = 7.5/0.8 = 9.375$ m along its axis. There $$M_{\max} = (75)(7.5) - 5(7.5)^{2} = 562.5 - 281.25 = \boxed{+281.25\ \text{kN}\cdot\text{m}}$$
  5. Evaluate the moment at the knee. Substituting $x = 12$ m, $$M_{2} = (75)(12) - 5(12)^{2} = 900 - 720 = \boxed{+180\ \text{kN}\cdot\text{m}}$$ and $M = 0$ at both supports, so the whole bending moment diagram is sagging; there are no negative segments and the minimum ordinates are the zeros at the two ends.
  6. Resolve the shear on member 1-2. Its axis is the unit vector $(0.8,\ 0.6)$, so the shear is $0.8$ times the net vertical force to the left of the section: $$V = 0.8\left(75 - 10x\right)$$ which runs from $+60$ kN at the pin to $0.8(75 - 120) = -36$ kN at the knee, passing through zero at $x = 7.5$ m as the moment peak requires.
  7. Resolve the shear on member 2-3. Its axis is $(0.6,\ -0.8)$, so the shear is now $0.6$ times the same net vertical force: $$V = 0.6\left(75 - 10x\right)$$ giving $-27$ kN just past the knee and $-45$ kN just before the roller. The step at the knee is not an error — it is the change of direction of the member, which redistributes the same resultant between shear and axial force.
Question 2 — reactions and controlling diagram ordinates
StructureReactionsShear: max / minMoment: max / min
(a)RA = 35 kN, RB = 85 kN+35 kN / −61 kN+210 kN·m at x = 6 m / −48 kN·m at x = 12 m
(b)R1 = 34 kN, M1 = −88 kN·m, R2 = 50 kN+34 kN / −26 kN+8.33 kN·m at x = 5.67 m / −88 kN·m at the wall
(c)H1 = 0, V1 = 75 kN, R3 = 75 kN+60 kN / −45 kN+281.25 kN·m at x = 7.5 m / 0 at both supports