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07-Str-A4 · May 2015

Question 8 of 9: Slope-deflection analysis of a frame on an inclined roller

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

Notes on this paper

Paper format. 07-Str-A4 Advanced Structural Analysis, National Examinations, May 2015 — three hours, closed book (an approved Sharp or Casio calculator is the only aid). Questions 1 and 2 are compulsory; the candidate then answers two of Questions 3, 4, 5, one of Questions 6, 7 and one of Questions 8, 9, so six questions totalling 100 marks constitute a complete paper. Marks are printed in the left margin. All nine questions are solved here, because the set is a study resource rather than an examination script.

Reference texts. R. C. Hibbeler, Structural Analysis (Pearson) — force/flexibility method, slope-deflection, moment distribution and influence lines; A. Kassimali, Structural Analysis (Cengage) — matrix stiffness formulation and support-settlement effects; J. C. McCormac, Structural Analysis: Using Classical and Matrix Methods (Wiley); CSA S16:19 Design of Steel Structures and CSA S6:19 Canadian Highway Bridge Design Code for the Canadian design setting in which these analyses are used.

Sign convention used throughout. Bending moments are reported as sagging positive and are plotted on the tension face of each member. Slope-deflection end moments follow the counter-clockwise-positive convention stated in Question 9: $$M_{ij}=\frac{2EI}{L}\left(2\theta_i+\theta_j-3\psi_{ij}\right)+M^{F}_{ij},\qquad \psi_{ij}=\frac{(\mathbf{D}_j-\mathbf{D}_i)\cdot \mathbf{e}_2}{L}$$ where $\mathbf{e}_2$ is the member axis rotated 90 degrees counter-clockwise, and the fixed-end moments of a downward uniform load are $M^{F}_{ij}=+wL^2/12$, $M^{F}_{ji}=-wL^2/12$. The sagging moment at the ends of a member is then $M(i)=-M_{ij}$ and $M(j)=+M_{ji}$.

Question 8: Slope-deflection analysis of a frame on an inclined roller (24 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.

QuantityValue
Beam 1–2$6\ \text{m}$, rigidity $3EI$, built in at joint 1
Column 2–3$4\ \text{m}$, rigidity $EI$
Load$w=12\ \text{kN/m}$ on the beam
Support at joint 3roller on a plane of slope $3:4$ (falling to the right)

Find. The end moments, the shear force and bending moment diagrams with maximum and minimum ordinates, and the reactions.

12 kN/m1233EIEI6 m4 m43
Question 8: the frame with its roller bearing on a plane of slope 3 in 4.

Approach. The inclined roller couples the vertical and horizontal movement of joint 3; use inextensibility to reduce the whole kinematics to a single translation parameter, then write slope-deflection equations in that parameter and the two rotations, and close the system with the virtual-work equation for the translation.

  1. Kinematics. Joint 1 is built in, so $u_1=v_1=0$; the beam is inextensible, so $u_2=0$; the column is inextensible, so $v_3=v_2$. The roller allows joint 3 to move only along the plane, whose direction is $(4,-3)/5$, so $$\frac{u_3}{4}=\frac{v_3}{-3}\;\Longrightarrow\;u_3=-\tfrac{4}{3}v_2$$ Everything is therefore governed by the single translation $v_2$, together with the rotations $\theta_2$ and $\theta_3$.
  2. Chord rotations. $$\psi_{12}=\frac{v_2}{6},\qquad \psi_{23}=\frac{-u_3}{4}=\frac{\tfrac{4}{3}v_2}{4}=\frac{v_2}{3}$$ so tilting the beam down at joint 2 simultaneously rakes the column — the essential feature of an inclined roller.
  3. Slope-deflection equations. With $M^{F}_{12}=+wL^{2}/12=+36$ and $M^{F}_{21}=-36\ \text{kN}\cdot\text{m}$, $$M_{12}=\tfrac{2(3EI)}{6}\left(\theta_2-3\psi_{12}\right)+36,\qquad M_{21}=\tfrac{2(3EI)}{6}\left(2\theta_2-3\psi_{12}\right)-36$$ $$M_{23}=\tfrac{2EI}{4}\left(2\theta_2+\theta_3-3\psi_{23}\right),\qquad M_{32}=\tfrac{2EI}{4}\left(2\theta_3+\theta_2-3\psi_{23}\right)$$
  4. Equilibrium equations. Joint 2 is rigid and joint 3 is a moment-free roller: $$M_{21}+M_{23}=0,\qquad M_{32}=0$$ and the third equation comes from a virtual translation along the roller plane, which by the inextensibility relations is a virtual $v_2^{*}=1$: $$\left(M_{12}+M_{21}\right)\psi^{*}_{12}+\left(M_{23}+M_{32}\right)\psi^{*}_{23} +W_{\text{ext}}=0$$
  5. Solve. The three equations give $$M_{12}=-108,\qquad M_{21}=M_{\text{sag}}(2)=+36,\qquad M_{32}=0\ \text{kN}\cdot\text{m}$$ i.e. the built-in end hogs $\boxed{108\ \text{kN}\cdot\text{m}}$ while the knee joint carries a sagging $\boxed{36\ \text{kN}\cdot\text{m}}$, and the joint displacements are $u_3=192/EI$ to the right and $v_3=-144/EI$, which satisfy $3u_3+4v_3=0$ as the roller requires.
  6. Beam diagrams. Vertical equilibrium of the beam with the two end moments gives $$V_1=\frac{w L}{2}+\frac{M_{21}-M_{12}}{L}\cdot\frac{1}{1}=60\ \text{kN},\qquad V_2=60-12(6)=-12\ \text{kN}$$ $$M(x)=-108+60x-6x^{2}\;\Rightarrow\; M_{\max}=\boxed{+42\ \text{kN}\cdot\text{m}}\ \text{at}\ x=5\ \text{m}$$ with the moment passing through $+36\ \text{kN}\cdot\text{m}$ at joint 2 and through zero at $x=2.0$ and $x=8.0$ — only the first of which lies on the beam.
  7. Column diagrams. The column carries a moment falling linearly from $36\ \text{kN}\cdot\text{m}$ at joint 2 to zero at the roller, so $$V_{23}=\frac{36}{4}=9\ \text{kN}\ \text{(constant)},\qquad N_{23}=12\ \text{kN\ (compression)}$$
  8. Reaction at the inclined roller and check. The reaction must be normal to the plane, i.e. along $(3,4)/5$: $$R_3=\sqrt{9^{2}+12^{2}}=\boxed{15\ \text{kN}}$$ with components $9\ \text{kN}$ horizontal and $12\ \text{kN}$ vertical. At the built-in end $V=60\ \text{kN}$ upward, $H=9\ \text{kN}$ to the left and $M=108\ \text{kN}\cdot\text{m}$; vertically $60+12=72=12(6)\ \checkmark$, horizontally $9-9=0\ \checkmark$, and moments about joint 1 give $-216+72+36+108=0\ \checkmark$.
-108+42+360Bending moment (kN.m) plotted on the tension face
Question 8: bending moment diagram, kN.m.
60-129Shear force (kN)
Question 8: shear force diagram, kN.
Question 8 — complete results
QuantityValue
Moment at joint 1$-108\ \text{kN}\cdot\text{m}$ (hogging) — minimum ordinate
Moment at joint 2$+36\ \text{kN}\cdot\text{m}$ (sagging), continuous into the column
Moment at joint 3$0$ (roller)
Maximum sagging moment in the beam$+42\ \text{kN}\cdot\text{m}$ at $x=5\ \text{m}$
Beam shear$+60\ \text{kN}$ at joint 1 to $-12\ \text{kN}$ at joint 2
Column shear / axial force$9\ \text{kN}$ / $12\ \text{kN}$ compression
Reaction at joint 3$15\ \text{kN}$ normal to the plane ($9\rightarrow$, $12\uparrow$)
Reaction at joint 1$60\ \text{kN}\uparrow$, $9\ \text{kN}\leftarrow$, $108\ \text{kN}\cdot\text{m}$