ENGR216 2019 Q A2Past paperOld spec ENGR2162:125 marks30 min

ENGR216 Summer 2019 Q A2[VALID] official answers

Answer ALL parts (a) - (d)

Consider the statically determinate beam with flexural rigidity EIEI and length LL depicted in Figure A2, subject to the distributed load w(x)w(x), where xx denotes the coordinate along the horizontal axis depicted in the figure with origin at end A of the beam.

Figure A2: beam AB of length L, roller support at A and pin support at B, downward distributed load w(x) decreasing from w0 at A to zero at B; x axis along the beam from A, y axis upwards at A.
Figure A2: beam AB of length L, roller support at A and pin support at B, downward distributed load w(x) decreasing from w0 at A to zero at B; x axis along the beam from A, y axis upwards at A.
Formulas you may need
  • Elastic curve d2ydx2=MEI\dfrac{d^2y}{dx^2} = \dfrac{M}{EI} (given in the question; learn this; on the 2025 sheet but not the 2026 one)
  • Resultant of a distributed load P=∫w dxP = \int w\,dx and its position xP=∫x w dx∫w dxx_P = \dfrac{\int x\,w\,dx}{\int w\,dx} (on the formula sheet)
  • dV/dx=−w(x)dV/dx = -w(x), dM/dx=V(x)dM/dx = V(x) and the positive shear / positive bending sign convention (on the formula sheet)
  • Equilibrium ∑Fx=0\sum F_x = 0, ∑Fy=0\sum F_y = 0, ∑M=0\sum M = 0; roller gives one reaction normal to its surface, pin gives two (learn this)
  • Boundary conditions for a simply supported beam: y=0y = 0 at each support (learn this)
  1. (a)
    Knowing that the bending moment M(x)M(x) is positive over the entire beam, and noting that the relationship between M(x)M(x) and the local deflection y(x)y(x) is: d2ydx2=MEI(1)\frac{d^2y}{dx^2} = \frac{M}{EI} \qquad (1) where the yy axis is depicted in Figure A2 and has origin at end A of the beam, sketch the deformed shape of the beam mean line. For your sketch, use the same Cartesian axes xx and yy defined in Figure A2.
    [5]2:2
  2. (b)
    Sketch the free body diagram of the loaded beam in Figure A2.
    [5]Third
  3. (c)
    Knowing that the distributed load w(x)w(x) is given by: w(x)=w0[1−x3L3](2)w(x) = w_0\left[1 - \frac{x^3}{L^3}\right] \qquad (2) where w0w_0 is a constant of dimension N/m, demonstrate that the vertical reactive forces RAR_A and RBR_B at the beam ends A and B are respectively: RA=920w0LandRB=310w0LR_A = \frac{9}{20} w_0 L \quad \text{and} \quad R_B = \frac{3}{10} w_0 L
    [10]2:2
  4. (d)
    Knowing that the equation of the deformed mean line of the beam is: y(x)=w0EI(x7840L3−x424+3Lx340)+C1x+C2(3)y(x) = \frac{w_0}{EI}\left(\frac{x^7}{840L^3} - \frac{x^4}{24} + \frac{3Lx^3}{40}\right) + C_1 x + C_2 \qquad (3) determine the constants C1C_1 and C2C_2 by imposing the compatibility condition of the beam deformation expressed by Equation (3) with the constraints acting on the beam depicted in Figure A2.
    [5]2:2