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Inclined load on a rectangular cantilever

Short answer

By resolving the inclined 2 kN load into principal axes and superposing bending, the maximum bending stress is 25.3 MPa at a corner. The neutral axis is at 52.4° to the horizontal axis. The resultant free-end deflection is 1.39 mm directed at 52.4° from the vertical.

A cantilever of length 1.5 m has a rectangular section 80 mm wide and 120 mm deep (depth vertical). A load of 2 kN acts at the free end in a plane inclined at 30∘30^\circ to the vertical axis of the section, passing through the centroid. Find (a) the maximum bending stress and its location, (b) the position of the neutral axis, (c) the resultant deflection of the free end. Take E=200E = 200 GPa.

Section properties (principal axes)

xx horizontal (width 80 mm), yy vertical (depth 120 mm):

Ix=80×120312=1.152×107 mm4,Iy=120×80312=5.12×106 mm4I_x = \frac{80\times120^3}{12} = 1.152\times10^{7}\ \text{mm}^4,\qquad I_y = \frac{120\times80^3}{12} = 5.12\times10^{6}\ \text{mm}^4

The section is symmetric, so x,yx, y are principal axes (Ixy=0I_{xy}=0).

Load components

Py=2000cos⁡30∘=1732.1 NPx=2000sin⁡30∘=1000.0 N\begin{aligned} P_y &= 2000\cos30^\circ = 1732.1\ \text{N} \\ P_x &= 2000\sin30^\circ = 1000.0\ \text{N} \end{aligned}

Moments at the fixed end (L=1500L = 1500 mm):

Mx=PyL=1732.05×1500=2.598×106 N mmMy=PxL=1000×1500=1.500×106 N mm\begin{aligned} M_x &= P_yL = 1732.05\times1500 = 2.598\times10^6\ \text{N mm} \\ M_y &= P_xL = 1000\times1500 = 1.500\times10^6\ \text{N mm} \end{aligned}

(a) Maximum stress

It occurs at a corner farthest from the neutral axis, at x=±40x = \pm40, y=±60y = \pm60 mm:

σmax=Mx yIx+My xIy=2.598×106×6011.52×106+1.5×106×405.12×106=13.53+11.72=25.25 MPa\begin{aligned} \sigma_{max} &= \frac{M_x\,y}{I_x} + \frac{M_y\,x}{I_y} = \frac{2.598\times10^6\times60}{11.52\times10^6} + \frac{1.5\times10^6\times40}{5.12\times10^6} \\ &= 13.53 + 11.72 = 25.25\ \text{MPa} \end{aligned}

The top fibre is in tension from PyP_y. The horizontal component bends the beam sideways, so the side away from it is in tension at the support. The corner where both tensions add carries +25.3+25.3 MPa and the diagonally opposite corner carries −25.3-25.3 MPa.

(b) Neutral axis

tan⁡α=MyIxMxIy=tan⁡ϕ IxIy=tan⁡30∘×11.525.12=0.5774×2.25=1.299\tan\alpha = \frac{M_yI_x}{M_xI_y} = \tan\phi\,\frac{I_x}{I_y} = \tan30^\circ\times\frac{11.52}{5.12} = 0.5774\times2.25 = 1.299 α=52.41∘\alpha = 52.41^\circ

The neutral axis passes through the centroid at 52.4∘52.4^\circ to the x-axis. It is turned towards the weaker axis (the y-axis, which has the smaller moment of inertia), compared with the position 30∘30^\circ that would be perpendicular to the load plane.

      y
      |  load plane (30 deg from y)
      | /     NA (52.4 deg from x)
      |/    /
  ----+----/----- x
     /|   /

(c) Deflection of the free end

δy=PyL33EIx=1732.05×150033×200×103×11.52×106=0.846 mmδx=PxL33EIy=1000×150033×200×103×5.12×106=1.099 mm\begin{aligned} \delta_y &= \frac{P_yL^3}{3EI_x} = \frac{1732.05\times1500^3}{3\times200\times10^3\times11.52\times10^6} = 0.846\ \text{mm} \\ \delta_x &= \frac{P_xL^3}{3EI_y} = \frac{1000\times1500^3}{3\times200\times10^3\times5.12\times10^6} = 1.099\ \text{mm} \end{aligned} δ=δx2+δy2=1.386 mm\delta = \sqrt{\delta_x^2 + \delta_y^2} = 1.386\ \text{mm}

The direction is at tan⁡−1(δx/δy)=52.4∘\tan^{-1}(\delta_x/\delta_y) = 52.4^\circ from the vertical: this is not the 30∘30^\circ of the load, and it is perpendicular to the neutral axis.

Answer: (a) σmax=25.3\sigma_{max} = 25.3 MPa at a corner; (b) neutral axis at 52.4∘52.4^\circ to the horizontal axis through the centroid; (c) resultant deflection 1.391.39 mm at 52.4∘52.4^\circ to the vertical.

✓ Answer checked by Claude Sonnet 5.5

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