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A horizontal load \(F\) is applied at point R on a two-member truss, as shown in the figure. Both the members are prismatic with cross-sectional area, \(A_{0}\), and made of the same material with Young’s modulus \(E\).

The horizontal displacement of point R is:

Two members PR and QR hang from a ceiling at P and Q, each at 45 degrees to it, meeting at R a vertical distance l below; F acts horizontally at R towards the right

  • A.0
  • B.\(\frac{Fl}{EA_{0}}\)
  • C.\(\sqrt{2}\frac{Fl}{EA_{0}}\)
  • D.\(2\frac{Fl}{EA_{0}}\)

Answer: C

The horizontal displacement of R is \(\sqrt{2}\frac{Fl}{EA_{0}}\).

Each member runs at 45 degrees from the ceiling down to R, so its length is \(\sqrt{2}l\). At joint R, vertical balance makes the two member forces equal and opposite, and horizontal balance then gives each a magnitude \(F/\sqrt{2}\): one in tension, the other in compression.

By the unit-load method, with n the member forces for a unit horizontal load at R (\(n = \pm 1/\sqrt{2}\)):

\[ \begin{aligned} \delta &= \sum \frac{NnL}{EA_{0}} = 2 \times \frac{(F/\sqrt{2})(1/\sqrt{2})(\sqrt{2}l)}{EA_{0}} \\ &= \sqrt{2}\frac{Fl}{EA_{0}} \end{aligned} \]

Fl/(EA0) results from taking the member length as l instead of \(\sqrt{2}l\), and 2Fl/(EA0) from taking each member force as F. The displacement cannot be zero, since both members change length.

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