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ILD and BM at mid span for triangular load

Short answer

The ILD for M_C is a triangle with peak L/4 at C. Integrating the triangular load from C to B yields M_C = WL^2/48 (sagging).

Draw influence line diagram and calculate the bending moment at mid span C for the beam shown in fig-7. [Figure: simply supported beam AB of span L, C at mid span; a triangular load increasing from zero at C to W kN/m at B over the right half.]

Data: simply supported beam ABAB of span LL; CC at mid-span. A triangular load acts on the right half CBCB, zero at CC and rising to WW kN/m at BB.

ILD for bending moment at C

A triangle with peak abL=(L/2)(L/2)L=L4\dfrac{ab}{L} = \dfrac{(L/2)(L/2)}{L} = \dfrac{L}{4} at CC, 0 at AA and BB. At a distance uu from BB (in the right half) the ordinate is

y=L/4L/2 u=u2y = \frac{L/4}{L/2}\,u = \frac{u}{2}
   A o--------------C--------------o B
                    /\  L/4
   ILD M_C:      0 /    \ 0
   Load on CB:   0 at C ........ W at B

Load intensity

At distance uu from BB: w(u)=W(1−2uL)w(u) = W\left(1 - \dfrac{2u}{L}\right), so w=Ww = W at BB (u=0u=0) and 0 at CC (u=L/2u = L/2).

Bending moment

MC=∫w y duM_C = \int w\,y\,du over the loaded length:

MC=∫0L/2W(1−2uL)u2 du=W2[u22−2u33L]0L/2=W2[L28−L212]=W2×L224=WL248\begin{aligned} M_C &= \int_0^{L/2} W\left(1-\frac{2u}{L}\right)\frac{u}{2}\,du = \frac{W}{2}\left[\frac{u^2}{2} - \frac{2u^3}{3L}\right]_0^{L/2} \\ &= \frac{W}{2}\left[\frac{L^2}{8} - \frac{L^2}{12}\right] = \frac{W}{2}\times\frac{L^2}{24} = \frac{WL^2}{48} \end{aligned}

Check by statics

Total load =12⋅W⋅L2=WL4=\tfrac12\cdot W\cdot\dfrac{L}{2} = \dfrac{WL}{4}, acting at 23⋅L2=L3\dfrac{2}{3}\cdot\dfrac{L}{2} = \dfrac{L}{3} from CC, i.e. 5L6\dfrac{5L}{6} from AA. RA=WL4×L/6L=WL24R_A = \dfrac{WL}{4}\times\dfrac{L/6}{L} = \dfrac{WL}{24}.

MC=RA×L2=WL24×L2=WL248M_C = R_A\times\frac{L}{2} = \frac{WL}{24}\times\frac{L}{2} = \frac{WL^2}{48}

Answer: MC=WL248M_C = \dfrac{WL^2}{48} (sagging).

✓ Answer checked by Claude Opus 5.5 (high effort)

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