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Moment area: mid-span deflection under UDL

Short answer

Using symmetry, the tangent at mid-span is horizontal. The deviation of the support from this tangent equals the mid-span deflection, yielding 5wL⁴/(384EI) downward.

Determine the deflection at mid span of a simply supported beam subjected to uniformly distributed load w kN/m on the whole span by moment area. [Figure: simply supported beam of span L, flexural rigidity EI, UDL w kN/m over the whole span.]

Given data

Simply supported beam, span LL, rigidity EIEI, UDL ww over the whole span. The deflection at mid-span C is required.

  w kN/m
 A ===================== B
 ^          L            ^

Bending moment

RA=RB=wL2,M=wLx2−wx22R_A = R_B = \frac{wL}{2},\qquad M = \frac{wLx}{2} - \frac{wx^2}{2}

Maximum moment at mid-span: MC=wL28M_C = \dfrac{wL^2}{8}. The M/EIM/EI diagram is a parabola with peak wL28EI\dfrac{wL^2}{8EI}.

Using the symmetry

By symmetry the tangent at mid-span C is horizontal. The deflection at C below the support level is therefore equal to the deviation of A from the tangent at C (Theorem II).

Area and its moment about A (portion A to C)

Area=∫0L/2MEIdx=w2EI[Lx22−x33]0L/2=wL324EI\text{Area} = \int_0^{L/2}\frac{M}{EI}dx = \frac{w}{2EI}\left[\frac{Lx^2}{2} - \frac{x^3}{3}\right]_0^{L/2} = \frac{wL^3}{24EI}

Using the parabola property, the area under a parabola from its vertex over base L/2L/2 with height hh is 23⋅L2⋅h=23⋅L2⋅wL28EI=wL324EI\tfrac23 \cdot \tfrac{L}{2}\cdot h = \tfrac23\cdot\tfrac{L}{2}\cdot\dfrac{wL^2}{8EI} = \dfrac{wL^3}{24EI} (check). Its centroid is 5L16\dfrac{5L}{16} from A.

Deflection at mid-span

tA/C=Area×xˉA=wL324EI×5L16t_{A/C} = \text{Area}\times\bar{x}_A = \frac{wL^3}{24EI}\times\frac{5L}{16} yC=5wL4384 EI (downward)\boxed{y_C = \frac{5wL^4}{384\,EI}}\ \text{(downward)}

Check with the slope: θA=wL324EI\theta_A = \dfrac{wL^3}{24EI} (clockwise), the area between A and C.

✓ Answer checked by Claude Opus 5.5 (high effort)

All Theory of Structures I chapter 4 questions →